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Bose Gas


A Bose gas is a many-particle quantum model whose state vectors are symmetric under permutations of particles. For N particles on a three-dimensional torus of side L, a standard Hamiltonian in units with kinetic coefficient one is

 H_(N,L)=sum_(i=1)^N(-Delta_i)+sum_(i<j)v_L(x_i-x_j),

where v_L is the periodic pair potential. The density is rho=N/L^3. A hard-sphere gas instead excludes configurations with pair distance at most a>0 and uses the kinetic quadratic form with zero boundary values on the excluded region. For hard spheres this exclusion distance is also the scattering length.

For a general many-particle density operator Gamma of trace one, the one-particle operator is gamma^((1))=NTr_(2,...,N)Gamma and has trace N. Its constant-orbital fraction is B=N^(-1)<u_0,gamma^((1))u_0>, with u_0=L^(-3/2). For a ground state whose condensate occupies this orbital, B is the condensate fraction and 1-B is the quantum depletion fraction.


See also

Bose-Einstein Condensation, Fock Space, Quantum Depletion, Scattering Length

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References

Lieb, E. H.; Seiringer, R.; Solovej, J. P.; and Yngvason, J. The Mathematics of the Bose Gas and Its Condensation. Basel, Switzerland: Birkhäuser, 2005. https://doi.org/10.1007/b137508.

Cite this as:

Weisstein, Eric W. "Bose Gas." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/BoseGas.html

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