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DNA Nanotweezers Studied with a Coarse-Grained Model of DNA ...
https://www-wales.ch.cam.ac.uk/Telluride.papers/prl10.pdf14 Jan 2011: 30 APRIL 2010. 178101-2. eight bases provide a ‘‘toehold’’ for binding of the antifuelf, which is also 24 bases long and complementary to thewhole of f. ... 60. 0,0 0,8 0,16 8,16 16,8 24,0. Free. Ene. rgy. / kT. -
Rational design of helical architecturesDwaipayan Chakrabarti,…
https://www-wales.ch.cam.ac.uk/Telluride.papers/PNAS.106.20164.2009.pdf4 Jan 2011: geometry. TheBLmGBD potential makes use of the orientation-dependentmolecular shape parameter and the energy parameter tomodel the interaction between two uniaxial oblate ellipsoids(24), each having a single-site representation. ... J Chem Phys 74:3316 -
This article appeared in a journal published by Elsevier. ...
https://www-wales.ch.cam.ac.uk/Telluride.papers/COSB.20.3.2010.pdf4 Jan 2011: aðq jÞ@q j;g. q j0. 1. 2pn j;g. 24. 35. 2. ... Annu Rev PhysChem 1997, 48:545-600. 24. Miller MA, Wales DJ: Energy landscape of a model protein.J Chem Phys 1999, 111:6610-6616. -
How many dimensions are required to approximate the potential ...
https://www-wales.ch.cam.ac.uk/Telluride.papers/rlj_05_1.pdf13 Jan 2011: Chem. Phys. 122, 084714 2005! Downloaded 24 Mar 2005 to 147.188.105.99. ... J. Chem. Phys. 122, 084714 2005! Downloaded 24 Mar 2005 to 147.188.105.99. -
DOI : 10.1002/cphc.201000233 Energy Landscapes of Clusters Bound by…
https://www-wales.ch.cam.ac.uk/Telluride.papers/CPC.11.2491.2010.pdf4 Jan 2011: 0892 0.04568 18.0000320936 4 0.0448 0.02298 18.0000240710 12 0.0145 0.00748 18.0000240710 4 0.0426 0.02188 18.0000000700 24 0.0140 0.00718 ... C. A. M. Mooij, D. Frenkel, H. N. W. Lekker-. kerker, Nature 1993, 365, 425.[24] A. -
Topographical complexity of multidimensional energy landscapes Tamiki …
https://www-wales.ch.cam.ac.uk/Telluride.papers/rlj_06_5.pdf13 Jan 2011: Our landscape and path complexity. measures are quite general, irrespective of the kinds of energy[i.e., potential or free energy (9, 24)] and model. ... Wales DJ, Dewsbury PEJ (2004) J Chem Phys 121:10284.24. Evans DA, Wales DJ (2003) J Chem Phys -
Unbekannt
https://www-wales.ch.cam.ac.uk/Telluride.papers/rlj_04_8.pdf13 Jan 2011: Name Length E Sequence. HP-20 20 )9 HPHP2H2PHP2HPH2P2HPHHP-24 24 )9 H2P2ðHP2Þ6H2HP-25 25 )8 P2HP2ðH2P4Þ3H2HP-36 36 )14 P3H2P2H2P5H7P2H2P4H2P2HP2HP-48 48 )23 P2HðP2H2Þ2P5H10P6ðH2P2Þ2HP2H5HP-50 50 )21 H2ðPHÞ3PH4PðHP3Þ3PðHP3Þ2HPH4ðPHÞ4H. -
No Job Name
https://www-wales.ch.cam.ac.uk/Telluride.papers/rlj_06_4.pdf13 Jan 2011: This model isclosely related to the “void model” for structural changes andmelting of clusters.24. ... A.; Wales, D. J.J. Chem. Phys.2004, 121, 6689.(24) Berry, R. S.; Smirnov, B. -
Reversible self-assembly of patchy particles into…
https://www-wales.ch.cam.ac.uk/Telluride.papers/jcp07b.pdf14 Jan 2011: Since high temperatures are equivalent to weakbonding interactions, this finding is consistent with the ex-perimental observation that protein-protein interactions in vi-rus capsids are generally weak.24. ... M. Teschke, J. Mol. Biol. 365,513 2007. 24 A. -
Emergent Complexity from SimpleAnisotropic Building Blocks:…
https://www-wales.ch.cam.ac.uk/Telluride.papers/ACSnano.4.219.2010.pdf4 Jan 2011: Address correspondence todw34@cam.ac.uk. Received for review October 4, 2009and accepted December 24, 2009. ... 24. Wales, D. J. Discrete Path Sampling. Mol. Phys. 2002, 100,3285–3306.
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