Liquid nanostripes
Equilibrium wetting of ethanol, a volatile liquid, onto chemically patterned nanostripes has been investigated using noncontact atomic force microscopy (AFM). The chemical patterns, generated by a conducting AFM tip, are composed of COOH terminated "wetting" regions and CH3 terminated &quo...
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| Published in: | Physical review letters Vol. 96; no. 5; p. 056104 |
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| Format: | Journal Article |
| Language: | English |
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10-02-2006
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| Abstract | Equilibrium wetting of ethanol, a volatile liquid, onto chemically patterned nanostripes has been investigated using noncontact atomic force microscopy (AFM). The chemical patterns, generated by a conducting AFM tip, are composed of COOH terminated "wetting" regions and CH3 terminated "nonwetting" regions. Controlled amounts of ethanol, from the vapor phase, condense on the COOH stripes and their shape is imaged in situ versus their width (70 < w < 300 nm). The measured profile shapes at saturation and their w(1/2) height dependence are well described by density functional theory with dispersive, nonretarded potentials. |
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| AbstractList | Equilibrium wetting of ethanol, a volatile liquid, onto chemically patterned nanostripes has been investigated using noncontact atomic force microscopy (AFM). The chemical patterns, generated by a conducting AFM tip, are composed of COOH terminated "wetting" regions and CH3 terminated "nonwetting" regions. Controlled amounts of ethanol, from the vapor phase, condense on the COOH stripes and their shape is imaged in situ versus their width (70 < w < 300 nm). The measured profile shapes at saturation and their w(1/2) height dependence are well described by density functional theory with dispersive, nonretarded potentials. Equilibrium wetting of ethanol, a volatile liquid, onto chemically patterned nanostripes has been investigated using noncontact atomic force microscopy (AFM). The chemical patterns, generated by a conducting AFM tip, are composed of COOH terminated "wetting" regions and CH3 terminated "nonwetting" regions. Controlled amounts of ethanol, from the vapor phase, condense on the COOH stripes and their shape is imaged in situ versus their width (70 < w < 300 nm). The measured profile shapes at saturation and their w(1/2) height dependence are well described by density functional theory with dispersive, nonretarded potentials. |
| ArticleNumber | 056104 |
| Author | Checco, Antonio Ocko, Benjamin M Gang, Oleg |
| Author_xml | – sequence: 1 givenname: Antonio surname: Checco fullname: Checco, Antonio organization: Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA – sequence: 2 givenname: Oleg surname: Gang fullname: Gang, Oleg – sequence: 3 givenname: Benjamin M surname: Ocko fullname: Ocko, Benjamin M |
| BackLink | https://www.ncbi.nlm.nih.gov/pubmed/16486959$$D View this record in MEDLINE/PubMed |
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| CitedBy_id | crossref_primary_10_1088_0957_4484_24_50_505301 crossref_primary_10_1063_1_2955860 crossref_primary_10_1002_anie_200801013 crossref_primary_10_1039_C8CC02596G crossref_primary_10_1021_acsami_1c17139 crossref_primary_10_1021_la4019376 crossref_primary_10_1039_b608630f crossref_primary_10_1021_la702321d crossref_primary_10_1088_1751_8113_40_10_003 crossref_primary_10_1103_PhysRevLett_102_106103 crossref_primary_10_1103_PhysRevE_93_052805 crossref_primary_10_1103_PhysRevLett_104_106102 crossref_primary_10_1021_la204774s crossref_primary_10_1103_PhysRevLett_105_076103 crossref_primary_10_1103_PhysRevLett_107_135701 crossref_primary_10_1103_PhysRevE_83_016212 crossref_primary_10_1088_0143_0807_31_1_008 crossref_primary_10_1002_smll_200800819 crossref_primary_10_1021_la7017677 crossref_primary_10_1002_adem_201500486 crossref_primary_10_1021_la701921z crossref_primary_10_1039_b903813b crossref_primary_10_1142_S0217979207043476 crossref_primary_10_1146_annurev_matsci_38_060407_132451 crossref_primary_10_1016_j_cis_2015_07_004 crossref_primary_10_1021_la703106s crossref_primary_10_1002_ange_200801013 crossref_primary_10_1002_admi_201600478 crossref_primary_10_1103_PhysRevLett_109_166101 crossref_primary_10_1021_la7013754 crossref_primary_10_1007_s10909_007_9462_2 crossref_primary_10_1103_PhysRevE_94_030801 crossref_primary_10_1146_annurev_matsci_38_060407_130335 crossref_primary_10_1103_PhysRevE_77_061601 crossref_primary_10_1063_1_2178786 crossref_primary_10_1103_PhysRevE_74_031608 crossref_primary_10_1016_j_ultramic_2005_11_009 crossref_primary_10_1039_C4SM01152J crossref_primary_10_1039_c2sm25747e crossref_primary_10_1039_c3sm51188j crossref_primary_10_1021_la302854t crossref_primary_10_1088_0953_8984_26_22_225001 crossref_primary_10_1103_PhysRevE_90_042926 |
| Cites_doi | 10.1021/la001607w 10.1103/PhysRevLett.91.186101 10.1021/la960189l 10.1103/PhysRevB.41.1111 10.1006/jcis.1995.1121 10.1021/jp980149l 10.1103/RevModPhys.57.827 10.1103/PhysRevLett.80.1920 10.1103/PhysRevLett.66.2108 10.1103/PhysRevE.60.6919 10.1002/(SICI)1521-4095(199901)11:1<55::AID-ADMA55>3.0.CO;2-8 10.1103/PhysRevLett.85.1930 10.1021/la970948f 10.1103/PhysRevA.43.4344 10.1007/s100510050907 10.1002/adfm.200400534 10.1016/S0167-5729(02)00077-8 |
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| References | PhysRevLett.96.056104Cc5R1 PhysRevLett.96.056104Cc4R1 PhysRevLett.96.056104Cc3R1 J. N. Israelachvili (PhysRevLett.96.056104Cc15R1) 1992 P. G. de Gennes (PhysRevLett.96.056104Cc1R1) 2003 PhysRevLett.96.056104Cc2R1 PhysRevLett.96.056104Cc9R1 PhysRevLett.96.056104Cc10R1 PhysRevLett.96.056104Cc8R1 PhysRevLett.96.056104Cc20R1 PhysRevLett.96.056104Cc6R1 PhysRevLett.96.056104Cc14R1 PhysRevLett.96.056104Cc13R1 PhysRevLett.96.056104Cc12R1 PhysRevLett.96.056104Cc11R1 PhysRevLett.96.056104Cc18R1 PhysRevLett.96.056104Cc17R1 PhysRevLett.96.056104Cc16R1 PhysRevLett.96.056104Cc19R1 |
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