Bibliography
189
(x i x k ) ω =
1
2
i ¯
h
α
∗
ki − α ik
coth
¯
hω
2kT
(I.13)
(f i f k ) ω =
1
2
i ¯
h
α
−1
ik − α
−1∗
ki
coth
¯
hω
2kT
(I.14)
with
x iω = α ik f kω,
f iω = α
−1
ik x kω
(I.15)
where α ki are the matrix elements of the susceptibility and α ∗
ki the corresponding
complex-conjugate element.
Bibliography
1. Callen, H.B., Welton, T.A.: Irreversibility and generalized noise. Phys. Rev. 83, 34 (1951)
2. Landau, L.D., Lifshitz, E.M.: Statistical Physics, p. 386. Pergamon Press, Oxford (1988)
3. Fornés, J.A.: Fluctuation-dissipation theorem and the polarizability of rodlike polyelectrolytes:
an electric circuit view. Phys. Rev. E. 57, 2110 (1998)
189
(x i x k ) ω =
1
2
i ¯
h
α
∗
ki − α ik
coth
¯
hω
2kT
(I.13)
(f i f k ) ω =
1
2
i ¯
h
α
−1
ik − α
−1∗
ki
coth
¯
hω
2kT
(I.14)
with
x iω = α ik f kω,
f iω = α
−1
ik x kω
(I.15)
where α ki are the matrix elements of the susceptibility and α ∗
ki the corresponding
complex-conjugate element.
Bibliography
1. Callen, H.B., Welton, T.A.: Irreversibility and generalized noise. Phys. Rev. 83, 34 (1951)
2. Landau, L.D., Lifshitz, E.M.: Statistical Physics, p. 386. Pergamon Press, Oxford (1988)
3. Fornés, J.A.: Fluctuation-dissipation theorem and the polarizability of rodlike polyelectrolytes:
an electric circuit view. Phys. Rev. E. 57, 2110 (1998)