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  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">ESurf</journal-id>
<journal-title-group>
<journal-title>Earth Surface Dynamics</journal-title>
<abbrev-journal-title abbrev-type="publisher">ESurf</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Earth Surf. Dynam.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">2196-632X</issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>

    <article-meta>
      <article-id pub-id-type="doi">10.5194/esurf-5-511-2017</article-id><title-group><article-title>Distinct phases of eustatic and tectonic forcing for late Quaternary
landscape evolution in southwest Crete, Greece</article-title>
      </title-group><?xmltex \runningtitle{Double alluvial fan records tectonic--eustatic interplay}?><?xmltex \runningauthor{V.~Mouslopoulou et~al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Mouslopoulou</surname><given-names>Vasiliki</given-names></name>
          <email>vasso@gfz-potsdam.de</email>
        <ext-link>https://orcid.org/0000-0002-5049-5027</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Begg</surname><given-names>John</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Fülling</surname><given-names>Alexander</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Moraetis</surname><given-names>Daniel</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2245-9256</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Partsinevelos</surname><given-names>Panagiotis</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Oncken</surname><given-names>Onno</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2894-480X</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>GeoForschungsZentrum, Telegrafenberg, 14473 Potsdam, Germany</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>GNS Science, P.O. Box 30368, Lower Hutt, New Zealand</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Humboldt University of Berlin, 12489 Berlin, Germany</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Sultan Qaboos University, P.O. Box 36, PC 123, Muscat, Oman</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Technical University of Crete, 73100 Chania, Greece</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Vasiliki Mouslopoulou (vasso@gfz-potsdam.de)</corresp></author-notes><pub-date><day>8</day><month>September</month><year>2017</year></pub-date>
      
      <volume>5</volume>
      <issue>3</issue>
      <fpage>511</fpage><lpage>527</lpage>
      <history>
        <date date-type="received"><day>5</day><month>December</month><year>2016</year></date>
           <date date-type="rev-request"><day>21</day><month>December</month><year>2016</year></date>
           <date date-type="rev-recd"><day>6</day><month>July</month><year>2017</year></date>
           <date date-type="accepted"><day>7</day><month>August</month><year>2017</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017.html">This article is available from https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017.html</self-uri>
<self-uri xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017.pdf">The full text article is available as a PDF file from https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017.pdf</self-uri>


      <abstract>
    <p>The extent to which climate, eustasy and tectonics interact to shape
the late Quaternary landscape is poorly known. Alluvial fans often
provide useful indexes that allow the decoding of information recorded
on complex coastal landscapes, such as those of the eastern
Mediterranean. In this paper we analyse and date (using infrared stimulated
luminescence
(IRSL) dating) a double alluvial fan system on southwest Crete, an
island straddling the forearc of the Hellenic subduction margin, in
order to constrain the timing and magnitude of its vertical
deformation and discuss the factors contributing to its landscape
evolution. The studied alluvial system is exceptional because each
of its two juxtaposed fans records individual phases of
alluvial and marine incision, thus providing unprecedented
resolution in the formation and evolution of its landscape.
Specifically, our analysis shows that the fan sequence at Domata
developed during Marine Isotope Stage (MIS) 3 due to five distinct
stages of marine transgressions and regressions and associated river
incision, in response to sea-level fluctuations and tectonic
uplift at averaged rates of <inline-formula><mml:math id="M1" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 2.2 mm yr<inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Interestingly, comparison of our results
with published tectonic uplift rates from western Crete shows that
uplift during 20–50 kyr BP was minimal (or even
negative). Thus, most of the uplift recorded at Domata must have
occurred in the last 20 kyr. This implies that eustasy
and tectonism impacted the landscape at Domata over mainly
distinct time intervals (e.g. sequentially and not synchronously),
with eustasy forming and tectonism preserving the coastal landforms.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Sea-level fluctuations relative to the modern sea level are well
constrained for the last 0.5 <inline-formula><mml:math id="M3" display="inline"><mml:mi mathvariant="normal">Myr</mml:mi></mml:math></inline-formula> (e.g. Imbrie et al.,
1984; Martinson et al., 1987; Bassinot et al., 1994; Chappell
et al., 1996; Dickinson, 2001; Siddall et al., 2003; Rabineau
et al., 2005; Lambeck and Purcell, 2005; Lisiecki and Raymo,
2005; Antonioli et al., 2007). When these fluctuations are used
in conjunction with dating techniques, they provide a powerful
tool for interpreting coastal geomorphology and assessing
vertical deformation from marine and marginal marine deposits
through the middle and late Quaternary (e.g. Pirazzoli et al.,
1996; Rabineau et al., 2005; Antonioli et al., 2007;
Mouslopoulou et al., 2015a). While there is little debate about
the role of tectonic uplift in generating the topographic relief
required for the processes of erosion and deposition,
uncertainty still exists as to the relative significance of
tectonic, eustatic and climatic contributions to deposition and
incision of fans of the Quaternary age and their variation through
time (e.g. Waters et al., 2010).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p>Map illustrating the location of Crete within the forearc
of the Hellenic subduction margin. The locations of the Hellenic Trough and
its splays (the Ptolemy, Pliny and Strabo troughs) are indicated. Labelled
arrows show geodetically derived site velocities (mm a<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) relative to a fixed
Nubia plate (Reilinger et al., 2010). The study area at Domata (D) is indicated
by a filled white circle while the regions of Sfakia (S), Elafonisi (E),
Palaiochora (P) and Agios Georgios (AG) are marked with blue circles.
WM <inline-formula><mml:math id="M5" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> White Mountains. Hillshade is derived from GeoMapApp.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f01.pdf"/>

      </fig>

      <p>Alluvial fans are excellent proxies for Quaternary landscape
evolution in a climate such as the Mediterranean and their study
could potentially place some constraints on the factors that
impacted the landscape during its formation and evolution (e.g.
Pope et al., 2008, 2016; Zacharias et al., 2009). Overall,
alluvial fan deposition is influenced by a rising or relatively
high sea level, by catchment size and sediment supply, by major
changes in climatic conditions (such as high rainfall and/or
short, intense storms), and by vegetation coverage in the
catchment area. These factors regulate stream carrying capacity
and sediment supply (e.g. Bull, 1990; Pope et al., 2016) and are
responsible for whether deposition or river entrenchment
processes predominate at any one time. Alluvial fan surface
abandonment and river entrenchment is favoured by eustatic
sea-level fall or tectonic uplift (or a combination of both),
reduction in sediment supply due to climatic amelioration,
densification of catchment vegetation, or reduced rainfall (e.g.
Pope et al., 2008, 2016; Waters et al., 2010). Fan aggradation
is encouraged by factors such as rising base level (sea level
for Domata), sediment supply, increased stream carrying capacity
(rainfall and/or temporal rainfall distribution) and reduction in
catchment vegetation cover.</p>
      <p>For example, in southwest Crete (eastern Mediterranean), Nemec
and Postma (1993) and Pope et al. (2008, 2016) studied a fan
system and showed that fan deposition was associated with all
last glacial stadial and interstadial conditions and that fan
entrenchment was governed by the major climatic transitions
between MIS5/4 and MIS2/1. Conversely, Tiberti
et al. (2014) and Mouslopoulou et al. (2015b) have shown that
tectonic uplift on western Crete is significant, reaching rates of
7–8 <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> during the late Quaternary. Despite this progress in
understanding, we are, however, still unable to precisely
appreciate the interplay between, and the relative importance
of, climate and tectonics during the late Quaternary in the
Mediterranean. How do severe uplift rates recorded along the
forearc of the Hellenic margin (where Crete lies) reconcile with
periods of prevalence of eustatic processes? Here we capitalise
on a well-preserved alluvial fan system at Domata in southern
Crete (Fig. 1) to study the late Quaternary (<inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M8" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP) interplay between sea-level fluctuations
and tectonics. To our knowledge, the site at Domata is unique on
the island of Crete as each alluvial fan-building episode has
been followed by distinct episodes of alluvial incision and
subsequent marine trimming (Figs. 2 and 3). Thus, at this site,
we have the opportunity to test the idea proposed by Pope
et al. (2016) that eustasy largely controls the landscape
evolution in southwest Crete.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p>Northward view of the beach at Domata illustrating the
two generations of fan surfaces and their separate episodes of marine
trimming. The location of the Klados Gorge, the two elevated marine benches
cut on bedrock and the AD 365 uplifted shoreline are indicated (for
a close-up view of the bioerosional AD 365 notch see Fig. 6c).</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f02.pdf"/>

      </fig>

      <p>Using luminescence dating together with the Siddall
et al. (2003) sea-level curve, we find that the alluvial fan
system at Domata was consecutively affected by (1) sea-level
fluctuations, triggering building of the fans and subsequent
river and marine incision between <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">45</mml:mn></mml:mrow></mml:math></inline-formula> and 20 <inline-formula><mml:math id="M10" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>
BP, during a period of minimal tectonic activity, and (2) intense
tectonic uplift between <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M12" display="inline"><mml:mi mathvariant="normal">ka</mml:mi></mml:math></inline-formula> and present, at
rates that exceeded those of the rising sea level, resulting in
the preservation of the entire fan sequence. These findings are
in accord with Pope et al. (2016) in showing that regional
tectonics did not necessarily play a key role in fan incision in
southern Crete.</p>
</sec>
<sec id="Ch1.S2">
  <title>Geological setting of Crete and vertical tectonics</title>
      <p>The Mediterranean island of Crete is a mountainous and elongate
landmass (<inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">260</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M14" display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> long from west to east,
60 <inline-formula><mml:math id="M15" display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> wide from north to south) that lies within the
uplifted forearc section of the Hellenic subduction margin, the
most seismically active region in Europe (Fig. 1).  The total
relative convergence rate between the subducting African plate
and the overriding Eurasian plate is <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">35</mml:mn></mml:mrow></mml:math></inline-formula>–40 <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (Reilinger et al., 2010; Fig. 1). The
subduction trench lies <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">225</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M19" display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> to the south of
Crete (e.g. Ryan et al., 1970; Le Pichon and Angelier, 1979)
while the north-dipping subduction interface lies at a depth of
<inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> to 65 <inline-formula><mml:math id="M21" display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> beneath Crete (Papazachos et al.,
2006; Vernant et al., 2014), with the projection of the down-dip
end of the locked zone aligning with the southern coastline of
Crete, where the study area is located (Fig. 1) (Meier et al.,
2007). The Hellenic Trough, a major bathymetric and tectonic
feature within the forearc, lies south of Crete and includes
three secondary features, which, from west to east, are named as
the Ptolemy, Pliny and Strabo troughs (Fig. 1).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p>The fan sequence at Domata looking obliquely towards
the southeast. The two fan surfaces and their respective stream-incised cliffs
are illustrated. The yellow dashed line in the present stream cliff
indicates the benched upper-fan erosional surface, which is overlain by the
deposits of the lower fan. This important marker was used to calculate
a long-term (39 <inline-formula><mml:math id="M22" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>) uplift rate at Domata (see text for details). White spots
mark the location of IRSL samples.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f03.pdf"/>

