path: root/content/know/concept/lehmann-representation/index.pdc

---
title: "Lehmann representation"
firstLetter: "L"
publishDate: 2021-11-03
categories:
- Physics
- Quantum mechanics

date: 2021-11-02T19:04:16+01:00
draft: false
markup: pandoc
---

# Lehmann representation

In many-body quantum theory, the **Lehmann representation**
is an alternative way to write the [Green's functions](/know/concept/greens-functions/),
obtained by expanding in the many-particle eigenstates
under the assumption of a time-independent Hamiltonian $\hat{H}$.

We start by writing out the
greater Green's function $G_{\nu \nu'}(t, t')$,
and then expanding its thermal expectation value $\expval{}$
into a sum of many-particle basis states $\ket{n}$:

$$\begin{aligned}
    G_{\nu \nu'}^>(t, t')
    = - \frac{i}{\hbar} \expval{\hat{c}_\nu(t) \hat{c}_{\nu'}^\dagger(t')}
    &= - \frac{i}{\hbar Z} \sum_{n} \matrixel**{n}{\hat{c}_\nu(t) \hat{c}_{\nu'}^\dagger(t') e^{-\beta \hat{H}}}{n}
\end{aligned}$$

Where $\beta = 1 / (k_B T)$, and $Z$ is the partition function
(see [canonical ensemble](/know/concept/canonical-ensemble/));
the operator $e^{\beta \hat{H}}$ gives the weight of each term at thermal equilibrium.
Since $\ket{n}$ is an eigenstate of $\hat{H}$ with energy $E_n$,
this gives us a factor of $e^{\beta E_n}$.
Furthermore, we are in the [Heisenberg picture](/know/concept/heisenberg-picture/),
so we write out the time-dependence of $\hat{c}_\nu$ and $\hat{c}_{\nu'}^\dagger$:

$$\begin{aligned}
    G_{\nu \nu'}^>(t, t')
    &= - \frac{i}{\hbar Z} \sum_{n} e^{-\beta E_n} \matrixel**{n}{e^{i \hat{H} t / \hbar} \hat{c}_\nu e^{- i \hat{H} t / \hbar}
    e^{i \hat{H} t' / \hbar} \hat{c}_{\nu'}^\dagger e^{- i \hat{H} t' / \hbar}}{n}
    \\
    &= - \frac{i}{\hbar Z} \sum_{n} e^{-\beta E_n}
    \matrixel**{n}{e^{i \hat{H} (t - t') / \hbar} \hat{c}_\nu e^{- i \hat{H} (t - t') / \hbar} \hat{c}_{\nu'}^\dagger}{n}
\end{aligned}$$

Where we used that the trace $\Tr\!(x) = \sum_{n} \matrixel{n}{x}{n}$
is invariant under cyclic permutations of $x$.
The $\ket{n}$ form a basis of eigenstates of $\hat{H}$,
so we insert an identity operator $\sum_{n'} \ket{n'} \bra{n'}$:

$$\begin{aligned}
    G_{\nu \nu'}^>(t - t')
    &= - \frac{i}{\hbar Z} \sum_{n n'} e^{- \beta E_n}
    \matrixel**{n}{e^{i \hat{H} (t - t') / \hbar} \hat{c}_\nu e^{- i \hat{H} (t - t') / \hbar}}{n'} \matrixel**{n'}{\hat{c}_{\nu'}^\dagger}{n}
    \\
    &= - \frac{i}{\hbar Z} \sum_{n n'} e^{-\beta E_n}
    \matrixel*{n}{\hat{c}_\nu}{n'} \matrixel*{n'}{\hat{c}_{\nu'}^\dagger}{n} e^{i (E_n - E_{n'}) (t - t') / \hbar}
\end{aligned}$$

Note that $G_{\nu \nu'}^>$ now only depends on the time difference $t - t'$,
because $\hat{H}$ is time-independent.
Next, we take the [Fourier transform](/know/concept/fourier-transform/)
$t \to \omega$ (with $t' = 0$):

$$\begin{aligned}
    G_{\nu \nu'}^>(\omega)
    &= - \frac{i}{\hbar Z} \sum_{n n'} e^{-\beta E_n} \matrixel*{n}{\hat{c}_\nu}{n'} \matrixel*{n'}{\hat{c}_{\nu'}^\dagger}{n}
    \int_{-\infty}^\infty e^{i (E_n - E_{n'}) t / \hbar} \: e^{i \omega t} \dd{t}
\end{aligned}$$

