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024 | 7 | _ | |2 pmid |a pmid:18507415 |
024 | 7 | _ | |2 DOI |a 10.1021/la800728x |
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041 | _ | _ | |a eng |
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084 | _ | _ | |2 WoS |a Chemistry, Multidisciplinary |
084 | _ | _ | |2 WoS |a Chemistry, Physical |
084 | _ | _ | |2 WoS |a Materials Science, Multidisciplinary |
100 | 1 | _ | |a Gordan, O. D. |b 0 |0 P:(DE-HGF)0 |
245 | _ | _ | |a On Pattern Transfer in Replica Molding |
260 | _ | _ | |a Washington, DC |b ACS Publ. |c 2008 |
300 | _ | _ | |a 6636 - 6639 |
336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
336 | 7 | _ | |a Output Types/Journal article |2 DataCite |
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336 | 7 | _ | |a article |2 DRIVER |
440 | _ | 0 | |a Langmuir |x 0743-7463 |0 4081 |v 24 |
500 | _ | _ | |a Record converted from VDB: 12.11.2012 |
520 | _ | _ | |a Nano- and micromolding of elastic materials produces smoothed replicas of the mold structures. This limits the technique's resolution. Here we identified surface tension as the cause of smoothing and derived explicit equations for calculating molded feature shapes. The characteristic length scale for smoothing is given by the ratio of the interface tension to Young's modulus of the molded material. This approach offers the possibility to correct for the smoothing caused by surface tension during mold design. Moreover, it can be exploited to measure interface tension. |
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700 | 1 | _ | |a Persson, B. N. J. |b 1 |0 P:(DE-HGF)0 |
700 | 1 | _ | |a Cesa, C. M. |b 2 |u FZJ |0 P:(DE-Juel1)VDB57503 |
700 | 1 | _ | |a Mayer, D. |b 3 |u FZJ |0 P:(DE-Juel1)128707 |
700 | 1 | _ | |a Hoffmann, B. |b 4 |u FZJ |0 P:(DE-Juel1)VDB27696 |
700 | 1 | _ | |a Dieluweit, S. |b 5 |u FZJ |0 P:(DE-Juel1)VDB5493 |
700 | 1 | _ | |a Merkel, R. |b 6 |u FZJ |0 P:(DE-Juel1)128833 |
773 | _ | _ | |a 10.1021/la800728x |g Vol. 24, p. 6636 - 6639 |p 6636 - 6639 |q 24<6636 - 6639 |0 PERI:(DE-600)2005937-1 |t Langmuir |v 24 |y 2008 |x 0743-7463 |
856 | 7 | _ | |u http://dx.doi.org/10.1021/la800728x |
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914 | 1 | _ | |y 2008 |
915 | _ | _ | |0 StatID:(DE-HGF)0010 |a JCR/ISI refereed |
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