      </fig>

      <p>Crete has been characterised by a complex history of vertical
movements during the Cenozoic (e.g. Peters et al., 1985). Onshore
sediments record a period of subsidence and basin development
through the middle and late Miocene (Serravallian to Messinian)
with a change to rapid uplift in the early Pliocene (Zanclean),
followed by slower long-term uplift that continues to the present
day (e.g. Le Pichon and Angelier, 1981; Angelier et al., 1982;
Meulenkamp et al., 1994; Zachariasse et al., 2008; Roberts
et al., 2013; Gallen et al., 2014).</p>
      <p>Late Quaternary tectonic uplift on Crete is uniform but transient
(Tiberti et al., 2014; Mouslopoulou et al., 2015b). Using dated
palaeo-shorelines and numerical models, Tiberti et al. (2014) and
Mouslopoulou et al. (2015b) show that the island of Crete has
experienced, during the last 20 thousand years, periods of severe
fluctuation in its vertical deformation (at rates of up to
8 <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), while in the preceding <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> thousand
years, vertical movement on Crete was either minimal or reversed
(subsidence of 0–3 <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>; Tiberti et al., 2014). High uplift rates
(<inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:math></inline-formula>–8 <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) have also been documented on western
Crete since 2 <inline-formula><mml:math id="M28" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP, in response to co-seismic uplift
(that locally reached up to 10 <inline-formula><mml:math id="M29" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>) (Pirazzoli et al.,
1996; Shaw et al., 2008; Mouslopoulou et al., 2015a). Uplift rate
transients on Crete are thought to result from non-uniform stress
accumulation and release on upper-plate reverse faults in the
overriding plate (Shaw et al., 2008; Stiros, 2010; Tiberti
et al., 2014; Mouslopoulou et al., 2015b).</p>
      <p>Historical and archaeological records have also been used to link
uplift in western Crete to earthquakes (Pirazzoli et al., 1982,
1996; Stiros, 2001; Papazachos and Papazachou, 2003;
Papadimitriou and Karakostas, 2008; Shaw et al., 2008;
Stefanakis, 2010; Strasser et al., 2011). In particular, historic
accounts of a major earthquake in Crete in <inline-formula><mml:math id="M30" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> AD 365 are
approximately coincident with historic documents recording
tsunami inundation of parts of the Libyan and Egyptian
coastlines, particularly Alexandria (Ammianus Marcellinus,
translated by C. D. Yonge, 1862; Polonia et al., 2013). A gently
tilted palaeo-shoreline (tidal notch) can be followed along the
western shoreline of Crete for <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">150</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M32" display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> from the
area of maximum uplift near the southwest tip (Elafonisi) to as
far east as Agios Georgios (Fig. 1). At Domata, our study site,
this notch is at 6 <inline-formula><mml:math id="M33" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> a.s.l. A number of studies
attribute the timing of this prominent palaeo-shoreline to the historic AD 365
earthquake (e.g. Pirazzoli et al., 1982, 1996;
Stiros, 2001; Shaw et al., 2008).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p><bold>(a)</bold> Digital elevation model of the study area at Domata as
viewed obliquely from the southwest. The model is derived by using the
nearest-neighbour algorithm along with the GPS measurements marked and
colour coded by 10 <inline-formula><mml:math id="M34" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> elevation bands. Note the upper- and lower-fan surfaces,
each incised following surface abandonment and each trimmed by marginal
marine processes. <bold>(b)</bold> Digital elevation model with National Greek Cadastre
Agency orthophoto draped onto it, along with the GPS measurements. The yellow polygon
depicts the area illustrated in the DEM of panel <bold>(a)</bold>. Red polygons indicate
the localities of the profiles presented in Fig. 5a.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f04.jpg"/>

      </fig>

</sec>
<sec id="Ch1.S3">
  <title>Data – methods – chronology</title>
      <p>At Domata a unique sequence of two juxtaposed generations of
alluvial fans is documented, each truncated by different episodes
of river and marine incision (see Figs. 2, 3 and 4). The discussion that follows gives a detailed
account of the materials and the geometry of the alluvial fan
system at Domata, establishes the stratigraphic relationships of
its key geomorphic features and provides the chronological
framework (sequence of events) within which the established
stratigraphic relationships developed.</p>
<sec id="Ch1.S3.SS1">
  <title>Coastal geomorphic features at Domata</title>
      <p>The landmass of the White Mountains (Lefka Ori) dominates the
landscape of western Crete (Figs. 1 and 2). At the southern
coastline of Crete, and proximal to our study area, the White
Mountains drop abruptly by <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1800</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M36" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> to sea level over
a distance of <inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M38" display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula>, forming a steep and rugged
landscape, often incised by narrow south-draining gorges
(Fig. 2). One such gorge is Klados, which reaches the sea at the
beach of Domata (Figs. 2 and 3). This steep subaerial landscape
extends offshore along most of the southwest coast of Crete, as
evidenced by the regional bathymetric slopes, which are steeper
offshore than onshore (Le Pichon and Angelier, 1979; Mascle
et al., 1986). As bedrock crops out along much of the southwestern
coastline of Crete, it is clear that bathymetric slopes are also
cut in bedrock, implying that the Quaternary sediment sequence
recorded at Domata has no significant thickness offshore.</p>
      <p>The rivers within the gorges of western Crete are usually
ephemeral and scour to bedrock, depositing gravels only locally,
commonly where valleys widen at junctions with side valleys,
across faults (e.g. Sfakia fans; Pope et al., 2008) or close to
the coast. As the rivers approach the sea, gradients shallow and
stream carrying capacity decreases, resulting in deposition from
bedload of fans grading to the shoreline. The headwaters of the
Klados River, only 7 <inline-formula><mml:math id="M39" display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> from the coast, reach an elevation
of <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1800</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M41" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> in the White Mountains, and no
significant areas of sediment accumulation exist between its upper
reaches and the fans near the coast that are the subject of this
paper. In the Klados Gorge area, bedrock comprises mainly
crystalline platy limestones with some chert and platy marbles
(Creutzburg and Siedel, 1975; Manutsoglu et al., 2003; Fassoulas
et al., 2004). The erosion of these units supplied the Domata area
mainly with carbonate clasts and limited chert clasts, which
explains the abundance of carbonates in the alluvial fans and
fluvial terraces.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p><bold>(a)</bold> Profiles of fan surfaces projected onto
common planes parallel with the modern Klados River channel (above) and
parallel with the modern coastline (below). The extent of the volumes of
upper-fan materials (pink) and lower-fan materials (light green) are
schematically illustrated beneath each measured profile. The locations of
each of the luminescence sample points are annotated by yellow dots. The
locations of the stratigraphic columns presented in Fig. 5b are also
indicated. Horizontal and vertical scales for each profile are similar, with
a vertical exaggeration (VE) of ca. 1.25. Note that the downstream slope of the upper- and lower-fan
surfaces are about the same, both a little steeper than the slope of the
modern stream channel. <bold>(b)</bold> Schematic stratigraphic columns for the upper (left) and lower
(right) alluvial fan deposits. Note that vertical scale bars indicate
elevation in metres above mean sea level for each column. The lower-fan
column reflects a stratigraphic section close to the junction between the
lower-fan coastal cliff and the river entrenchment. The upper-fan section is
located close to the western end of the marine cliff. Their stratigraphic
location is indicated in Fig. 5a. Note that the right-hand edge of the
lower-fan section represents relative competence of materials.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f05.pdf"/>

