Atomic matter of nonzero-momentum Bose-Einstein condensation and orbital current order
... Confining bosonic atoms in an optical lattice can bring out different and new physics beyond the standard BoseEinstein condensation 共BEC兲 observed in a single trap 关1,2兴. The superfluid–Mott-insulator experiment on an optical lattice 关3兴, based on an early theoretical idea 关4,5兴, demonstrated one su ...
... Confining bosonic atoms in an optical lattice can bring out different and new physics beyond the standard BoseEinstein condensation 共BEC兲 observed in a single trap 关1,2兴. The superfluid–Mott-insulator experiment on an optical lattice 关3兴, based on an early theoretical idea 关4,5兴, demonstrated one su ...
Section_36_Turbulenc..
... The function P(V ) is called the probability distribution function, or PDF. According the Central Limit Theorem, for random fluctuations the PDF is Gaussian. If the PDF, and V , are independent of position the turbulence is said to be homogeneous. If the PDF is independent of arbitrary rotations of ...
... The function P(V ) is called the probability distribution function, or PDF. According the Central Limit Theorem, for random fluctuations the PDF is Gaussian. If the PDF, and V , are independent of position the turbulence is said to be homogeneous. If the PDF is independent of arbitrary rotations of ...
Chapter 13 Ideal Fermi gas
... We define the Fermi temperature TF as εF = kB T F . For low temperatures T << TF , the Fermi distribution deviates from that at T = 0 mainly in the neighborhood of εF in a layer of thickness kB T , i.e., particles at energies of order kB T below the Fermi energy are excited to energies of order kB T ...
... We define the Fermi temperature TF as εF = kB T F . For low temperatures T << TF , the Fermi distribution deviates from that at T = 0 mainly in the neighborhood of εF in a layer of thickness kB T , i.e., particles at energies of order kB T below the Fermi energy are excited to energies of order kB T ...
