2007
DOI: 10.1103/physrevlett.98.138102
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Proton Momentum Distribution in a Protein Hydration Shell

Abstract: The momentum distribution of protons in the hydration shell of a globular protein has been measured through deep inelastic neutron scattering at 180 and 290 K, below and above the crossover temperature T c 1:23T g , where T g 219 K is the glass transition temperature. It is found that the mean kinetic energy of the water hydrogens shows no temperature dependence, but the measurements are accurate enough to indicate a sensible change of momentum distribution and effective potential felt by protons, compatible w… Show more

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Cited by 49 publications
(56 citation statements)
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“…As anticipated, the 4p 2 np measured in two supercooled states shows a low-momentum narrowing along with a shoulder at about p 17 A ÿ1 , while no such feature is visible for the two stable phases. It has been shown that secondary peaks in the radial momentum distribution indicate quantum delocalization, or coherent interference of the proton over the two sites of a doublewell potential [15,26,27]. In other words, assuming that each water proton is shared by a covalent bound oxygen and a H-bonded one, the proton will be coherent over two separated sites along the H-bond direction.…”
Section: =2mentioning
confidence: 99%
“…As anticipated, the 4p 2 np measured in two supercooled states shows a low-momentum narrowing along with a shoulder at about p 17 A ÿ1 , while no such feature is visible for the two stable phases. It has been shown that secondary peaks in the radial momentum distribution indicate quantum delocalization, or coherent interference of the proton over the two sites of a doublewell potential [15,26,27]. In other words, assuming that each water proton is shared by a covalent bound oxygen and a H-bonded one, the proton will be coherent over two separated sites along the H-bond direction.…”
Section: =2mentioning
confidence: 99%
“…In recent years, several DINS experiments have addressed the study of bulk water in stable liquid, 7 solid, 8 and supercooled liquid 13,14 phases and in confined geometry. [15][16][17][18] In parallel, novel simulation techniques have been employed to calculate the n(p) using open path integral simulations 19 implemented with first principles molecular dynamics 20 within the path integral Car-Parrinello molecular dynamics (PICPMD) framework. 21 The path integral simulation has access to the three dimensional n( p), and thus provides complementary information to the spherically averaged n(p) obtained via DINS a) Author to whom correspondence should be addressed.…”
Section: Introductionmentioning
confidence: 99%
“…In as much as 20Å is the characteristic distance between elements of biological cells, the energetics of the interactions between these elements, and hence some of the properties of water that make life possible, are determined by this state, not the molecular state. It has already been demonstrated that changes in the zero-point motion of the protons can produce binding of water molecules to dry dna 22 , and that the protons in a partial layer of water on the surface of lysozyme has a delocalized momentum distribution similar to those described here [23][24] . Simulations based on empirical potential models of water cannot be expected to give these properties correctly.…”
mentioning
confidence: 76%