        </fig>

      <p>In order to better interpret the geomorphology at Domata, we
topographically surveyed and modelled the entire study region
(Figs. 3 and 4). The data acquisition was performed with a double-precision Real Time Kinematic (RTK) GPS receiver and was corrected
to provide coordinates under the Greek Geodetic Reference System
(GGRS 87). The topographic dataset includes a total of 4156 survey
points, measured under an excellent geometric dilution of
precision (GDOP) and an accuracy of <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M43" display="inline"><mml:mi mathvariant="normal">cm</mml:mi></mml:math></inline-formula>. Some areas
were not surveyed due to dense vegetation; however, values for
these regions were interpolated using the nearest-neighbour
method. A series of breaklines and sparse elevation models from
the National Cadastre and Mapping Agency of Greece were
incorporated in the model (Fig. 4a) to optimise representation.</p>
      <p>Older geomorphic features are present at Domata in the form of two
marine benches cut in bedrock at elevations of about 100 and
360 <inline-formula><mml:math id="M44" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> on the western slopes above the Klados River
(Fig. 2). While we cannot assign ages to these benches, their
altitude and geomorphic similarity with known and dated (MIS5 and/or MIS7)
late Pleistocene marine benches elsewhere in Crete (e.g. Strasser
et al., 2011; Gallen et al., 2014; Strobl et al., 2014) provide
some stratigraphic and chronological context for the age of the
alluvial fans at Domata (i.e. because of their lower elevation,
the alluvial fan surfaces that are the subject of this paper are
expected to be younger than 125 <inline-formula><mml:math id="M45" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>).</p>
      <p>At Domata, two triangular, elevated fan surfaces (a lower and an
upper surface), covering a combined surface area of <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> near the mouth of Klados River, rise to an
inland elevation of <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M49" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> (Figs. 2–4). The
fan surfaces are derived from a single feeder channel, the Klados
River, which drains a relatively small catchment (immediately west
of the larger and better-known Samaria Gorge) and they lie at the
seaward end of a narrow entrenched gorge. They are unique in south
Crete as they are protected from alluvial erosion by a low bedrock
ridge (see Fig. 2), which channels the river flow to the western
side of its narrow valley. Where the Klados River leaves its
bedrock gorge, <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M51" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> from the coast, its channel is
incised into gravels <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M53" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> below an abandoned fan
surface, the lower of the two surfaces (Figs. 2 and 3). Gravel
deposits beneath the surface on lap bedrock on both sides of the
valley without structural deformation (e.g. faulting).
Downstream, <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M55" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> from the river mouth, the seaward
extent of the lower-fan surface is at ca. 35 <inline-formula><mml:math id="M56" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> a.s.l. (Fig. 5a). Here, both the fan surface and its alluvial
entrenchment cliff are trimmed parallel with, and close to, the
present shoreline (Figs. 2 and 3). The linearity and parallelism
of this cliff to the modern coastline clearly imply that this
cliff has been trimmed by the sea. The elevation of the lower-fan
surface decreases eastwards along the sea-trimmed cliff to <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M58" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> a.s.l. near the east end of Domata beach
(Figs. 2 and 5a). Along this coastal cliff, the highest elevation
of the lower-fan surface occurs <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">190</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M60" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> east of the
Klados River (Figs. 2 and 5a).</p>
      <p>The upper-fan surface lies at <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M62" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> elevation at
its upstream extent, <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">60</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M64" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> above the active river
bed and <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M66" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> above the lower-fan surface (Figs. 4
and 5a). The upper-fan deposits are truncated by an old river
incision (trending <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">200</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M68" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) that is older than the
lower-fan surface, as the deposits of the lower fan lap against
the buried upper-fan deposits (Fig. 3). Downstream, the seaward
extent of the upper-fan surface and its entrenchment cliff is
truncated by another marine cliff (trending <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">130</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>)
that predates deposition of the lower fan, as the lower-fan
surface also laps against this (Figs. 2 and 3).  Where the marine
trimming truncates the upper-fan surface and its river
entrenchment cliff, the upper-fan surface has an elevation of
ca. 60 <inline-formula><mml:math id="M71" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>, and this decreases eastwards to <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M73" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> at the east end of the beach (Figs. 2, 4 and 5a). In
the east, the upper-fan surface is overlain by silty sand near the
eastern end of Domata beach (Fig. 5a). This deposit is preserved
seaward of the only stream gully that crosses the upper-fan
surface, draining the bedrock area behind that fan; this ephemeral
stream is undoubtedly the source of this younger silty sand (UF-2
sample in Table 1).</p>
      <p>Lower-fan materials exposed in the sea cliff are dominantly poorly
sorted, matrix-supported gravels, moderately stratified, with
coarser beds commonly <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M75" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> thick and sometimes
clast-supported, and finer beds <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M77" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> thick that
display lateral lensing and channelling (see stratigraphic log in
Fig. 5b). Along the coastal cliff, bedding is convex up,
sub-parallel with the lower-fan surface (Fig. 6a). Some individual
beds can be traced laterally up to 200–300 <inline-formula><mml:math id="M78" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> (see thin
dashed lines in Fig. 6a). In the coastal cliff, lower-fan
materials lap onto a gently undulating, sub-horizontal
discontinuity on an underlying older alluvial gravel
(e.g. remnants of the upper fan) that is coarser and more commonly
clast-supported (Fig. 5b), and has a higher fine-grained content
(Figs. 2, 3, 5b and 6a). The contact surface between the two fan
units is very clear and extends along the length of the beach
(Figs. 5 and 6a) and also up the Klados River for <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M80" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> (Fig. 3). In places, the contact is locally
obscured by fallen debris, but it is clearly sub-horizontal, with
low relief, and it undoubtedly separates the two fan units
(Fig. 6a). At each end of the beach, the older gravel materials
lap onto older sedimentary rocks (gravel and sand) (Fig. 6c).</p>

