Optical properties of deep glacial ice at the South Pole

M. Ackermann(Deutsches Elektronen-Synchrotron DESY), J. Ahrens(Johannes Gutenberg University Mainz), X. Bai(University of Delaware), M. Bartelt(TU Dortmund University), S. W. Barwick(University of California, Irvine), Ryan Bay(University of California, Berkeley), T. Becka(Johannes Gutenberg University Mainz), J. K. Becker(TU Dortmund University), Klaus Becker(University of Wuppertal), P. Berghaus(Université Libre de Bruxelles), E. Bernardini(Deutsches Elektronen-Synchrotron DESY), Daniel Bertrand(Université Libre de Bruxelles), D. J. Boersma(University of Wisconsin–Madison), S. Böser(Deutsches Elektronen-Synchrotron DESY), O. Botner(Uppsala University), A. Bouchta(Uppsala University), O. Bouhali(Université Libre de Bruxelles), C. P. Burgess(Stockholm University), T. Burgess(Stockholm University), T. Castermans(University of Mons), D. Chirkin(Lawrence Berkeley National Laboratory), Bertrand Collin(Pennsylvania State University), J. M. Conrad(Uppsala University), J. Cooley(University of Wisconsin–Madison), D. F. Cowen(Pennsylvania State University), Anna Davour(Uppsala University), C. De Clercq(Vrije Universiteit Brussel), C. Pérez de los Heros(Uppsala University), P. Desiati(University of Wisconsin–Madison), T. DeYoung(Pennsylvania State University), P. Ekström(Stockholm University), T. Feser(Johannes Gutenberg University Mainz), T. K. Gaisser(University of Delaware), R. Ganugapati(University of Wisconsin–Madison), H. Geenen(University of Wuppertal), L. Gerhardt(University of California, Irvine), A. Goldschmidt(Lawrence Berkeley National Laboratory), A. Groß(TU Dortmund University), A. Hallgren(Uppsala University), F. Halzen(University of Wisconsin–Madison), K. Hanson(University of Wisconsin–Madison), D. Hardtke(University of California, Berkeley), T. Harenberg(University of Wuppertal), T. Hauschildt(University of Delaware), K. Helbing(Lawrence Berkeley National Laboratory), M. Hellwig(Johannes Gutenberg University Mainz), P. Herquet(University of Mons), G. C. Hill(University of Wisconsin–Madison), J. Hodges(University of Wisconsin–Madison), Daan Hubert(Vrije Universiteit Brussel), B. Hughey(University of Wisconsin–Madison), P. O. Hulth(Stockholm University), K. Hultqvist(Stockholm University), S. Hundertmark(Stockholm University), J. Jacobsen(Lawrence Berkeley National Laboratory), K.‐H. Kampert(University of Wuppertal), A. Karle(University of Wisconsin–Madison), M. Kestel(Pennsylvania State University), G. Kohnen(University of Mons), L. Köpke(Johannes Gutenberg University Mainz), M. Kowalski(Deutsches Elektronen-Synchrotron DESY), K. Kuehn(University of California, Irvine), R.M. Lang(Deutsches Elektronen-Synchrotron DESY), H. Leich(Deutsches Elektronen-Synchrotron DESY), M. Leuthold(Deutsches Elektronen-Synchrotron DESY), I. Liubarsky(Imperial College London), J. Lundberg(Uppsala University), J. Madsen(University of Wisconsin–River Falls), P. Marciniewski(Uppsala University), H. S. Matis(Lawrence Berkeley National Laboratory), C. McParland(Lawrence Berkeley National Laboratory), T. Messarius(TU Dortmund University), Y. Minaeva(Stockholm University), P. Miočinović(University of California, Berkeley), R. Morse(University of Wisconsin–Madison), K. Münich(TU Dortmund University), R. Nahnhauer(Deutsches Elektronen-Synchrotron DESY), J. W. Nam(University of California, Irvine), T. Neunhöffer(Johannes Gutenberg University Mainz), P. Nießen(University of Delaware), D. R. Nygren(Lawrence Berkeley National Laboratory), Ph. Olbrechts(Vrije Universiteit Brussel), A. C. Pohl(Uppsala University), R. Porrata(University of California, Berkeley), P. B. Price(University of California, Berkeley), G. T. Przybylski(Lawrence Berkeley National Laboratory), K. Rawlins(University of Wisconsin–Madison), E. Resconi(Deutsches Elektronen-Synchrotron DESY), W. Rhode(TU Dortmund University), M. Ribordy(University of Mons), S. Richter(University of Wisconsin–Madison), J. Rodrı́guez Martino(Stockholm University), H.‐G. Sander(Johannes Gutenberg University Mainz), S. Schlenstedt(Deutsches Elektronen-Synchrotron DESY), A. Schneider(University of Wisconsin–Madison), R. Schwarz(University of Wisconsin–Madison), A. Silvestri(University of California, Irvine), M. Solarz(University of California, Berkeley), G. M. Spiczak(University of Wisconsin–River Falls), Christian Spiering(Deutsches Elektronen-Synchrotron DESY), M. Stamatikos(University of Wisconsin–Madison), D. Steele(University of Wisconsin–Madison), P. Steffen(Deutsches Elektronen-Synchrotron DESY), R. G. Stokstad(Lawrence Berkeley National Laboratory), K.‐H. Sulanke(Deutsches Elektronen-Synchrotron DESY), I. Taboada(University of California, Berkeley), O. Tarasova(Deutsches Elektronen-Synchrotron DESY), L. Thollander(Stockholm University), S. Tilav(University of Delaware), Wolfgang Wagner(TU Dortmund University), C. Walck(Stockholm University), M. Walter(Deutsches Elektronen-Synchrotron DESY), Y.‐R. Wang(University of Wisconsin–Madison), C. H. Wiebusch(University of Wuppertal), R. Wischnewski(Deutsches Elektronen-Synchrotron DESY), H. Wissing(Deutsches Elektronen-Synchrotron DESY), K. Woschnagg(University of California, Berkeley)
Journal of Geophysical Research Atmospheres
July 8, 2006
Cited by 538Open Access
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Abstract

We have remotely mapped optical scattering and absorption in glacial ice at the South Pole for wavelengths between 313 and 560 nm and depths between 1100 and 2350 m. We used pulsed and continuous light sources embedded with the AMANDA neutrino telescope, an array of more than six hundred photomultiplier tubes buried deep in the ice. At depths greater than 1300 m, both the scattering coefficient and absorptivity follow vertical variations in concentration of dust impurities, which are seen in ice cores from other Antarctic sites and which track climatological changes. The scattering coefficient varies by a factor of seven, and absorptivity (for wavelengths less than ∼450 nm) varies by a factor of three in the depth range between 1300 and 2300 m, where four dust peaks due to stadials in the late Pleistocene have been identified. In our absorption data, we also identify a broad peak due to the Last Glacial Maximum around 1300 m. In the scattering data, this peak is partially masked by scattering on residual air bubbles, whose contribution dominates the scattering coefficient in shallower ice but vanishes at ∼1350 m where all bubbles have converted to nonscattering air hydrates. The wavelength dependence of scattering by dust is described by a power law with exponent −0.90 ± 0.03, independent of depth. The wavelength dependence of absorptivity in the studied wavelength range is described by the sum of two components: a power law due to absorption by dust, with exponent −1.08 ± 0.01 and a normalization proportional to dust concentration that varies with depth; and a rising exponential due to intrinsic ice absorption which dominates at wavelengths greater than ∼500 nm.


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