2016
DOI: 10.1038/ngeo2848
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Global atmospheric teleconnections during Dansgaard–Oeschger events

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Cited by 127 publications
(173 citation statements)
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“…(4) Yet interlab reproducibility (INSTAAR CRDS-CFA vs. UW CRDS) of down-sampled dxs has a low R 2 value of 0.29, but still within the same range of values between ∼ 1 and 4 ‰. These results suggest that the inherent noise in dxs measurements may make this parameter most useful at timescales of centuries to millennia when the range of WDC dxs increases to ∼ 0 to 12 ‰ (Markle et al, 2017).…”
Section: Wais Divide Ice Core Testsmentioning
confidence: 76%
“…(4) Yet interlab reproducibility (INSTAAR CRDS-CFA vs. UW CRDS) of down-sampled dxs has a low R 2 value of 0.29, but still within the same range of values between ∼ 1 and 4 ‰. These results suggest that the inherent noise in dxs measurements may make this parameter most useful at timescales of centuries to millennia when the range of WDC dxs increases to ∼ 0 to 12 ‰ (Markle et al, 2017).…”
Section: Wais Divide Ice Core Testsmentioning
confidence: 76%
“…This could be explained by an important contribution of sublimated moisture with kinetic fractionation. Additionally, the significant negative correlation between d ln and δ 18 O in summer precipitation on the East Antarctic Plateau (Figure c) should indicate the effect of kinetic fractionation during sublimation because the influences of equilibrium fractionation and kinetic fractionation during snow formation on deuterium excess are eliminated by the logarithmic definition (Markle et al, ; Schoenemann et al, ; Schoenemann & Steig, ; Uemura et al, ). When the δ 18 O is lower (corresponding to lower temperature and RH), stronger kinetic fractionation during sublimation is expected, and vice versa.…”
Section: Discussionmentioning
confidence: 99%
“…The second‐order parameters of δD, δ 18 O, and δ 17 O, d‐excess and 17 O‐excess, defined as d‐excess = δD − 8 × δ 18 O (Dansgaard, ) and 17 O‐excess = ln(δ 17 O + 1) − 0.528 × ln(δ 18 O + 1) (Barkan & Luz, ; Landais et al, ; Luz & Barkan, ), can preserve a climatic signal from the moisture source region (Angert et al, ; Johnsen et al, ; Jouzel et al, ; Jouzel et al, ; Landais et al, ; Masson‐Delmotte et al, ; Markle et al, ; Merlivat & Jouzel, ; Uemura et al, ; Vimeux et al, , ), imprinted by kinetic fractionation of water stable isotopes during evaporation. The d‐excess is mainly controlled by the sea surface temperature (SST) and/or relative humidity (RH) at the moisture source region (Merlivat & Jouzel, ; Steen‐Larsen, Sveinbjörnsdottir, et al, ; Uemura et al, ), though the effect of SST has been questioned by direct observations of water stable isotopes in water vapor in the marine boundary layer (Steen‐Larsen et al, , ).…”
Section: Introductionmentioning
confidence: 99%
“…420 000 years at Vostok (Petit et al, 1999), 720 000 years at Dome F (Kawamura et al, 2017) and 800 000 years at Dome C (EPICA, 2004(EPICA, , 2006. Even though reconstructions from ice cores from Greenland and West Antarctica do not extend as far back as from East Antarctica, high resolution analyses of these cores provide very fine temporal resolution from which the seasonal cycle can be resolved (Vinther et al,10 2010; Markle et al, 2017). Seasonal variations are also imprinted in the snow isotopic composition of high accumulation sites in coastal areas of Antarctica (Morgan, 1985;Masson-Delmotte et al, 2003;Küttel et al, 2012).…”
Section: Introductionmentioning
confidence: 99%