The numerical evaluation of coherent-state path-integral representations for partition functions and other quantities in equilibrium quantum statistical mechanics is discussed. Several coherent-state path-integral schemes are introduced, which differ from each other by the order of approximation and by the operator ordering employed in the high-temperature approximation of the density operator. Simple one-dimensional systems are used to test these schemes. For the harmonic oscillator, finite-dimensional approximations to the coherent-state path integral are calculated analytically and compared to each other and to the real-space path integral. For anharmonic systems, integrations must be approximated by quadrature formulas. This leads to a ...
The density matrix theory, the ancestor of density functional theory, provides the immediate framewo...
By returning to the underlying discrete time formalism, we relate spurious results in coherent state...
We consider a set of operators hat{x}=(hat{x}_1,..., hat{x}_N) with diagonal representatives P(n) in...
The numerical evaluation of coherent-state path integrals for quantum dynamical problems is discusse...
Coherent state path integral representations for matrix elements of density operators are compared t...
In this project two steps involved in the handling of path integrals are reexamined in detail for co...
The path-integral quantization of thermal scalar, vector and spinor fields is performed newly in the...
The authors examine several topical subjects, commencing with a general introduction to path integra...
The definition and formulas for the harmonic oscillator coherent states and spin coherent states are...
This thesis presents and develops the path integral simulation techniques in application to small qu...
We construct a representation of the coherent state path integral using the Weyl symbol of the Hamil...
The overcompleteness of the coherent states basis leads to a multiplicity of representations of Feyn...
This thesis presents and develops the path integral simulation techniques in application to small qu...
This thesis presents and develops the path integral simulation techniques in application to small qu...
The overcompleteness of the coherent states basis leads to a multiplicity of representations of Feyn...
The density matrix theory, the ancestor of density functional theory, provides the immediate framewo...
By returning to the underlying discrete time formalism, we relate spurious results in coherent state...
We consider a set of operators hat{x}=(hat{x}_1,..., hat{x}_N) with diagonal representatives P(n) in...
The numerical evaluation of coherent-state path integrals for quantum dynamical problems is discusse...
Coherent state path integral representations for matrix elements of density operators are compared t...
In this project two steps involved in the handling of path integrals are reexamined in detail for co...
The path-integral quantization of thermal scalar, vector and spinor fields is performed newly in the...
The authors examine several topical subjects, commencing with a general introduction to path integra...
The definition and formulas for the harmonic oscillator coherent states and spin coherent states are...
This thesis presents and develops the path integral simulation techniques in application to small qu...
We construct a representation of the coherent state path integral using the Weyl symbol of the Hamil...
The overcompleteness of the coherent states basis leads to a multiplicity of representations of Feyn...
This thesis presents and develops the path integral simulation techniques in application to small qu...
This thesis presents and develops the path integral simulation techniques in application to small qu...
The overcompleteness of the coherent states basis leads to a multiplicity of representations of Feyn...
The density matrix theory, the ancestor of density functional theory, provides the immediate framewo...
By returning to the underlying discrete time formalism, we relate spurious results in coherent state...
We consider a set of operators hat{x}=(hat{x}_1,..., hat{x}_N) with diagonal representatives P(n) in...