<?xmltex \floatpos{p}?><table-wrap id="Ch1.T1" orientation="landscape"><caption><p>Luminescence dosimetry measurements and potassium feldspar IRSL ages (indicated
in bold).</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.63}[.63]?><oasis:tgroup cols="16">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="center"/>
     <oasis:colspec colnum="8" colname="col8" align="center"/>
     <oasis:colspec colnum="9" colname="col9" align="center"/>
     <oasis:colspec colnum="10" colname="col10" align="center"/>
     <oasis:colspec colnum="11" colname="col11" align="center"/>
     <oasis:colspec colnum="12" colname="col12" align="center"/>
     <oasis:colspec colnum="13" colname="col13" align="center"/>
     <oasis:colspec colnum="14" colname="col14" align="left"/>
     <oasis:colspec colnum="15" colname="col15" align="left"/>
     <oasis:colspec colnum="16" colname="col16" align="center"/>
     <oasis:thead>
       <oasis:row>  
         <oasis:entry colname="col1">Sample (depth)</oasis:entry>  
         <oasis:entry colname="col2">Lab. no. <?xmltex \hack{\hfill\break}?>(aliquot no.)</oasis:entry>  
         <oasis:entry colname="col3">U</oasis:entry>  
         <oasis:entry colname="col4">Th</oasis:entry>  
         <oasis:entry colname="col5">K</oasis:entry>  
         <oasis:entry colname="col6">Cosmic dose rate</oasis:entry>  
         <oasis:entry colname="col7">Water cont. measured</oasis:entry>  
         <oasis:entry colname="col8">Water cont. estimated</oasis:entry>  
         <oasis:entry colname="col9">Dose rate (<inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>  
         <?xmltex \mcwidth{244pt}?><oasis:entry namest="col10" nameend="col13" align="left">Equivalent dose (<inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) (Gy)<?xmltex \hack{\hfill\break}?> <bold>IRSL age (ka)</bold></oasis:entry>  
         <oasis:entry colname="col14">SD</oasis:entry>  
         <oasis:entry colname="col15">SE<inline-formula><mml:math id="M111" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">h</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col16">Overdispersion<inline-formula><mml:math id="M112" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">i</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">(ppm)<inline-formula><mml:math id="M113" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4">(ppm)<inline-formula><mml:math id="M114" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">(%)<inline-formula><mml:math id="M115" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6">(mGy ka<inline-formula><mml:math id="M116" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)<inline-formula><mml:math id="M117" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">(%)<inline-formula><mml:math id="M118" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">c</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col8">(%)<inline-formula><mml:math id="M119" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">d</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col9">(Gy ka<inline-formula><mml:math id="M120" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)<inline-formula><mml:math id="M121" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">e</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col10">Mean</oasis:entry>  
         <oasis:entry colname="col11">Median</oasis:entry>  
         <oasis:entry colname="col12">CAM<inline-formula><mml:math id="M122" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">f</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col13">MAM<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">g</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col14">(%)</oasis:entry>  
         <oasis:entry colname="col15">(%)</oasis:entry>  
         <oasis:entry colname="col16">(%)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"/>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7"/>  
         <oasis:entry colname="col8"/>  
         <oasis:entry colname="col9"/>  
         <oasis:entry colname="col10"/>  
         <oasis:entry colname="col11"/>  
         <oasis:entry colname="col12"/>  
         <oasis:entry colname="col13"/>  
         <oasis:entry colname="col14"><bold>(ka)</bold></oasis:entry>  
         <oasis:entry colname="col15"><bold>(ka)</bold></oasis:entry>  
         <oasis:entry colname="col16"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">UF-1 (0.3 <inline-formula><mml:math id="M124" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col2">HUB-0423 (12)</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.46</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.63</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.06</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.11</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:mn mathvariant="normal">195</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">1.1</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.99</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col10">41.7 Gy</oasis:entry>  
         <oasis:entry colname="col11">36.0 Gy</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:mn mathvariant="normal">38.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">4.4</mml:mn></mml:mrow></mml:math></inline-formula> Gy</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:mn mathvariant="normal">27.7</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">5.0</mml:mn></mml:mrow></mml:math></inline-formula> Gy</oasis:entry>  
         <oasis:entry colname="col14">42.7 %</oasis:entry>  
         <oasis:entry colname="col15">12.3 %</oasis:entry>  
         <oasis:entry colname="col16">39.8 %</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"/>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7"/>  
         <oasis:entry colname="col8"/>  
         <oasis:entry colname="col9"/>  
         <oasis:entry colname="col10"><bold>42.1 ka</bold></oasis:entry>  
         <oasis:entry colname="col11"><bold>36.4 ka</bold></oasis:entry>  
         <oasis:entry colname="col12"><bold>38.8</bold> <inline-formula><mml:math id="M133" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> <bold>5.2 ka</bold></oasis:entry>  
         <oasis:entry colname="col13"><bold>27.9</bold> <inline-formula><mml:math id="M134" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> <bold>5.4 ka</bold></oasis:entry>  
         <oasis:entry colname="col14"><bold>18.0 ka</bold></oasis:entry>  
         <oasis:entry colname="col15"><bold>5.2 ka</bold></oasis:entry>  
         <oasis:entry colname="col16"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">UF-2 (1.1 <inline-formula><mml:math id="M135" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col2">HUB-0424 (7)</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.06</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.36</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.13</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.53</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mn mathvariant="normal">173</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">17</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">5.1</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mn mathvariant="normal">5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.67</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.11</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col10">41.7 Gy</oasis:entry>  
         <oasis:entry colname="col11">38.6 Gy</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mn mathvariant="normal">41.2</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.4</mml:mn></mml:mrow></mml:math></inline-formula> Gy</oasis:entry>  
         <oasis:entry colname="col13">–</oasis:entry>  
         <oasis:entry colname="col14">17.5 %</oasis:entry>  
         <oasis:entry colname="col15">6.6 %</oasis:entry>  
         <oasis:entry colname="col16">15.0 %</oasis:entry>
       <?xmltex \interline{[5.690551pt]}?></oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"/>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7"/>  
         <oasis:entry colname="col8"/>  
         <oasis:entry colname="col9"/>  
         <oasis:entry colname="col10"><bold>25.0 ka</bold></oasis:entry>  
         <oasis:entry colname="col11"><bold>23.1 ka</bold></oasis:entry>  
         <oasis:entry colname="col12"><bold>24.7</bold> <inline-formula><mml:math id="M143" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> <bold>2.1 ka</bold></oasis:entry>  
         <oasis:entry colname="col13"><bold>–</bold></oasis:entry>  
         <oasis:entry colname="col14"><bold>4.4 ka</bold></oasis:entry>  
         <oasis:entry colname="col15"><bold>1.7 ka</bold></oasis:entry>  
         <oasis:entry colname="col16"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">RB-1 (28.0 <inline-formula><mml:math id="M144" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col2">HUB-0425 (11)</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.84</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.62</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.15</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:mn mathvariant="normal">17</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">1.6</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.96</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.06</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col10">51.3 Gy</oasis:entry>  
         <oasis:entry colname="col11">43.4 Gy</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:mn mathvariant="normal">46.3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">6.2</mml:mn></mml:mrow></mml:math></inline-formula> Gy</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:mn mathvariant="normal">34.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">6.2</mml:mn></mml:mrow></mml:math></inline-formula> Gy</oasis:entry>  
         <oasis:entry colname="col14">49.4 %</oasis:entry>  
         <oasis:entry colname="col15">14.9 %</oasis:entry>  
         <oasis:entry colname="col16">44.1 %</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"/>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7"/>  
         <oasis:entry colname="col8"/>  
         <oasis:entry colname="col9"/>  
         <oasis:entry colname="col10"><bold>53.4 ka</bold></oasis:entry>  
         <oasis:entry colname="col11"><bold>45.2 ka</bold></oasis:entry>  
         <oasis:entry colname="col12"><bold>48.0</bold> <inline-formula><mml:math id="M153" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> <bold>7.1 ka</bold></oasis:entry>  
         <oasis:entry colname="col13"><bold>35.8</bold> <inline-formula><mml:math id="M154" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> <bold>6.8 ka</bold></oasis:entry>  
         <oasis:entry colname="col14"><bold>26.4 ka</bold></oasis:entry>  
         <oasis:entry colname="col15"><bold>8.0 ka</bold></oasis:entry>  
         <oasis:entry colname="col16"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">LF-1a/b (0.28 <inline-formula><mml:math id="M155" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col2">HUB-0426 (10)</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.67</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.09</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:mn mathvariant="normal">194</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">19</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">0.3</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.01</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col10">39.9 Gy</oasis:entry>  
         <oasis:entry colname="col11">29.1 Gy</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:mn mathvariant="normal">34.7</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">5.8</mml:mn></mml:mrow></mml:math></inline-formula> Gy</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:mn mathvariant="normal">29.0</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">5.2</mml:mn></mml:mrow></mml:math></inline-formula> Gy</oasis:entry>  
         <oasis:entry colname="col14">58.2 %</oasis:entry>  
         <oasis:entry colname="col15">18.4 %</oasis:entry>  
         <oasis:entry colname="col16">52.8 %</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"/>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7"/>  
         <oasis:entry colname="col8"/>  
         <oasis:entry colname="col9"/>  
         <oasis:entry colname="col10"><bold>39.5 ka</bold></oasis:entry>  
         <oasis:entry colname="col11"><bold>28.8 ka</bold></oasis:entry>  
         <oasis:entry colname="col12"><bold>34.3</bold> <inline-formula><mml:math id="M164" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> <bold>6.2 ka</bold></oasis:entry>  
         <oasis:entry colname="col13"><bold>28.6</bold> <inline-formula><mml:math id="M165" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> <bold>5.5 ka</bold></oasis:entry>  
         <oasis:entry colname="col14"><bold>23.0 ka</bold></oasis:entry>  
         <oasis:entry colname="col15"><bold>7.3 ka</bold></oasis:entry>  
         <oasis:entry colname="col16"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">LF-2a/b (0.24 <inline-formula><mml:math id="M166" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col2">HUB-0427 (13)</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.73</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.67</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.1</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:mn mathvariant="normal">195</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">1.3</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.07</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col10">44.0 Gy</oasis:entry>  
         <oasis:entry colname="col11">42.8 Gy</oasis:entry>  
         <oasis:entry colname="col12"><inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mn mathvariant="normal">42.6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">3.2</mml:mn></mml:mrow></mml:math></inline-formula> Gy</oasis:entry>  
         <oasis:entry colname="col13"><inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:mn mathvariant="normal">39.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">5.4</mml:mn></mml:mrow></mml:math></inline-formula> Gy</oasis:entry>  
         <oasis:entry colname="col14">26.2 %</oasis:entry>  
         <oasis:entry colname="col15">7.3 %</oasis:entry>  
         <oasis:entry colname="col16">26.6 %</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"/>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7"/>  
         <oasis:entry colname="col8"/>  
         <oasis:entry colname="col9"/>  
         <oasis:entry colname="col10"><bold>41.2 ka</bold></oasis:entry>  
         <oasis:entry colname="col11"><bold>40.0 ka</bold></oasis:entry>  
         <oasis:entry colname="col12"><bold>39.9</bold> <inline-formula><mml:math id="M175" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> <bold>4.0 ka</bold></oasis:entry>  
         <oasis:entry colname="col13"><bold>36.9</bold> <inline-formula><mml:math id="M176" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> <bold>5.6 ka</bold></oasis:entry>  
         <oasis:entry colname="col14"><bold>10.8 ka</bold></oasis:entry>  
         <oasis:entry colname="col15"><bold>3.0 ka</bold></oasis:entry>  
         <oasis:entry colname="col16"/>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table><?xmltex \hack{
\setlength\tabularwidth{0.9\tabularwidth}
}?><?xmltex \begin{scaleboxenv}{.63}[.63]?><table-wrap-foot><p><?xmltex \hack{\vspace*{2mm}}?>
<inline-formula><mml:math id="M81" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula> Uranium, thorium and potassium contents were determined via high-resolution gamma ray spectrometry (HPGe detector). <?xmltex \hack{\\}?>U-238: U-234 (53.2 <inline-formula><mml:math id="M82" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>), Th-234 (63.3 <inline-formula><mml:math id="M83" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>), Ra-226 (186.1 <inline-formula><mml:math id="M84" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>), Pb-214 (295.2, 351.9 <inline-formula><mml:math id="M85" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>), Bi-214 (609.3, 1120.3, 1764.5 <inline-formula><mml:math id="M86" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>), Pb-210 (46.5 <inline-formula><mml:math id="M87" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>).  <?xmltex \hack{\\}?>Th-232: Ac-228 (338.3, 911.2, 969.0 <inline-formula><mml:math id="M88" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>), Pb-212 (238.6 <inline-formula><mml:math id="M89" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>), Bi-212 (727.3 <inline-formula><mml:math id="M90" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>), Tl-208 (583.2 <inline-formula><mml:math id="M91" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>). <?xmltex \hack{\\}?>K-40: 1461.0 <inline-formula><mml:math id="M92" display="inline"><mml:mi mathvariant="normal">keV</mml:mi></mml:math></inline-formula>.<?xmltex \hack{\\}?>U-238 and Th-232: the arithmetic means of the activities of the above-mentioned natural daughter products were used (<inline-formula><mml:math id="M93" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> standard error).<?xmltex \hack{\\}?>The internal K content of the potassium feldspar was set to <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:mn mathvariant="normal">12.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> % (Huntley and Baril, 1997).<?xmltex \hack{\\}?><inline-formula><mml:math id="M95" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula> Cosmic dose rates were estimated regarding geographic position (35<inline-formula><mml:math id="M96" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 24<inline-formula><mml:math id="M97" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E), altitude and sampling depth.<?xmltex \hack{\\}?><inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">c</mml:mi></mml:msup></mml:math></inline-formula> Water content of sediment samples as a percentage of dry mass (oven-dried for 24 <inline-formula><mml:math id="M99" display="inline"><mml:mi mathvariant="normal">h</mml:mi></mml:math></inline-formula> at 105 <inline-formula><mml:math id="M100" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C).<?xmltex \hack{\\}?><inline-formula><mml:math id="M101" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">d</mml:mi></mml:msup></mml:math></inline-formula> Water content used for dose rate calculation.<?xmltex \hack{\\}?><inline-formula><mml:math id="M102" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">e</mml:mi></mml:msup></mml:math></inline-formula> For coarse-grain potassium feldspar an <inline-formula><mml:math id="M103" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> value of <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.15</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>  was assumed (Balescu and Lamothe, 1994).<?xmltex \hack{\\}?><inline-formula><mml:math id="M105" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">f</mml:mi></mml:msup></mml:math></inline-formula> Central Age Model (CAM) according Galbraith et al. (1999)<?xmltex \hack{\\}?><inline-formula><mml:math id="M106" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">g</mml:mi></mml:msup></mml:math></inline-formula> Minimum Age Model (MAM) according Galbraith et al. (1999). Sigma b was set to 0.25.<?xmltex \hack{\\}?><inline-formula><mml:math id="M107" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">h</mml:mi></mml:msup></mml:math></inline-formula> SE of the mean: SD divided by the square root of the number of measured aliquots.<?xmltex \hack{\\}?><inline-formula><mml:math id="M108" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">i</mml:mi></mml:msup></mml:math></inline-formula> The overdispersion describes the variation in the equivalent dose in addition to the expected error. It is given by the CAM.
</p></table-wrap-foot><?xmltex \end{scaleboxenv}?></table-wrap>

      <?xmltex \floatpos{p}?><fig id="Ch1.F6" specific-use="star"><caption><p><bold>(a)</bold> The present marine cliff
at Domata (above), annotated to highlight various sedimentary relationships
(below). The cliff comprises mostly moderately bedded gravels of the
lower-fan sequence. The lower contact of the lower-fan gravels (white dashed
line) is irregular and sub-horizontal, with lower-fan bedding (white dotted
lines) lapping onto it. Some individual horizons within the lower-fan
deposits can be traced laterally for hundreds of metres, but channelling,
bed-lensing and pinch-outs are present. Note also the exposed marine cliff
beneath the upper-fan surface (behind the forested lower-fan surface).
<bold>(b)</bold> Looking west across the Klados River mouth (foreground), the
uplifted shoreline attributed to the AD 365 earthquake (dashed red line,
lower left) aligns well with a low terrace riser on the west side of the
river (thick dashed white line, middle). Incision of the modern channel below
the surface is attributable to post-earthquake adjustment to new base levels.
Note the sea cliffing of the last interglacial marine terrace (thick dashed
red line at the top of the image) and the upper- and lower-fan deposits. The
upper fan and western parts of the lower fan are overlain by accumulated
rockfall debris and the solid thin white line approximates its surface. The
lower-fan surface is marked with a fine dotted white line. <bold>(c)</bold>
Annotated image of the west end of Domata beach illustrating the relationship
between the unconformity at the base of the fan sequence and the AD 365
bioerosional notch. Specifically, the picture shows a dissected erosional
surface on older sediments that predates the fan deposits and the AD 365
bioerosional notch post-dating both the erosional surface and the fan
deposits that rest on it. The picture was taken about 150 <inline-formula><mml:math id="M177" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> west of
the mouth of the Klados River.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f06.jpg"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p>Individual IRSL ages for all selected aliquots and
resulting kernel density estimates. Mean: arithmetic mean; SD: standard deviation; SE: standard error; CAM: Central Age Model; MAM: Minimum Age Model. The box plots, below the main graph, describe the
dose distribution as follows: median as bold line, box delimited by the
first and third quartiles, and whiskers defined by the extremes within 1.5
interquartile ranges.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f07.pdf"/>

