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Shear viscosity of a highly excited string and black hole membrane paradigm

Shear viscosity of a highly excited string and black hole membrane paradigm

Shear viscosity of a highly excited string and black hole membrane paradigm. Yuya Sasai Helsinki Institute of Physics and Department of Physics University of Helsinki in collaboration with A. Zahabi. Based on arXiv:1010.5380 Accepted by PRD. RIKEN symposium 2010 18 December 2010.

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419 views • 28 slides
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249 views • 17 slides
Chen, Yeng -Long

Chen, Yeng -Long

Polymer Physics and Flow - Theory. Chen, Yeng -Long. DNA / Polymer physics in n anoslits and nanochannels . Macromolecules, 2010, 2011, 2012. I = 35 mM. 20nm. 65nm. 110n m. 192n m. 465n m. 2 m m. Linear. Circular. h =104 nm. 4 mM. 7.5 mM. 15 mM. 30 mM. 250 mM. Linear.

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182 views • 3 slides
REU: Site for Polymer Science and Engineering Gustavo Carri , University of Akron, DMR 1004747

REU: Site for Polymer Science and Engineering Gustavo Carri , University of Akron, DMR 1004747

REU: Site for Polymer Science and Engineering Gustavo Carri , University of Akron, DMR 1004747.

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158 views • 2 slides
Education: Two graduate students Venkat Panchagnula (Chemistry Department)

Education: Two graduate students Venkat Panchagnula (Chemistry Department)

Theory and Computer Simulations of Polyelectrolyte-Polyampholyte Complexes Andrey Dobrynin, University of Connecticut, DMR-0305203.

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171 views • 2 slides
cool to recover former density

cool to recover former density

Why do some thin polymer films melt so far below the bulk ? Jane E.G. Lipson, Dartmouth College, DMR 1104658. Bulk sample in the melt has a characteristic density at T. Bulk polymer goes from melt to glass at the glass transition temperature, T g . Changing to a thin film

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141 views • 2 slides

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