Here, we recognize the integral
as a [Dirac delta function](/know/concept/dirac-delta-function/) $\delta$,
thereby introducing a factor of $2 \pi$,
and arriving at the Lehmann representation of $G_{\nu \nu'}^>$:

$$\begin{aligned}
    \boxed{
        G_{\nu \nu'}^>(\omega)
        = - \frac{2 \pi i}{Z} \sum_{n n'} e^{-\beta E_n} \matrixel*{n}{\hat{c}_\nu}{n'} \matrixel*{n'}{\hat{c}_{\nu'}^\dagger}{n}
        \: \delta(E_n - E_{n'} + \hbar \omega)
    }
\end{aligned}$$

We now go through the same process for the lesser Green's function $G_{\nu \nu'}^<(t, t')$:

$$\begin{aligned}
    G_{\nu \nu'}^<(t - t')
    &= \mp \frac{i}{\hbar Z} \sum_{n} \matrixel*{n}{\hat{c}_{\nu'}^\dagger(t') \hat{c}_\nu(t) e^{-\beta \hat{H}}}{n}
    \\
    &= \mp \frac{i}{\hbar Z} e^{-\beta E_n} \sum_{n n'} \matrixel*{n}{\hat{c}_{\nu'}^\dagger}{n'} \matrixel*{n'}{\hat{c}_\nu}{n}
   e^{i (E_{n'} - E_n) (t - t') / \hbar}
\end{aligned}$$

Where $-$ is for bosons, and $+$ for fermions.
Fourier transforming yields the following:

$$\begin{aligned}
    G_{\nu \nu'}^<(\omega)
    &= \mp \frac{2 \pi i}{\hbar Z} \sum_{n n'} e^{-\beta E_n} \matrixel*{n}{\hat{c}_{\nu'}^\dagger}{n'} \matrixel*{n'}{\hat{c}_\nu}{n}
    \: \delta(E_{n'} - E_n + \hbar \omega)
\end{aligned}$$

We swap $n$ and $n'$, leading to the following
Lehmann representation of $G_{\nu \nu'}^<$:

$$\begin{aligned}
    \boxed{
        G_{\nu \nu'}^<(\omega)
        = \mp \frac{2 \pi i}{Z} \sum_{n n'} e^{-\beta E_{n'}} \matrixel*{n}{\hat{c}_\nu}{n'} \matrixel*{n'}{\hat{c}_{\nu'}^\dagger}{n}
        \: \delta(E_n - E_{n'} + \hbar \omega)
    }
\end{aligned}$$

Due to the delta function $\delta$,
each term is only nonzero for $E_n' = E_n + \hbar \omega$,
so we write:

$$\begin{aligned}
    G_{\nu \nu'}^<(\omega)
    = \mp \frac{2 \pi i}{\hbar Z} \sum_{n n'} e^{-\beta (E_n + \hbar \omega)}
    \matrixel*{n}{\hat{c}_\nu}{n'} \matrixel*{n'}{\hat{c}_{\nu'}^\dagger}{n} \: \delta(E_n - E_{n'} + \hbar \omega)
\end{aligned}$$

Therefore, we arrive at the following useful relation
between $G_{\nu \nu'}^<$ and $G_{\nu \nu'}^>$:

$$\begin{aligned}
    \boxed{
        G_{\nu \nu'}^<(\omega)
        = \pm e^{-\beta \hbar \omega} G_{\nu \nu'}^>(\omega)
    }
\end{aligned}$$

Moving on, let us do the same for
the retarded Green's function $G_{\nu \nu'}^R(t, t')$, given by:

$$\begin{aligned}
    G_{\nu \nu'}^R(t \!-\! t')
    &= \Theta(t \!-\! t') \Big( G_{\nu \nu'}^>(t - t') - G_{\nu \nu'}^<(t - t') \Big)
    \\
    &= - \frac{i}{\hbar Z} \Theta(t \!-\! t') \sum_{n n'}
    \matrixel*{n}{\hat{c}_\nu}{n'} \matrixel*{n'}{\hat{c}_{\nu'}^\dagger}{n}
     \Big( e^{-\beta E_n} \mp e^{- \beta E_{n'}} \Big) e^{i (E_n - E_{n'}) (t - t') / \hbar}
\end{aligned}$$

We take the Fourier transform, but to ensure convergence,
we must introduce an infinitesimal positive $\eta \to 0^+$ to the exponent
(and eventually take the limit):

$$\begin{aligned}
    G_{\nu \nu'}^R(\omega)
    &= - \frac{i}{\hbar Z} \sum_{n n'} \Big( ... \Big) \int_{-\infty}^\infty \Theta(t) e^{i (E_n - E_{n'}) t / \hbar} e^{i (\omega + i \eta) t} \dd{t}
    \\
    &= - \frac{i}{\hbar Z} \sum_{n n'} \Big( ... \Big) \int_0^\infty e^{i (E_n - E_{n'}) t / \hbar} e^{i (\omega + i \eta) t} \dd{t}
    \\
    &= - \frac{i}{\hbar Z} \sum_{n n'} \Big( ... \Big)
    \bigg[ \frac{\hbar e^{i (\hbar \omega + E_n - E_{n'}) t / \hbar} e^{- \eta t}}{i (\hbar \omega + E_n - E_{n'}) - \hbar \eta} \bigg]_0^\infty
\end{aligned}$$