        </fig>

      <p>Another subtle geomorphic feature of interest is a bioerosion
notch indicating an uplifted palaeo-shoreline at <inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M179" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>
above the present sea level at the west end of Domata beach (Fig. 6b
and c). This notch continues west and east from Domata and has
been mapped around the coastline of western Crete and attributed
to a seismically uplifted palaeo-shoreline dated at <inline-formula><mml:math id="M180" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> AD 365
(e.g. Pirazzoli et al., 1982, 1996; Shaw et al., 2008). Figure 6c
illustrates the relationship between the unconformity at the base
of the fan sequence and the AD 365 bioerosional notch. Our
interpretation of the stratigraphy is as follows: a dissected
erosional surface on older sediments predates the fan deposits,
while the AD 365 bioerosional notch post-dates both the older
surface and the fan deposits that rest on it. Here it is evident
that the unconformity does not represent the same feature as the
AD 365 bioerosional notch. Instead, Fig. 6c clearly shows that the
AD 365 bioerosional notch post-dates both the deeply dissected
erosional surface (of older deposits) and the fan deposits that
rest on it. In other words, the apparent coincidence of the
“wave-cut bench” and the AD 365 bioerosional notch that may
appear locally at Domata cannot mean that the entire Domata fan
deposits are Holocene in age (as it was suggested in the
discussion associated with this article). Further, the presence of
a small terrace on the west side of the Klados River (Fig. 6b), at
approximately the same elevation (6 <inline-formula><mml:math id="M181" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>) as the bioerosion
notch, represents an alluvial terrace stranded by that uplift. As
with the lower-fan surface, this terrace has been trimmed by the
sea. This late-stage uplift resulted in a readjustment of the
Klados River bed and incision near the mouth of the stream
(Fig. 6b).</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Luminescence dating of alluvial fans</title>
      <p>To place chronological constrains on the series of geomorphic
features described here from Domata, we collected, in steel
tubes, five samples for optically stimulated luminescence (OSL) dating from depths ranging from 0.24 to
1.1 <inline-formula><mml:math id="M182" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> below the ground surface (Table 1). One sample was
collected from close to the surface of the upper fan (UF-1) to
constrain the end of the upper-fan aggradation (surface
abandonment) and the initiation of incision (Figs. 3 and
5a). A further sample (RB-1) was collected from the upper-fan
deposits exposed in the lower reaches of the Domata stream cliff
to constrain the age of deposition of the early upper-fan deposits
(Figs. 3 and 5a). Two samples collected from close to the
lower-fan surface (LF-1a/b and LF-2a/b) were to provide
constraints on the timing of lower-fan abandonment and initiation
of incision (Figs. 3 and 5a). A further sample (UF-2) was
collected from deposits (silty sand) mantling both the lower- and
upper-fan surfaces, near the east end of the Domata beach to test
its age relative to UF-1 and UF-2. The results of the luminescence
analysis are presented in Table 1 and Fig. 7.</p>
<sec id="Ch1.S3.SS2.SSS1">
  <title>Sample preparation and measurements</title>
      <p>All samples were dated in the luminescence lab at Humboldt
University of Berlin (Germany), where they were prepared under
subdued red light according to standard procedures. After
separating the wanted grain size fractions by wet sieving
(38–63 and 90–200 <inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>), carbonates and
organic material were removed using 10 % hydrochloric acid and
10 % hydrogen peroxide. Quartz and potassium feldspar were
extracted from the coarser-grain fraction by density separation
using heteropolytungstate heavy liquid (LST) of 2.75, 2.62 and
2.58 <inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. The subsequent etching of the separated
quartz with hydrofluoric acid (40 %, 60 <inline-formula><mml:math id="M185" display="inline"><mml:mi mathvariant="normal">min</mml:mi></mml:math></inline-formula>)
eliminated any potential feldspar contamination and removed the
alpha-irradiated outer grain layer. From the finer fraction of
38–63 <inline-formula><mml:math id="M186" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> sediment, quartz was isolated by a 2-week treatment
with 38 % hexafluorosilicic acid. After renewed sieving, small
multiple-grain aliquots (2 <inline-formula><mml:math id="M187" display="inline"><mml:mi mathvariant="normal">mm</mml:mi></mml:math></inline-formula>) of etched
quartz (90–200 and 38–63 <inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>) and potassium feldspar
(90–200 <inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>) were prepared.</p>
      <p>Quartz OSL measurements were
performed on a Risø TL/OSL-DA-15 reader (blue LED stimulation
at 470 <inline-formula><mml:math id="M190" display="inline"><mml:mi mathvariant="normal">nm</mml:mi></mml:math></inline-formula> and detection through a Hoya U-340 filter with
transmission centred on 330 <inline-formula><mml:math id="M191" display="inline"><mml:mi mathvariant="normal">nm</mml:mi></mml:math></inline-formula>) and on a Lexsyg
luminescence measurement system (green LED stimulation at
525 <inline-formula><mml:math id="M192" display="inline"><mml:mi mathvariant="normal">nm</mml:mi></mml:math></inline-formula> and detection through a Schott BG3 Delta-BP 365/50
EX-interference filter combination at 380 <inline-formula><mml:math id="M193" display="inline"><mml:mi mathvariant="normal">nm</mml:mi></mml:math></inline-formula>). Feldspar
IRSL (infrared stimulated luminescence) measurements were
conducted on a Lexsyg luminescence measurement system
(IR laser diode)
stimulation at 850 <inline-formula><mml:math id="M194" display="inline"><mml:mi mathvariant="normal">nm</mml:mi></mml:math></inline-formula> and detection through a Schott BG39
AHF BrightLine HC 414/46 interference filter combination at
410 <inline-formula><mml:math id="M195" display="inline"><mml:mi mathvariant="normal">nm</mml:mi></mml:math></inline-formula>). Quartz palaeo-doses were measured using a SAR
(single aliquot regenerative) protocol according to Murray and Wintle
(2000, 2003), with the preheat temperature set to 240 <inline-formula><mml:math id="M196" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C
(10 <inline-formula><mml:math id="M197" display="inline"><mml:mi mathvariant="normal">s</mml:mi></mml:math></inline-formula>) and test dose cut heat to 160 <inline-formula><mml:math id="M198" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. Wallinga
et al. (2000) introduced the SAR protocol to the IRSL dating of
potassium feldspar. It was modified here following Blair
et al. (2005), applying equal preheat procedures after every
irradiation step (250 <inline-formula><mml:math id="M199" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, 60 <inline-formula><mml:math id="M200" display="inline"><mml:mi mathvariant="normal">s</mml:mi></mml:math></inline-formula>). The appropriate
preheat temperatures and durations were identified conducting dose
recovery tests on samples RB-1 and LF-2a/b (SAR equivalent dose
determinations of known lab doses with varying preheat
temperatures). Quartz was stimulated at 125 <inline-formula><mml:math id="M201" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C for
40 <inline-formula><mml:math id="M202" display="inline"><mml:mi mathvariant="normal">s</mml:mi></mml:math></inline-formula>, feldspar at 50 <inline-formula><mml:math id="M203" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C for 300 <inline-formula><mml:math id="M204" display="inline"><mml:mi mathvariant="normal">s</mml:mi></mml:math></inline-formula>. The
built-in beta sources (Sr-90) emitted 0.068 <inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:mi mathvariant="normal">Gy</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
(Lexsyg) and 0.093 <inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:mi mathvariant="normal">Gy</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (Risø). The
sediment dose rates were estimated by measuring the contents of
uranium, thorium and potassium on a high-resolution gamma
spectrometer. The cosmic-ray dose rates were estimated from
geographic position, elevation and burial depth (Prescott and
Hutton, 1994).  The internal potassium content of the measured
feldspar was assumed to be <inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:mn mathvariant="normal">12.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> % according to
Huntley and Baril (1997).</p>
</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <title>Luminescence results</title>
      <p>Quartz OSL dating results reported in Pope et al. (2008) and OSL
and U series dating of Pope et al. (2016) proved the suitability
of standard quartz SAR protocols for dating fan sediments along
the nearby Sfakia piedmont in southern Crete (Fig. 1). In
contrast, the investigated quartz from Domata showed poor
luminescence properties: the OSL signals were dim, dose recovery
tests yielded unsatisfactory results, the highly scattering
palaeo-doses produced positively skewed broad distributions and the
resulting quartz ages showed no relationship with stratigraphy
(underestimation of true age). This led to the conclusion that
quartz is not an appropriate material for dating the alluvial
fans at Domata. The most likely explanation for the
unsuitability of the quartz (weak, or even missing, fast OSL
signal component) is the dominance in our samples of fresh
insensitive quartz, which had undergone a few sedimentation cycles
(Preusser et al., 2006; Steffen et al., 2009). Thus,
potassium feldspar (IRSL) was used to date the landforms
at Domata instead.</p>
      <p>The feldspar (IRSL) dating produced reliable age ranges
(Fig. 7). Best results for dose recovery tests on
laboratory-bleached feldspar samples from Domata were obtained
without applying any sensitivity correction. Thus, a simplified
SAR protocol without test dose measurement was used for the
palaeo-dose determination of the natural potassium feldspar
samples. No fading tests were made to correct for any potential
age underestimation.  Sensitivity changes were assessed by
repeating the first irradiation step at the end of each SAR cycle
assuming that the luminescence intensities should coincide
(recycling ratio close to 1.0). Here, a recycling ratio between
0.85 and 1.15 was tolerated. The <inline-formula><mml:math id="M208" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> value for assessing the
alpha particle contribution to the palaeo-dose was set to <inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> (Balescu and Lamothe, 1994). Basic statistical values are
presented in Table 1. Under perfect conditions the arithmetic
mean and the median should coincide. However, here the mean value is
always larger compared to the median, which is typical for positively
skewed age distributions. This can indicate insufficient exposure
of the sediment to daylight during the last sedimentation
cycle. However, also post-depositional mixing, contamination with
younger grains from the surface (low sampling depth,
bioturbation) or microdosimetric inhomogeneities are also possible
reasons for skewed age distributions. Compared to the mean, the
median is less sensitive to large outliers (RB-1, LF-1a/b). The
Central Age Model (CAM) and the Minimum Age Model (MAM) according to
Galbraith et al. (1999) were used to further describe the age
distributions (Fig. 7 and Table 1). Minimum age models are
recommended when dating mixed-age sediments, yielding broad age
distributions to better estimate the population of well-bleached
grains (Galbraith and Roberts, 2012).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p><bold>(a)</bold> The two alluvial fans with their tree cover (<italic>Pinus brutia).</italic> Arrows
indicate the  soil cover that develops on each of the fan surfaces. <bold>(b)</bold>
The soil development on the lower-fan (LF) surface is <inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">12</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M211" display="inline"><mml:mi mathvariant="normal">cm</mml:mi></mml:math></inline-formula>
(as indicated by the white arrows). <bold>(c)</bold>  The soil development on the
upper-fan (UF) surface is <inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M213" display="inline"><mml:mi mathvariant="normal">cm</mml:mi></mml:math></inline-formula> (see white arrows). The fan
gravel in both cases is indicated.</p></caption>
            <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f08.pdf"/>

