Presents an optimal transport framework for simulating particle systems with arbitrary cell shapes and volumes that automatically handles exclusion constraints.
Klimczuk , author P
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La substitution in Nd1-xLaxNiC2 suppresses the CDW at xc=0.38 while AFM persists, then AFM softens and superconductivity appears once AFM reaches zero temperature, consistent with a possible quantum critical point.
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Multicellular simulations with shape and volume constraints using optimal transport
Presents an optimal transport framework for simulating particle systems with arbitrary cell shapes and volumes that automatically handles exclusion constraints.
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Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd$_{1-x}$La$_x$NiC$_2$ compounds
La substitution in Nd1-xLaxNiC2 suppresses the CDW at xc=0.38 while AFM persists, then AFM softens and superconductivity appears once AFM reaches zero temperature, consistent with a possible quantum critical point.