2002
DOI: 10.1088/0953-8984/14/8/106
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Spectroscopic probing of local hydrogen-bonding structures in liquid water

Abstract: We have studied the electronic structure of liquid water using x-ray absorption spectroscopy at the oxygen K edge. Since the x-ray absorption process takes less than a femtosecond, it allows probing of the molecular orbital structure of frozen, local geometries of water molecules at a timescale that has not previously been accessible. Our results indicate that the electronic structure of liquid water is significantly different from that of the solid and gaseous forms, resulting in a pronounced pre-edge feature… Show more

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Cited by 312 publications
(426 citation statements)
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“…For liquid water it was demonstrated by Wernet et al 1 that the investigated molecular dynamics simulations, including ab initio Car-Parrinello molecular dynamics (CPMD) 23 , all resulted in a preponderance of DD species with two donating H-bonds. XA spectra of DD molecules are characterized by the same features typical of the spectrum of bulk ice with weak pre-and mainedges and an intense and broad post-edge around 540 eV 1, 8,9,21 Fig. 1 (left) Experimental XA spectrum of gas phase water from ref.…”
mentioning
confidence: 88%
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“…For liquid water it was demonstrated by Wernet et al 1 that the investigated molecular dynamics simulations, including ab initio Car-Parrinello molecular dynamics (CPMD) 23 , all resulted in a preponderance of DD species with two donating H-bonds. XA spectra of DD molecules are characterized by the same features typical of the spectrum of bulk ice with weak pre-and mainedges and an intense and broad post-edge around 540 eV 1, 8,9,21 Fig. 1 (left) Experimental XA spectrum of gas phase water from ref.…”
mentioning
confidence: 88%
“…XAS (elsewhere also NEXAFS or XANES) 5 and the corresponding non-resonant x-ray Raman spectroscopy (XRS) 6 are well-established experimental techniques that have recently been extended to measurements of the local electronic structure of liquid water 1, [7][8][9][10][11] . Both XAS and XRS show major differences in the spectral profiles between bulk ice and liquid water 1,8,9 ; there is a well-defined pre-edge structure that can be seen in the spectrum of the liquid and is substantially reduced in the bulk ice spectrum; the remaining intensity is mainly due to proton disorder and minor defects 12 . The liquid water spectrum, with strong pre-edge (535 eV) and main-edge (537 eV) features, instead closely resembles that of the ice surface where a dominant fraction of the water molecules in the first half-bilayer has one free O-H bond 1, 13 .…”
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confidence: 99%
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“…As is well known, the acceptor spectrum bears a close resemblance to the monomer spectrum, whereas the donor spectrum is substantially affected by the formation of the hydrogen bond [141] ; the same feature is seen also in the case of alcohols. [142] The experimental XAS edge of water in the gas phase is roughly at 534 eV, [143] thus the XCH method (without corrections for functional dependence, etc.) underestimates the transition energy by some 5.5 eV.…”
Section: Core Electron Excitationsmentioning
confidence: 99%
“…[1][2][3][4][5][6][7][8] The exploration of structural and binding properties of water clusters may provide a route to understand bulk water in its liquid or solid phase. [1,9] Thus many studies have been presented on the structure of water clusters from small to large sizes both experimentally and theoretically. [10][11][12][13][14][15][16][17][18][19][20] For small clusters with up to ten water molecules, most computational ab initio investigations predict approximately the same geometries, which are consistent with experimental results.…”
Section: Introductionmentioning
confidence: 99%