          </fig>

      <p>Collectively, our potassium feldspar measurements suggest that
the ages of the landforms at Domata range between <inline-formula><mml:math id="M214" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">55</mml:mn></mml:mrow></mml:math></inline-formula> and
25 <inline-formula><mml:math id="M215" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP (Table 1). All mean values indicate a last
glacial age for all samples and appear in stratigraphic
order. Median values are all in stratigraphic sequence (except
for LF-2a/b), although they are significantly younger than the
mean and the CAM values. The CAM ages are consistent with the
mean and median values in indicating a last glacial age (MIS3)
for all samples. The CAM series data are all in stratigraphic
order (except for the LF-2a/b sample), and the absolute values
are younger than the means. The MAM ages lean towards the
younger end of the timescale, which is to be expected because
they are the minimum possible ages, not the most likely ages.</p>
      <p><?xmltex \hack{\newpage}?>Thus, the chronostratigraphy of the majority of the geomorphic
landforms formed during MIS 3 (29–57 <inline-formula><mml:math id="M216" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>). When used in
conjunction with the sequence of events dictated by the
stratigraphy presented in Sect. 3.1 and the Siddall et al. (2003)
sea-level curve, the chronology of the geomorphic events that
formed the landscape at Domata can be established reasonably
well, despite the significant errors in the luminescence
measurements (Fig. 7). The landscape evolution, including its
chronology, is discussed in Sect. 4.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS3">
  <title>Soil development</title>
      <p>We have performed a macroscopic soil profile characterisation for
the soil horizons that develop on the two fan surfaces
(Fig. 8a). The fan surfaces dip gently, with a maximum
gradient of <inline-formula><mml:math id="M217" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:math></inline-formula> to 8<inline-formula><mml:math id="M218" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and incision is restricted to a few
dry and shallow (<inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M220" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>) creek courses. Thus, erosion on
these surfaces is expected to be minimal. Nevertheless, to
minimise the effect of soil erosion, we performed our soil profiles
away from creek incisions.</p>
      <p>The soils at Domata are categorised as Leptosols (Soil Atlas of
Europe, 2005; FAO, 2006) and comprise a shallow (<inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M222" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>) soil cover over coarse sediment of highly
calcareous material (Fig. 8). Soils on both the upper and
lower fans have common parent material (fan gravels), mainly
consisting of limestone pebbles and cobbles, and the fans are
covered by pine trees (<italic>Pinus brutia</italic>) (Fig. 8a). However, the soils
of the upper- and lower-fan surfaces differ
macroscopically and in their physical, biochemical and geochemical
parameters. Soil thickness, averaged from six soil profiles, varies
from 0.1 <inline-formula><mml:math id="M223" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> (Fig. 8b) beneath the lower-fan surface to
0.4 <inline-formula><mml:math id="M224" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> (Fig. 8c) beneath the upper-fan surface. The upper-fan soil
is yellowish brown with A and (weak) B horizons and texture from
subangular to granular, while the lower-fan soil is yellowish with
granular texture and has no distinct horizons (apart from a very
thin horizon A) (Fig. 8b and c).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p>The IRSL chronology of the geomorphic features at Domata
plotted against a simplified version of the global sea-level curve after
Siddall et al. (2003). The shaded zone in the background represents the stated error range of Siddall
et al. Large filled circles represent means of IRSL
dates, small filled circles represent medians and the bars are error bars (at 1<inline-formula><mml:math id="M225" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>). The geomorphic event sequence described in the text is shown above the
figure and the favoured of three alternative high sea-level stands within
MIS 3 to have trimmed the upper-fan surface
is identified with a solid vertical blue line at 39 <inline-formula><mml:math id="M226" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP.</p></caption>
          <?xmltex \igopts{width=284.527559pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f09.pdf"/>

