000000689 001__ 689
000000689 005__ 20240610115326.0
000000689 0247_ $$2DOI$$a10.1021/la0013805
000000689 0247_ $$2WOS$$aWOS:000167762700007
000000689 0247_ $$2Handle$$a2128/1465
000000689 037__ $$aPreJuSER-689
000000689 041__ $$aeng
000000689 082__ $$a670
000000689 084__ $$2WoS$$aChemistry, Multidisciplinary
000000689 084__ $$2WoS$$aChemistry, Physical
000000689 084__ $$2WoS$$aMaterials Science, Multidisciplinary
000000689 1001_ $$0P:(DE-HGF)0$$aSchwarz, U. S.$$b0
000000689 245__ $$aBending frustration of lipid-water mesophases based on cubic minimal surfaces
000000689 260__ $$aWashington, DC$$bACS Publ.$$c2001
000000689 300__ $$a2084 - 2096
000000689 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article
000000689 3367_ $$2DataCite$$aOutput Types/Journal article
000000689 3367_ $$00$$2EndNote$$aJournal Article
000000689 3367_ $$2BibTeX$$aARTICLE
000000689 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000000689 3367_ $$2DRIVER$$aarticle
000000689 440_0 $$04081$$aLangmuir$$v17$$x0743-7463$$y7
000000689 500__ $$aRecord converted from VDB: 12.11.2012
000000689 520__ $$aInverse bicontinuous cubic phases are ubiquitous in lipid-water mixtures and consist of a lipid bilayer forming a cubic minimal surface, thereby dividing space into two cubic networks of water channels. For small hydrocarbon chain lengths, the monolayers can be modeled as parallel surfaces to a minimal midsurface. The bending energy of the cubic phases is determined by the distribution of Gaussian curvature over the minimal midsurfaces which we calculate for seven different structures (G, D, P, I-WP, C(P), S, and F-RD). We show that the free-energy densities of the structures G, D, and P are considerably lower than those of the other investigated structures due to their narrow distribution of Gaussian curvature. The Bonnet transformation between G, D, and P implies that these phases coexist along a triple line, which also includes an excess water phase. Our model includes thermal membrane undulations. Our qualitative predictions remain unchanged when higher order terms in the curvature energy are included. Calculated phase diagrams agree well with the experimental results for 2:1 lauric acid/dilauroyl phosphatidylcholine and water.
000000689 536__ $$0G:(DE-Juel1)FUEK53$$2G:(DE-HGF)$$aPolymere, Membranen und komplexe Flüssigkeiten$$c23.30.0$$x0
000000689 588__ $$aDataset connected to Web of Science
000000689 650_7 $$2WoSType$$aJ
000000689 7001_ $$0P:(DE-Juel1)130665$$aGompper, G.$$b1$$uFZJ
000000689 773__ $$0PERI:(DE-600)2005937-1$$a10.1021/la0013805$$gVol. 17, p. 2084 - 2096$$p2084 - 2096$$q17<2084 - 2096$$tLangmuir$$v17$$x0743-7463$$y2001
000000689 8564_ $$uhttps://juser.fz-juelich.de/record/689/files/111.pdf$$yOpenAccess
000000689 8564_ $$uhttps://juser.fz-juelich.de/record/689/files/111.jpg?subformat=icon-1440$$xicon-1440$$yOpenAccess
000000689 8564_ $$uhttps://juser.fz-juelich.de/record/689/files/111.jpg?subformat=icon-180$$xicon-180$$yOpenAccess
000000689 8564_ $$uhttps://juser.fz-juelich.de/record/689/files/111.jpg?subformat=icon-640$$xicon-640$$yOpenAccess
000000689 909CO $$ooai:juser.fz-juelich.de:689$$pdnbdelivery$$pVDB$$pdriver$$popen_access$$popenaire
000000689 9131_ $$0G:(DE-Juel1)FUEK53$$bStruktur der Materie und Materialforschung$$k23.30.0$$lFestkörperforschung$$vPolymere, Membranen und komplexe Flüssigkeiten$$x0
000000689 9141_ $$y2001
000000689 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed
000000689 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000000689 9201_ $$0I:(DE-Juel1)VDB31$$d31.12.2006$$gIFF$$kIFF-TH-II$$lTheorie II$$x0
000000689 970__ $$aVDB:(DE-Juel1)111
000000689 9801_ $$aFullTexts
000000689 980__ $$aVDB
000000689 980__ $$aJUWEL
000000689 980__ $$aConvertedRecord
000000689 980__ $$ajournal
000000689 980__ $$aI:(DE-Juel1)ICS-2-20110106
000000689 980__ $$aUNRESTRICTED
000000689 980__ $$aFullTexts
000000689 981__ $$aI:(DE-Juel1)IBI-5-20200312
000000689 981__ $$aI:(DE-Juel1)IAS-2-20090406
000000689 981__ $$aI:(DE-Juel1)ICS-2-20110106