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Past Climate Variability and Change in the Arctic and at High Latitudes

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136<br />

The U.S. <strong>Clim<strong>at</strong>e</strong> Science Program Chapter 5<br />

Unfortun<strong>at</strong>ely<br />

<strong>the</strong> picture is cloudy—<br />

not unlike <strong>the</strong> basal ice<br />

itself, which has<br />

a small amount of silt<br />

<strong>and</strong> s<strong>and</strong> dispersed<br />

through it.<br />

The central Greenl<strong>and</strong><br />

cores do reveal two<br />

important facts: MIS 5e<br />

was warmer than MIS 1,<br />

<strong>and</strong> <strong>the</strong> elev<strong>at</strong>ion <strong>in</strong> <strong>the</strong><br />

center of <strong>the</strong> ice sheet<br />

was similar to th<strong>at</strong> of <strong>the</strong><br />

modern ice sheet.<br />

5.3.3c icE-shEEt changEs<br />

The GreenlAnd ice Sheet dur<strong>in</strong>g MIS 5e covered<br />

a smaller area than it does now. How much<br />

smaller is not known with certa<strong>in</strong>ty. The most<br />

compell<strong>in</strong>g evidence is <strong>the</strong> absence of pre-MIS<br />

5e ice <strong>in</strong> <strong>the</strong> ice cores from south, northwest,<br />

<strong>and</strong> East GreenlAnd (<strong>the</strong> loc<strong>at</strong>ions dYe-3, cAMp<br />

centurY, <strong>and</strong> renlAnd drill<strong>in</strong>g sites, respectively).<br />

In all of <strong>the</strong>se cores, <strong>the</strong> clim<strong>at</strong>e record<br />

extends through <strong>the</strong> entire last glacial epoch<br />

<strong>and</strong> <strong>the</strong>n term<strong>in</strong><strong>at</strong>es <strong>at</strong> <strong>the</strong> bed <strong>in</strong> a layer of ice<br />

deposited <strong>in</strong> a much warmer clim<strong>at</strong>e (Koerner,<br />

1989; Koerner <strong>and</strong> Fisher, 2002). This basal ice<br />

is most likely MIS 5e ice. Moreover, <strong>the</strong> composition<br />

of this ice is not an average of glacial<br />

<strong>and</strong> <strong>in</strong>terglacial values, as would be expected if<br />

it were a mixture of ices from earlier cold <strong>and</strong><br />

warm clim<strong>at</strong>es. Instead, <strong>the</strong> ice composition<br />

exclusively <strong>in</strong>dic<strong>at</strong>es a clim<strong>at</strong>e considerably<br />

warmer than th<strong>at</strong> of <strong>the</strong> Holocene. (One cannot<br />

entirely elim<strong>in</strong><strong>at</strong>e <strong>the</strong> possibility th<strong>at</strong> each core<br />

<strong>in</strong>dependently bottomed on a rock th<strong>at</strong> had been<br />

transported up from <strong>the</strong> bed, <strong>and</strong> th<strong>at</strong> older ice<br />

lies bene<strong>at</strong>h each rock, but this seems highly<br />

improbable.)<br />

At dYe-3, <strong>the</strong> oxygen isotope composition of<br />

this basal ice layer is reported as δ 18O = –23‰,<br />

which means th<strong>at</strong> it is 23‰ (or 2.3%) lighter<br />

than st<strong>and</strong>ard mean ocean w<strong>at</strong>er. Moreover, a<br />

value of δ 18O = –30‰ is reported for modern<br />

snowfall <strong>in</strong> <strong>the</strong> source region (up-flow from<br />

<strong>the</strong> site of dYe-3). At cAMp centurY, a value of<br />

δ 18O = –25‰ is reported for basal ice; a value<br />

of δ 18O = –31.5‰ is reported <strong>in</strong> <strong>the</strong> source<br />

region (see Table 2 of Koerner, 1989). These<br />

changes of about 7‰ are much larger than <strong>the</strong><br />

MIS 5e-to-MIS 1 clim<strong>at</strong>ic signal (about 3.3‰,<br />

accord<strong>in</strong>g to <strong>the</strong> central GreenlAnd cores; see<br />

below <strong>in</strong> this section). Thus, <strong>the</strong> MIS 5e ice <strong>at</strong><br />

dYe-3 <strong>and</strong> cAMp centurY not only <strong>in</strong>dic<strong>at</strong>es a<br />

warmer clim<strong>at</strong>e but also a much lower source<br />

elev<strong>at</strong>ion: <strong>the</strong> ice sheet was re-grow<strong>in</strong>g when<br />

<strong>the</strong>se MIS 5e ices were deposited.<br />

In comb<strong>in</strong><strong>at</strong>ion, <strong>the</strong>se two observ<strong>at</strong>ions (absence<br />

of pre-MIS 5e ice, <strong>and</strong> anomalously lowelev<strong>at</strong>ion<br />

sources of <strong>the</strong> basal ice) <strong>in</strong>dic<strong>at</strong>e th<strong>at</strong><br />