Leading us to the following Lehmann representation
of the retarded Green's function $G_{\nu \nu'}^R$:

$$\begin{aligned}
    \boxed{
        G_{\nu \nu'}^R(\omega)
        = \frac{1}{Z} \sum_{n n'}
        \frac{\matrixel*{n}{\hat{c}_\nu}{n'} \matrixel*{n'}{\hat{c}_{\nu'}^\dagger}{n}}{\hbar (\omega + i \eta) + E_n - E_{n'}}
        \Big( e^{-\beta E_n} \mp e^{- \beta E_{n'}} \Big)
    }
\end{aligned}$$

Finally, we go through the same steps for the advanced Green's function $G_{\nu \nu'}^A(t, t')$:

$$\begin{aligned}
    G_{\nu \nu'}^A(t \!-\! t')
    &= \Theta(t' \!-\! t) \Big( G_{\nu \nu'}^<(t - t') - G_{\nu \nu'}^>(t - t') \Big)
    \\
    &= \frac{i}{\hbar Z} \Theta(t' \!-\! t) \sum_{n n'}
    \matrixel*{n}{\hat{c}_\nu}{n'} \matrixel*{n'}{\hat{c}_{\nu'}^\dagger}{n}
     \Big( e^{-\beta E_n} \mp e^{- \beta E_{n'}} \Big) e^{i (E_n - E_{n'}) (t - t') / \hbar}
\end{aligned}$$

For the Fourier transform, we must again introduce $\eta \to 0^+$
(although note the sign):

$$\begin{aligned}
    G_{\nu \nu'}^A(\omega)
    &= \frac{i}{\hbar Z} \sum_{n n'} \Big( ... \Big) \int_{-\infty}^\infty \Theta(-t) e^{i (E_n - E_{n'}) t / \hbar} e^{i (\omega - i \eta) t} \dd{t}
    \\
    &= \frac{i}{\hbar Z} \sum_{n n'} \Big( ... \Big) \int_{-\infty}^0 e^{i (E_n - E_{n'}) t / \hbar} e^{i (\omega - i \eta) t} \dd{t}
    \\
    &= \frac{i}{\hbar Z} \sum_{n n'} \Big( ... \Big)
    \bigg[ \frac{\hbar e^{i (\hbar \omega + E_n - E_{n'}) t / \hbar} e^{\eta t}}{i (\hbar \omega + E_n - E_{n'}) + \hbar \eta} \bigg]_{-\infty}^0
\end{aligned}$$

Therefore, the Lehmann representation of
the advanced Green's function $G_{\nu \nu'}^A$ is as follows:

$$\begin{aligned}
    \boxed{
        G_{\nu \nu'}^A(\omega)
        = \frac{1}{Z} \sum_{n n'}
        \frac{\matrixel*{n}{\hat{c}_\nu}{n'} \matrixel*{n'}{\hat{c}_{\nu'}^\dagger}{n}}{\hbar (\omega - i \eta) + E_n - E_{n'}}
        \Big( e^{-\beta E_n} \mp e^{- \beta E_{n'}} \Big)
    }
\end{aligned}$$

As a final note, let us take the complex conjugate of this expression:

$$\begin{aligned}
    \big( G_{\nu \nu'}^A(\omega) \big)^*
    = \frac{1}{Z} \sum_{n n'}
    \frac{\matrixel*{n}{\hat{c}_{\nu'}}{n'} \matrixel*{n'}{\hat{c}_\nu^\dagger}{n}}{\hbar (\omega + i \eta) + E_n - E_{n'}}
    \Big( e^{-\beta E_n} \mp e^{- \beta E_{n'}} \Big)
\end{aligned}$$

Note the subscripts $\nu$ and $\nu'$.
Comparing this to $G_{\nu \nu'}^R$ gives us another useful relation:

$$\begin{aligned}
    \boxed{
        G^R_{\nu \nu'}(\omega)
        = \big( G^A_{\nu' \nu}(\omega) \big)^*
    }
\end{aligned}$$



## References
1.  H. Bruus, K. Flensberg,
    *Many-body quantum theory in condensed matter physics*,
    2016, Oxford.