Here, \Gamma
represents the coupling strength between system and the fermionic environment with chemical potential \mu
and band-width W
.
With Matsubara Expansion, the correlation function can be analytically solved and expressed as follows:
with
where \zeta_l=(2 l - 1)\pi
. This can be constructed by the built-in function Fermion_Lorentz_Matsubara
:
ds # coupling operator
Γ # coupling strength
μ # chemical potential of the environment
W # band-width of the environment
kT # the product of the Boltzmann constant k and the absolute temperature T
N # Number of exponential terms for each correlation functions (C^{+} and C^{-})
bath = Fermion_Lorentz_Matsubara(ds, Γ, μ, W, kT, N - 1)
With Padé Expansion, the correlation function can be analytically solved and expressed as the following exponential terms:
with
where the parameters \kappa_l
and \zeta_l
are described in J. Chem. Phys. 134, 244106 (2011) and N
represents the number of exponential terms for C^{\nu=\pm}
. This can be constructed by the built-in function Fermion_Lorentz_Pade
:
ds # coupling operator
Γ # coupling strength
μ # chemical potential of the environment
W # band-width of the environment
kT # the product of the Boltzmann constant k and the absolute temperature T
N # Number of exponential terms for each correlation functions (C^{+} and C^{-})
bath = Fermion_Lorentz_Pade(ds, Γ, μ, W, kT, N - 1)