<strong>the</strong> GreenlAnd marg<strong>in</strong> had retre<strong>at</strong>ed considerably<br />

dur<strong>in</strong>g MIS 5e. Of gre<strong>at</strong>est importance is<br />

th<strong>at</strong> retre<strong>at</strong> of <strong>the</strong> marg<strong>in</strong> northward past dYe-3<br />

implies th<strong>at</strong> <strong>the</strong> sou<strong>the</strong>rn dome of <strong>the</strong> ice sheet<br />

was nearly or completely gone.<br />

In this context it is useful to underst<strong>and</strong> <strong>the</strong><br />

genesis of <strong>the</strong> basal ice layer, <strong>and</strong> <strong>the</strong> layer <strong>at</strong><br />

dYe-3 <strong>in</strong> particular. Unfortun<strong>at</strong>ely <strong>the</strong> picture<br />

is cloudy—not unlike <strong>the</strong> basal ice itself, which<br />

has a small amount of silt <strong>and</strong> s<strong>and</strong> dispersed<br />

through it, mak<strong>in</strong>g it opaque. This silty basal<br />

layer is about 25 m thick (Souchez et al., 1998).<br />

Overly<strong>in</strong>g it is “clean” (not notably silty) ice th<strong>at</strong><br />

appears to be typical of polar ice sheets. Its total<br />

gas content <strong>and</strong> gas composition <strong>in</strong>dic<strong>at</strong>e th<strong>at</strong><br />

<strong>the</strong> ice formed by normal densific<strong>at</strong>ion of firn<br />

<strong>in</strong> a cold, dry environment. The oxygen isotope<br />

composition of this clean ice is –30.5‰. The<br />

bottom 4 m of <strong>the</strong> silty ice is radically different;<br />

its oxygen isotope value is –23‰, <strong>and</strong> its gas<br />

composition <strong>in</strong>dic<strong>at</strong>es substantial alter<strong>at</strong>ion by<br />

w<strong>at</strong>er. The total gas content of this basal silty<br />

ice is about half th<strong>at</strong> of normal cold ice formed<br />

from solid-st<strong>at</strong>e transform<strong>at</strong>ion of firn, <strong>the</strong> carbon<br />

dioxide content is 100 times normal, <strong>and</strong><br />

<strong>the</strong> oxygen/nitrogen r<strong>at</strong>io is less than 20% th<strong>at</strong><br />

of normal cold ice. This basal silty layer may<br />

be superimposed ice (ice formed by refreez<strong>in</strong>g<br />

of meltw<strong>at</strong>er <strong>in</strong> snow on a glacier or ice sheet,<br />

as Koerner (1989) suggested for <strong>the</strong> entire silty<br />

layer), or it may be non-glacial snowpack, or it<br />

may be a remnant of segreg<strong>at</strong>ion ice <strong>in</strong> permafrost<br />

(permafrost commonly conta<strong>in</strong>s rel<strong>at</strong>ively<br />

“clean” although still impure lenses of ice, called<br />

segreg<strong>at</strong>ion ice).<br />

In any case, <strong>the</strong> upper 21 m of <strong>the</strong> silty ice may<br />

be expla<strong>in</strong>ed as a mixture of <strong>the</strong>se two end members<br />

(Souchez et al. 1998). As <strong>the</strong>y deform, ice<br />

sheets do mix ice layers by small-scale structural<br />

fold<strong>in</strong>g (e.g., Alley et al., 1995b), by <strong>in</strong>teractions<br />

between rock particles, by gra<strong>in</strong>-boundary diffusion,<br />

<strong>and</strong> possibly by o<strong>the</strong>r processes. Unfortun<strong>at</strong>ely,<br />

<strong>the</strong>re is no way to dist<strong>in</strong>guish rigorously<br />

how much this ice really is a mixture of <strong>the</strong>se<br />

end-member components <strong>and</strong> how much of it<br />

is warm-clim<strong>at</strong>e (presumably MIS 5e) normal<br />

ice-sheet ice. The difficulty is th<strong>at</strong> <strong>the</strong> bottom<br />

layer is not itself well mixed (its gas composition<br />

is highly variable), so a mix<strong>in</strong>g model for<br />

<strong>the</strong> middle layer uses an essentially arbitrary<br />

composition for one end member. Souchez et<br />

al., (1998) used <strong>the</strong> composition <strong>at</strong> <strong>the</strong> top of <strong>the</strong><br />

bottom layer for <strong>the</strong>ir mix<strong>in</strong>g calcul<strong>at</strong>ions, but it<br />

could just as well be argued th<strong>at</strong> <strong>the</strong> composition<br />

here is determ<strong>in</strong>ed by exchange with <strong>the</strong> overly<strong>in</strong>g<br />

layer <strong>and</strong> is not a fixed quantity.<br />

As discussed <strong>in</strong> section 5.3.2b, above, <strong>in</strong> a<br />

recent study, Willerslev et al. (2007) exam<strong>in</strong>ed<br />

biological molecules <strong>in</strong> <strong>the</strong> silty ice from

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