2022
DOI: 10.1103/physrevlett.128.045501
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Density Depletion and Enhanced Fluctuations in Water near Hydrophobic Solutes: Identifying the Underlying Physics

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Cited by 24 publications
(18 citation statements)
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“…As a perspective, recent theoretical studies proposed that more complex behaviors could arise when increasing the solute size: Hande et al [49] . proposed that the length‐scale cross‐over predicted by the LCW theory does not take place for large alcohols, while Coe et al [50] . showed that vapor bubbles formed at the interface between water and extended hydrophobic surfaces have a prominent effect on hydration free energies.…”
Section: Figurementioning
confidence: 99%
“…As a perspective, recent theoretical studies proposed that more complex behaviors could arise when increasing the solute size: Hande et al [49] . proposed that the length‐scale cross‐over predicted by the LCW theory does not take place for large alcohols, while Coe et al [50] . showed that vapor bubbles formed at the interface between water and extended hydrophobic surfaces have a prominent effect on hydration free energies.…”
Section: Figurementioning
confidence: 99%
“…So far, this assumption could not be directly tested experimentally, and our approach makes it possible to do so, as we have shown here for small alcohols. As a perspective, recent theoretical studies proposed that more complex behaviors could arise when increasing the solute size: Hande et al [49] proposed that the length-scale cross-over predicted by the LCW theory does not take place for large alcohols, while Coe et al [50] showed that vapor bubbles formed at the interface between water and extended hydrophobic surfaces have a prominent effect on hydration free energies. These new findings call for further refinement of our theoretical understanding, and THz calorimetry will be a valuable tool to confirm and possibly improve these models.…”
mentioning
confidence: 99%
“…( 5) turns into − κ 2 ∫ drρ(r)rr, where the integral is the matrix of second spatial moments of the density profile. The alternative form − κ 2 〈∑ i r i r i 〉 is obtained upon expressing the density profile as the average of ρðrÞ and carrying out the integral over r. Collecting all terms and dividing by κ 2 we obtain the sum rule (5) for the case of an interacting system inside of a harmonic trap as: R drdr 0 ρðrÞρðr 0 Þhðr; r 0 Þrr 0 ¼ R drρðrÞðk B Tκ À1 1 À rrÞ.…”
Section: Resultsmentioning
confidence: 99%
“…However, much of modern condensed matter physics is focused on seemingly entirely different physical behavior, namely that of fluctuating, disordered, spatially random, yet strongly interacting systems that possess a large number of degrees of freedom. Recent examples include active particles that display freezing 3 and wetting 4 , hydrophobicity rationalized as critical drying 5 , the structure of two-dimensional colloidal liquids 6 and that of fluid interfaces 7,8 .…”
mentioning
confidence: 99%