2024
DOI: 10.1016/j.cossms.2024.101159
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Nanocrystal programmable assembly beyond hard spheres (or shapes) and other (simple) potentials

Alex Travesset
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“…The excellent agreement between simulation and MOLT-CF reported in Figure c provides evidence that the large (∼500 k B T ) cohesive free energies correspond to actual thermodynamic equilibrium. This is because segment–segment interactions are a fraction of k B T , so bonds among CH 2 and CH 3 break and reform many times over simulation time (see refs , for a more detailed discussion). Moreover, the very large cohesive energy does not hinder structural transitions, such as the bcc-fcc Bain transformation, , because the free-energy barrier between phases is also of the order of k B T …”
Section: Structure Of Solvent-swollen Npslsmentioning
confidence: 99%
“…The excellent agreement between simulation and MOLT-CF reported in Figure c provides evidence that the large (∼500 k B T ) cohesive free energies correspond to actual thermodynamic equilibrium. This is because segment–segment interactions are a fraction of k B T , so bonds among CH 2 and CH 3 break and reform many times over simulation time (see refs , for a more detailed discussion). Moreover, the very large cohesive energy does not hinder structural transitions, such as the bcc-fcc Bain transformation, , because the free-energy barrier between phases is also of the order of k B T …”
Section: Structure Of Solvent-swollen Npslsmentioning
confidence: 99%