        </fig>

      <p>Comparison of the macroscopic characteristics of the soils at
Domata with the soils identified at the piedmonts at the nearby
region of Sfakia (Fig. 1) by Pope et al. (2008) provides
additional evidence that the alluvial fan system at Domata was
formed during MIS 3 (as constrained by the IRSL
dating). Specifically, at Domata we find soils the characteristics
of which closely resemble the soils that developed at Sfakia
during stage 2C (70–16 <inline-formula><mml:math id="M227" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP), while there is a total
absence of older soils that developed during stage 2A (<inline-formula><mml:math id="M228" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">144</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M229" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>) (Pope et al., 2008). The former (stage 2C) is
a brown to yellowish-brown soil with limited B horizon and
subangular texture, characteristics that match the soils at
Domata, whereas the latter contains highly crystalline iron oxides
with a clear B horizon.</p>
      <p>The macroscopic observations (upper-fan soil is thicker and redder) also
imply that the upper-fan soil is more mature compared to that of
the lower fan. Preliminary geochemical analysis (Moraetis et al.,
2015) confirms that the soil in the upper fan is more mature (e.g. older),
as it has lower specific surface area and higher
content of well-shaped hematite (and less goethite) compared to
that in the lower fan (Wang et al., 2013). This observation is also in
agreement with soil analysis in the nearby region of Sfakia
(Fig. 1), where Pope et al. (2008) showed that the soil redness
and the content of crystalline iron oxide (hematite) increase with
increasing alluvial fan age. The greater age of the upper-fan soil
compared to the lower-fan soil is also independently demanded by our
stratigraphic observations on crosscutting and incision of fans
and the luminescence dating that shows that the upper-fan surface
developed at least 5 <inline-formula><mml:math id="M230" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> earlier than the lower-fan
surface (see discussion in Sect. 4; Table 1). According to Lair
et al. (2009) and Huang et al. (2016), the <inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M232" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>
difference in the residence time between the two soil horizons is
sufficient to generate the recorded macroscopic and geochemical
changes.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><caption><p>The sequence of events that contributed to the
development of the landscape at Domata is schematically illustrated: <bold>(a)</bold>
upper-fan deposition due to sea-level high stand (base level);  <bold>(b)</bold>
abandonment of the upper-fan surface due to falling sea level;  <bold>(c)</bold> sea-level
rise resulting in the trimming of the upper-fan deposits and cutting
of a marine bench;  <bold>(d)</bold> lower-fan deposition starts during relatively high
sea level and laps against both the river incision cliff and the coastal
cliff in the upper fan; <bold>(e)</bold> as sea level falls, the lower-fan surface is
abandoned through entrenchment;  <bold>(f)</bold> a return to high sea level results in
coastal trimming of the lower-fan deposits;  <bold>(g)</bold> one or more earthquakes in
the first millennium AD resulted in 6 <inline-formula><mml:math id="M233" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> of uplift at Domata and
corresponding adjustments to the lower Klados River geomorphology. The
approximate chronology of each stage is annotated.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f10.pdf"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <title>Interpretation of landscape evolution at Domata</title>
      <p>According to our luminescence age range and the relative location
of the fan surfaces below the marine terrace (see Fig. 2) of
inferred MIS5 age, the majority of the geomorphic landforms at
Domata we discuss formed during MIS 3 (29–57 <inline-formula><mml:math id="M234" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>)
(Table 1 and Figs. 2 and 7). The sequence of events that resulted
in the development of the landscape at Domata, as dictated by the
analysis of the geomorphic landforms and the superposition of the
luminescence dating onto the well-established sea-level curve of
Siddall et al. (2003)<fn id="Ch1.Footn1"><p>The shape of the sea-level
fluctuations varies slightly globally. Thus, in this
work we designate the empirical, high-resolution sea-level curve of Siddall
et al. (2003) from the Red Sea that covers the last
128 <inline-formula><mml:math id="M235" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>. Siddall et al. (2003) estimate the error in
their sea-level curve at <inline-formula><mml:math id="M236" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">12</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M237" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>, thus, all sea-level
elevations discussed subsequently are subject to this
uncertainty.</p></fn> (Fig. 9), is as following (from oldest to youngest)
(Fig. 10): (a) deposition of the upper-fan materials (Fig. 10a);
(b) river entrenchment leading to abandonment of the upper-fan
surface (Fig. 10b); (c) marine trimming of the upper-fan surface
deposits, the fan deposits and its alluvial entrenchment cliff
(Fig. 10c); (d) deposition of the lower-fan materials against the
upper-fan materials in its alluvial entrenchment cliff and the
sea cliff in the upper fan (Fig. 10d); (e) river entrenchment
leading to abandonment of the lower-fan surface (Fig. 10e); (f)
marine trimming of the lower-fan deposits and the alluvial
entrenchment cliff (Fig. 10f); and (g) seismic uplift resulting in
a stranded palaeo-shoreline, the development of a river terrace
riser and the oversteepening of the lower river channel
(Fig. 10g). In the following discussion we provide evidence in
support of each stage of the landscape evolution at Domata and
establish its relative chronology.</p>
      <p>The initiation of deposition of the upper fan (Fig. 10a) has
occurred post <inline-formula><mml:math id="M238" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M239" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP and prior to
45 <inline-formula><mml:math id="M240" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> (RB-1 sample; within MIS 3 of Lisiecki and Raymo,
2005; Table 1); this coincides with a period of elevated sea level
(ca. <inline-formula><mml:math id="M241" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>70 to <inline-formula><mml:math id="M242" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>80 <inline-formula><mml:math id="M243" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> according to the sea-level curve of Siddall et al. (2003); Fig. 9).  We argue that upper-fan deposition cannot have
started as early as 53.4 <inline-formula><mml:math id="M244" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> (mean of RB-1 sample;
Table 1) because there is no geomorphic evidence (e.g. marine
cliffs) representing the two subsequent high sea-level stands at
ca. 45 and 39 <inline-formula><mml:math id="M245" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>. Thus, the deposition of the upper fan
post-dates 53 <inline-formula><mml:math id="M246" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> and is completed by <inline-formula><mml:math id="M247" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">45</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M248" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP, when the sea level rose to reach
ca. <inline-formula><mml:math id="M249" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>72 <inline-formula><mml:math id="M250" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> (Siddall et al., 2003). The period that
follows, between 45 and 41 <inline-formula><mml:math id="M251" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>, reflects the start of
a cooling climatic period (possibly with an increase in sediment
supply) and a falling sea level to <inline-formula><mml:math id="M252" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>87 <inline-formula><mml:math id="M253" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> (Fig. 9). During
this period, alluvial fan entrenchment resulted in fan surface
abandonment and development of the alluvial cliff in the upper-fan
deposits (Fig. 3), and the upper fan was eventually abandoned
(Fig. 10b). This was followed, at <inline-formula><mml:math id="M254" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">39</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M255" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP, by
marine transgression resulting in marine trimming of the upper-fan
surface, the alluvial entrenchment cliff and development of
a sub-horizontal marine abrasion surface in early upper-fan
deposits at about the sea level of the time (ca. <inline-formula><mml:math id="M256" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>70 <inline-formula><mml:math id="M257" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>)
(see yellow dashed line on the river cliff in Figs. 3, 9 and
10c). This allowed up to 10 000 <inline-formula><mml:math id="M258" display="inline"><mml:mi mathvariant="normal">years</mml:mi></mml:math></inline-formula> for upper-fan
deposition and incision before the fan is trimmed by the sea
during the high sea-level peak at ca. 39 <inline-formula><mml:math id="M259" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>.</p>
      <p>Lower-fan deposition commenced (Fig. 10d) soon after marine
trimming of the upper fan (Fig. 9). The relatively high sea level
at 37 <inline-formula><mml:math id="M260" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> (ca. <inline-formula><mml:math id="M261" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>75 <inline-formula><mml:math id="M262" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>; see Fig. 9) promoted fan
deposition, and the possibly deteriorating climatic conditions,
involving episodically increased river flow and/or carrying capacity and
diminishing vegetation density in the upper catchment, resulted
in increased sediment supply. Lower-fan deposits lapped against
alluvial entrenchment and marine cliffs cut previously in
upper-fan deposits by alluvial incision along the Klados River and
by the marine trimming sub-parallel to the modern shoreline
(Fig. 10d). Lower-fan surface abandonment and river entrenchment
through incision commenced at <inline-formula><mml:math id="M263" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">36</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M264" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> (LF-2a/b
sample; Table 1). We argue that the lower-fan surface was
abandoned (Fig. 10e) sometime between <inline-formula><mml:math id="M265" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">36</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M266" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> and
29 <inline-formula><mml:math id="M267" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> due to river entrenchment resulting from a rapidly
falling sea level (that continued until <inline-formula><mml:math id="M268" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">18</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M269" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>)
(Fig. 9).</p>
      <p>Marine trimming of the lower-fan surface and deposits cannot have
occurred between deposition and the last glacial maximum (<inline-formula><mml:math id="M270" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">18</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M271" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>), as the sea level progressively declined during that
period. Following 18 <inline-formula><mml:math id="M272" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>, the sea level rose rapidly by <inline-formula><mml:math id="M273" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M274" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> in less than 10 <inline-formula><mml:math id="M275" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> (Fig. 9). The marine
trimming of the lower-fan surface and deposits occurred during the
Holocene high sea-level stand. This is expected to have commenced
as the sea level approached roughly the present level
ca. 4–5 <inline-formula><mml:math id="M276" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> ago (Fig. 10f).  Between 18 and
5 <inline-formula><mml:math id="M277" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP, while the sea level was rising fast, tectonic
uplift at Domata must have outpaced the rising sea level, protecting
the entire sequence from marine inundation and
destruction. Immediately prior to the co-seismic uplift that
affected western Crete at AD 365 (Pirazzoli et al., 1982), the
foot of the lower marine cliff would have been within the
intertidal zone. Today, due to the 6 <inline-formula><mml:math id="M278" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> of uplift
associated with that earthquake, the prominent stranded
palaeo-shoreline and the foot of the marine-trimmed cliff are at
approximately similar levels and the sea cliff may be isolated
from further trimming (Figs. 6b and 10g). We interpret a low
terrace riser at about this elevation near the mouth of the Klados
River (see lower white dashed line in Fig. 6b) to be a relict from
the river channel of that time, and in the lower ca. 100 <inline-formula><mml:math id="M279" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>
of its course the river has downcut in response to that
first-millennium earthquake uplift.</p>
      <p>In summary, deposition of the upper and lower fan was controlled
by a marine base level and, in both cases, fan incision resulted
due to the falling sea level. The deposition of the upper fan was
largely completed by <inline-formula><mml:math id="M280" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">45</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M281" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP, during a period of
relatively high sea level (ca. <inline-formula><mml:math id="M282" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>70 <inline-formula><mml:math id="M283" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>), and fan incision
resulting in surface abandonment occurred between ca. 45 and
40 <inline-formula><mml:math id="M284" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>. Marine trimming of the upper-fan deposits occurred
during a sea-level high (ca. <inline-formula><mml:math id="M285" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>72 <inline-formula><mml:math id="M286" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>) at
ca. 39 <inline-formula><mml:math id="M287" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>. Lower-fan deposition was initiated soon
afterwards and fan surface abandonment occurred between 36 and
29 <inline-formula><mml:math id="M288" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>.  The age of the sandy unit that mantles both the
upper- and the lower-fan surfaces is <inline-formula><mml:math id="M289" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M290" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> (UF-2;
Fig. 9 and Table 1), post-dating both fans as expected by its
stratigraphic relationship with respect to the fans (silty sand
that mantles both the lower and upper fans).</p>
</sec>
<sec id="Ch1.S5">
  <title>The importance of tectonic uplift at Domata</title>
      <p>The fan sequence at Domata provides a unique opportunity to link
terrestrial deposition with sea-level fluctuations and vertical
tectonics on southwestern Crete. Geomorphic analysis combined with
dating shows that the development of the fan sequence can be
accounted for by eustatic changes coupled with vertical
tectonics. The latter can be rationalised if we consider that the
landforms at Domata were formed 70 to 90 <inline-formula><mml:math id="M291" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> (within the
known error margins) below the current sea level, implying that,
unless tectonic uplift was significant, the entire sequence would
have been inundated, and thus modified or destroyed, by the rising
sea level during the last 20 <inline-formula><mml:math id="M292" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> (Siddall et al.,
2003). A requirement of its preservation is that since its
deposition, the tectonic uplift rate has outpaced the rising
sea level. Thus, a question that arises concerns the relationship between the rate of tectonic uplift and rising sea level at Domata. Dating key terrestrial and marginal
marine geomorphological features at Domata provided an
average uplift rate for this part of Crete that can be compared to
the rate of rising sea level and also to other rates of tectonic
uplift on western Crete (which have been independently
derived). It also provides a means of testing the main finding of
Pope et al. (2016) that, during the late Quaternary, the landscape at
the nearby site of Sfakia mainly responded to sea-level and
climatic changes.</p>
      <p>Our data show that the marine trimming episode at
ca. 39 <inline-formula><mml:math id="M293" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> left a coastal cliff and cut an erosional
intertidal abrasion surface in the upper-fan deposits (see yellow
dashed line in Fig. 3). This surface provides a good datum upon
which to estimate subsequent uplift. Indeed, a total uplift of
86 <inline-formula><mml:math id="M294" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M295" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> the 12 <inline-formula><mml:math id="M296" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> error margin of the sea-level
curve) is required to elevate this marine abrasion surface to its
current altitude of 14 <inline-formula><mml:math id="M297" display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula>  Thus, the minimum uplift
rate required to accomplish this is ca. 2.2 <inline-formula><mml:math id="M298" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.
Indeed, the plot in Fig. 11 shows that with an average rate of
<inline-formula><mml:math id="M299" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">2.2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M300" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> since formation (black line), the
fan sequence would have escaped the destructive interaction with
the wave zone and, therefore, modification due to erosion (e.g.
the black line of uniform uplift rate does not intersect the
sea-level curve during the last 39 <inline-formula><mml:math id="M301" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>).  Independent
support for similar uplift rates comes from published radiocarbon
ages on beachrock materials that mantle marine palaeo-shorelines in
nearby localities: a calibrated radiocarbon age of
36 790–38 694 <inline-formula><mml:math id="M302" display="inline"><mml:mi mathvariant="normal">yr</mml:mi></mml:math></inline-formula> BP from reworked rhodoliths in
beachrock at an elevation of 10.5 <inline-formula><mml:math id="M303" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> at Sougia,
9 <inline-formula><mml:math id="M304" display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> to the west of Domata, is within a few thousand years
of the proposed timing of marine trimming of the upper fan and
yields an average uplift rate of 2.4 <inline-formula><mml:math id="M305" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
(Mouslopoulou et al., 2015a). Similarly, beachrock on a marine
terrace at 17 <inline-formula><mml:math id="M306" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> elevation at Palaiochora, 20 <inline-formula><mml:math id="M307" display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula>
west of Domata, yields a calibrated radiocarbon age of
36 682–38 732 <inline-formula><mml:math id="M308" display="inline"><mml:mi mathvariant="normal">yr</mml:mi></mml:math></inline-formula> BP, producing an average uplift rate
of 2.5 <inline-formula><mml:math id="M309" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (Mouslopoulou et al.,
2015a). Comparable uplift rates (1.8–2.7 <inline-formula><mml:math id="M310" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)
have been independently recorded for the last <inline-formula><mml:math id="M311" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> 000 <inline-formula><mml:math id="M312" display="inline"><mml:mi mathvariant="normal">years</mml:mi></mml:math></inline-formula> at numerous localities on western Crete by
Shaw et al. (2008), Strasser et al. (2011) and Tiberti
et al. (2014). Thus, the preservation and subaerial exposure of
the landscape at Domata is due to the sufficient tectonic uplift
that southern Crete experienced during the late Quaternary.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11"><caption><p>The plot discusses the required uplift rate to elevate
the marine cliff and bench
of the upper fan from its elevation at genesis (39 <inline-formula><mml:math id="M313" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP) to its present elevation (<inline-formula><mml:math id="M314" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>14 <inline-formula><mml:math id="M315" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>). The simplified sea-level curve
(after Siddall et al., 2003) is illustrated by the thick blue line. The black
line represents a constant uplift rate of 2.2 <inline-formula><mml:math id="M316" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (established in this
study). The dashed red line represents a minimum uplift rate for Domata of
<inline-formula><mml:math id="M317" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">5.3</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M318" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> tailored to empirical data (Tiberti et al., 2014;
Mouslopoulou et al., 2015b). The solid red line represents the uplift rate
required for the fan system to escape marine inundation and
destruction (see text for details).</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/5/511/2017/esurf-5-511-2017-f11.pdf"/>

