bosons fermions
... Their excess precipitates to the lowest level, which becomes macroscopically occupied, i.e., it holds a finite fraction of all atoms. This is the BE condensate. ...
... Their excess precipitates to the lowest level, which becomes macroscopically occupied, i.e., it holds a finite fraction of all atoms. This is the BE condensate. ...
SEMICLASSICAL AND LARGE QUANTUM NUMBER LIMITS
... Conversely, the anticlassical or extreme quantum limit is reached for the opposite conditions to those listed in (3), e.g. |F | → ∞ or E → 0 for d > 0. For positive degrees d, e.g. all sorts of homogeneous oscillators, the first line of (3) expresses the widely appreciated fact, that the semiclassic ...
... Conversely, the anticlassical or extreme quantum limit is reached for the opposite conditions to those listed in (3), e.g. |F | → ∞ or E → 0 for d > 0. For positive degrees d, e.g. all sorts of homogeneous oscillators, the first line of (3) expresses the widely appreciated fact, that the semiclassic ...
Quantum Mirror Symmetry for Borcea
... In general, the solutions to the Picard-Fuchs equations (that is, the periods) may be compiled into an optimal solution, a multivariate function of all parameters, known as the I − f unction of that family. This is the object of interest in quantum mirror symmetry. For one-parameter families, the Dw ...
... In general, the solutions to the Picard-Fuchs equations (that is, the periods) may be compiled into an optimal solution, a multivariate function of all parameters, known as the I − f unction of that family. This is the object of interest in quantum mirror symmetry. For one-parameter families, the Dw ...
