Liquid 4He on Cs : drying, depinning, and the non-wetting thin-film

dc.contributor.authorReinelt, Dietmardeu
dc.contributor.authorIov, Valentindeu
dc.contributor.authorLeiderer, Paul
dc.contributor.authorKlier, Jürgendeu
dc.date.accessioned2011-03-24T14:53:40Zdeu
dc.date.available2011-03-24T14:53:40Zdeu
dc.date.issued2005deu
dc.description.abstractLiquid 4He shows a dewetting phase on Cs and Rb at low temperatures. These are the only substrates which are not wetted by 4He. On Cs the wetting temperature, Tw, is about 2 K. Usually one observes a thick metastable helium film remaining on the Cs substrate when either the surface is cooled below Tw (so starting from a wet film) or when bulk helium (in the form of a drop or an advancing film) is deposited on the Cs. The contact line of this film is generally very stable and so there is no dewetting. However, we have observed that spontaneous drying of helium on Cs can occur and that contact lines can recede for temperatures close to Tw. This exceptional behaviour is analysed and the dependence of substrate roughness is discussed. Furthermore, we have studied the non-wetting thin-film of liquid 4He on Cs. Far away from coexistence this film grows as a two-dimensional (2D) gas until about one monolayer is obtained, then remains nearly constant for a certain range of chemical potential and, close to coexistence, rapidly forms a thicker 2D-liquid-like film as stable thermodynamical solution.eng
dc.description.versionpublished
dc.format.mimetypeapplication/pdfdeu
dc.identifier.citationFirst publ. in: Journal of physics / Condensed Matter, 17 (2005), 9, pp. S403-S414deu
dc.identifier.doi10.1088/0953-8984/17/9/008
dc.identifier.ppn264519035deu
dc.identifier.urihttp://kops.uni-konstanz.de/handle/123456789/5164
dc.language.isoengdeu
dc.legacy.dateIssued2007deu
dc.rightsAttribution-NonCommercial-NoDerivs 2.0 Generic
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/2.0/
dc.subject.ddc530deu
dc.titleLiquid 4He on Cs : drying, depinning, and the non-wetting thin-filmeng
dc.typeJOURNAL_ARTICLEdeu
dspace.entity.typePublication
kops.citation.bibtex
@article{Reinelt2005Liqui-5164,
  year={2005},
  doi={10.1088/0953-8984/17/9/008},
  title={Liquid 4He on Cs : drying, depinning, and the non-wetting  thin-film},
  number={9},
  volume={17},
  journal={Journal of physics / Condensed Matter},
  pages={S403--S414},
  author={Reinelt, Dietmar and Iov, Valentin and Leiderer, Paul and Klier, Jürgen}
}
kops.citation.iso690REINELT, Dietmar, Valentin IOV, Paul LEIDERER, Jürgen KLIER, 2005. Liquid 4He on Cs : drying, depinning, and the non-wetting thin-film. In: Journal of physics / Condensed Matter. 2005, 17(9), pp. S403-S414. Available under: doi: 10.1088/0953-8984/17/9/008deu
kops.citation.iso690REINELT, Dietmar, Valentin IOV, Paul LEIDERER, Jürgen KLIER, 2005. Liquid 4He on Cs : drying, depinning, and the non-wetting thin-film. In: Journal of physics / Condensed Matter. 2005, 17(9), pp. S403-S414. Available under: doi: 10.1088/0953-8984/17/9/008eng
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    <dcterms:abstract xml:lang="eng">Liquid 4He shows a dewetting phase on Cs and Rb at low temperatures. These are the only substrates which are not wetted by 4He. On Cs the wetting temperature, Tw, is about 2 K. Usually one observes a thick metastable helium film remaining on the Cs substrate when either the surface is cooled below Tw (so starting from a wet film) or when bulk helium (in the form of a drop or an advancing film) is deposited on the Cs. The contact line of this film is generally very stable and so there is no dewetting. However, we have observed that spontaneous drying of helium on Cs can occur and that contact lines can recede for temperatures close to Tw. This exceptional behaviour is analysed and the dependence of substrate roughness is discussed. Furthermore, we have studied the non-wetting  thin-film  of liquid 4He on Cs. Far away from coexistence this film grows as a two-dimensional (2D) gas until about one monolayer is obtained, then remains nearly constant for a certain range of chemical potential and, close to coexistence, rapidly forms a thicker 2D-liquid-like film as stable thermodynamical solution.</dcterms:abstract>
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kops.sourcefieldJournal of physics / Condensed Matter. 2005, <b>17</b>(9), pp. S403-S414. Available under: doi: 10.1088/0953-8984/17/9/008deu
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kops.sourcefield.plainJournal of physics / Condensed Matter. 2005, 17(9), pp. S403-S414. Available under: doi: 10.1088/0953-8984/17/9/008eng
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