      </fig>

      <p>In order to quantify the relative contribution of tectonics and
eustasy to the formation of the landscape at Domata, here we
compare published information on incremental uplift rates
calculated by Tiberti et al. (2014) and Mouslopoulou
et al. (2015b) for western Crete over the last <inline-formula><mml:math id="M319" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M320" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> with the uplift rate calculated for Domata over
the last 39 <inline-formula><mml:math id="M321" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> (ca. 2.2 <inline-formula><mml:math id="M322" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>; this
study). Comparison shows that during the time period over which
the key features at Domata formed (MIS 3), no significant uplift
was accommodated on Crete as the region was experiencing a tectonically quiet period
with no uplift (Mouslopoulou et al., 2015b) or even gentle
subsidence between <inline-formula><mml:math id="M323" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> and 45 <inline-formula><mml:math id="M324" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> (Tiberti et al., 2014). Thus, the shaping of the
landscape at Domata during MIS 3 must have been largely achieved
by sea-level fluctuations. This comparison also suggests that most
of the <inline-formula><mml:math id="M325" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">80</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M326" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> of uplift (subtracting 6 <inline-formula><mml:math id="M327" display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> of
late Holocene co-seismic uplift) has been accumulated sometime
between 5 and 20 <inline-formula><mml:math id="M328" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP, resulting in an average uplift
rate of 5.3 <inline-formula><mml:math id="M329" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (Fig. 11; dashed red
line). However, this uplift rate would have been insufficient to
outpace the rising sea level between 8 and 12 <inline-formula><mml:math id="M330" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP (see
dashed red line intersecting the sea-level curve in Fig. 11) and
thus the fan sequence would have been inundated and modified or
destroyed by the rising sea level.  This, in turn, implies that
the uplift rate at Domata was higher than
5.3 <inline-formula><mml:math id="M331" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. We favour a scenario in which uplift was
mostly accommodated by about 9 <inline-formula><mml:math id="M332" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP, at an average rate of
<inline-formula><mml:math id="M333" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M334" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (see solid red line in Fig. 11 that
does not intersect the sea-level curve). Comparable uplift rates
(7–8 <inline-formula><mml:math id="M335" display="inline"><mml:mrow><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) have been independently recorded at
numerous localities on western and eastern Crete for the last
20 000 <inline-formula><mml:math id="M336" display="inline"><mml:mi mathvariant="normal">years</mml:mi></mml:math></inline-formula> by Tiberti et al. (2014) and Mouslopoulou
et al. (2015b) and they result from transient earthquake slip on
upper-plate faults that splay off the plate interface and extend
beneath Crete at relatively steep angles (Mouslopoulou et al.,
2015b).  Such transient rates have been observed at several other
margins globally (Mouslopoulou et al., 2016, and references
therein).</p>
      <p><?xmltex \hack{\newpage}?>Thus, the development and evolution (<inline-formula><mml:math id="M337" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula>–20 <inline-formula><mml:math id="M338" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP) of the suite of geomorphic features at
Domata can be largely explained by eustatic sea-level fluctuations
and sedimentation variations controlled by climatic conditions,
without the requirement for significant vertical movements. This
conclusion largely supports the main finding of Pope
et al. (2016), who dated a fan sequence at Sfakia
(ca. 25 <inline-formula><mml:math id="M339" display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> to the east of Domata). However, it is the subsequent tectonic uplift that preserved and subaerially exposed
the coastal geomorphic features.</p>
      <p>Intriguing conclusions of the Pope et al. (2016) high-resolution dating work also include that
three sometimes overlapping phases of fan deposition since the last interglacial are separated
by two phases of fan entrenchment, the first close
to the MIS 5–4 (ca. 70 <inline-formula><mml:math id="M340" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>) boundary, the other close to
the MIS 2–1 boundary (ca. 14 <inline-formula><mml:math id="M341" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>), triggered by major
climatic changes. Fan deposition at Sfakia has to a large degree
persisted through stadial and interstadial periods during the last
125 <inline-formula><mml:math id="M342" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula>. Periods of entrenchment at Sfakia do not appear
to correlate with the two entrenchment periods at Domata. The
Sfakia fan is somewhat different from the Domata fan in catchment
size (ca. 28 <inline-formula><mml:math id="M343" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> compared with ca. 11 <inline-formula><mml:math id="M344" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>),
fan size (5.3 <inline-formula><mml:math id="M345" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> compared with 0.1 <inline-formula><mml:math id="M346" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>),
the presence of more than one feeder channel at Sfakia, and in the
nature of deposits (primarily clast-supported gravels at Sfakia
compared with primarily matrix-supported gravels at
Domata). Whether these differences are responsible for differences
in depositional and entrenchment histories and in preservation of
marine cliffs at Sfakia is uncertain. However, one
conclusion of the work of Pope et al. (2016) compatible with our own is recognition of
the importance of base-level (sea-level) changes in the process of
incision.</p>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <title>Conclusions</title>
      <p>Alluvial fans often provide a useful index with which to decode the
information recorded on the landscape in complex tectonic settings,
such as those of the eastern Mediterranean. Herein we use analysis of
geomorphic landforms and luminescence dating on an alluvial fan
system with two separate periods of depositional activity on Crete,
an island straddling the forearc of the Hellenic subduction margin,
to constrain its vertical deformation and discuss the contributing
factors responsible for its landscape evolution. Our
interpretations suggest that sea-level fluctuations in response to
varying climatic conditions formed the landscape at Domata during
MIS 3 (<inline-formula><mml:math id="M347" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">57</mml:mn></mml:mrow></mml:math></inline-formula>–29 <inline-formula><mml:math id="M348" display="inline"><mml:mi mathvariant="normal">kyr</mml:mi></mml:math></inline-formula> BP). It is, however, because of
the fast tectonic uplift that Crete experienced during the
subsequent <inline-formula><mml:math id="M349" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> thousand years that the entire alluvial
sequence escaped destruction and/or modification due to marine
inundation and is subaerially preserved today. Thus, both eustasy
and tectonism impacted the formation and preservation of the
landscape at Domata, but over temporally distinct time periods.</p><?xmltex \hack{\newpage}?>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability">

      <p>All of our data are presented in the main article. There
are no more data associated with this work available.</p>
  </notes><notes notes-type="authorcontribution">

      <p>VM, JB and DM conceived the research idea and performed all associated
fieldwork and analysis of the results. AF performed the IRSL dating and
PP performed the RTK survey. OO provided guidance and contributed to the
development of the ideas presented in this article. All authors contributed
to the writing of the paper.</p>
  </notes><notes notes-type="competinginterests">

      <p>The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p>We are grateful to Nikos Mouslopoulos and the late Stavros Sartzetakis for their
generous help during fieldwork. We dedicate this work to our beloved Cretan
friend Stavros, whose spirit now wings through the gorges and across the
mountains guarding the landscape of his homeland, western Crete. We thank
the National Cadastre and Mapping Agency of Greece for providing, free of
charge, digital elevation maps and imagery for building the DEMs in Fig. 4. We are grateful to M. Tiberti, M. Brandon and the anonymous reviewer for
several constructive comments that greatly improved this article. We would
also like to thank the Associate Editor V. Vanacker and the Editor F. Herman
for efficiently handling this submission. <?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
The article processing charges for this open-access <?xmltex \hack{\newline}?> publication
were covered by a Research <?xmltex \hack{\newline}?> Centre of the Helmholtz Association.
<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Veerle Vanacker <?xmltex \hack{\newline}?>
Reviewed by: Mara Monica Tiberti, Mark Brandon, and one anonymous referee</p></ack><ref-list>
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    <!--<article-title-html>Distinct phases of eustatic and tectonic forcing for late Quaternary landscape evolution in southwest Crete, Greece</article-title-html>
<abstract-html><p class="p">The extent to which climate, eustasy and tectonics interact to shape
the late Quaternary landscape is poorly known. Alluvial fans often
provide useful indexes that allow the decoding of information recorded
on complex coastal landscapes, such as those of the eastern
Mediterranean. In this paper we analyse and date (using infrared stimulated
luminescence
(IRSL) dating) a double alluvial fan system on southwest Crete, an
island straddling the forearc of the Hellenic subduction margin, in
order to constrain the timing and magnitude of its vertical
deformation and discuss the factors contributing to its landscape
evolution. The studied alluvial system is exceptional because each
of its two juxtaposed fans records individual phases of
alluvial and marine incision, thus providing unprecedented
resolution in the formation and evolution of its landscape.
Specifically, our analysis shows that the fan sequence at Domata
developed during Marine Isotope Stage (MIS) 3 due to five distinct
stages of marine transgressions and regressions and associated river
incision, in response to sea-level fluctuations and tectonic
uplift at averaged rates of  ∼  2.2 mm yr<sup>−1</sup>. Interestingly, comparison of our results
with published tectonic uplift rates from western Crete shows that
uplift during 20–50 kyr BP was minimal (or even
negative). Thus, most of the uplift recorded at Domata must have
occurred in the last 20 kyr. This implies that eustasy
and tectonism impacted the landscape at Domata over mainly
distinct time intervals (e.g. sequentially and not synchronously),
with eustasy forming and tectonism preserving the coastal landforms.</p></abstract-html>
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