Homework Set 3

Problem 1: Action on fermionic creation and annihilation operators on Fock states

Using the following convention

$|11111000\dots ⟩={\hat{c}}_5^{†}{\hat{c}}_4^{†}{\hat{c}}_3^{†}{\hat{c}}_2^{†}{\hat{c}}_1^{†}|\mathrm{v}\mathrm{a}\mathrm{c}\mathrm{u}\mathrm{u}\mathrm{m}⟩$

where $|\mathrm{v}\mathrm{a}\mathrm{c}\mathrm{u}\mathrm{u}\mathrm{m}>=|0000\dots ⟩$:

(a) Evaluate ${\hat{c}}_3^{†}{\hat{c}}_6{\hat{c}}_4{\hat{c}}_6^{†}{\hat{c}}_3|111110000\dots ⟩$.

(b) Write $|1101100100\dots ⟩$ in terms of excitations about the "filled Fermi sea" $|1111100000\dots ⟩$. Interpret your answer in terms of electron and hole excitations.

(c) Find $⟨\mathrm{\Phi }|\hat{N}|\mathrm{\Phi }⟩$, where $|\mathrm{\Phi }⟩=A|100⟩+B|111000⟩$ and $\hat{N}=\sum _i{\hat{c}}_i^{†}+{\hat{c}}_i$ is the operator of the total particle number.

Problem 2: Density-density correlation function for noninteracting electrons

The pair correlation function gives the relative probability of finding a particle at position ${\mathbf{𝐫}}^{\prime }$ if we know that there is one at position $\mathbf{𝐫}$. It is defined by:

$G(\mathbf{𝐫}-{\mathbf{𝐫}}^{\prime })=⟨\mathrm{\Phi }(\mathbf{𝐫})|{\hat{\mathrm{\Psi }}}^{†}({\mathbf{𝐫}}^{\prime })\hat{\mathrm{\Psi }}({\mathbf{𝐫}}^{\prime })|\mathrm{\Phi }(\mathbf{𝐫})⟩=⟨{\mathrm{\Phi }}_0|{\hat{\mathrm{\Psi }}}^{†}(\mathbf{𝐫}){\hat{\mathrm{\Psi }}}^{†}({\mathbf{𝐫}}^{\prime })\hat{\mathrm{\Psi }}({\mathbf{𝐫}}^{\prime })\hat{\mathrm{\Psi }}(\mathbf{𝐫})|{\mathrm{\Phi }}_0⟩$

Here $|\mathrm{\Phi }(\mathbf{𝐫})⟩=\hat{\mathrm{\Psi }}(\mathbf{𝐫})|{\mathrm{\Phi }}_0⟩$ is a state with $N-1$ particles, obtained after removal of one particle at position $\mathbf{𝐫}$, so that pair correlation function is computed as the expectation value of the density operator in this new quantum state. Compute the pair correlation function for a system of translationally invariant noninteracting spinless bosons in many-body state

$|{\mathrm{\Phi }}_0⟩=|n_{{\mathbf{𝐤}}_0},n_{{\mathbf{𝐤}}_1},\dots ⟩$

by transforming field operators to creation and annihilation operators in momentum representation while assuming that bosons are enclosed in a box of volume $V$ with periodic boundary conditions. Your final result should be a function of $\mathbf{𝐫},{\mathbf{𝐫}}^{\prime }$ and sums over $n_{\mathbf{𝐤}}$, where you can also use that

$⟨{\mathrm{\Phi }}_0|{\hat{\mathrm{\Psi }}}^{†}(\mathbf{𝐫})\hat{\mathrm{\Psi }}(\mathbf{𝐫})|{\mathrm{\Phi }}_0⟩=\frac{1}{V}\sum _{\mathbf{𝐤}}{n}_{\mathbf{𝐤}}=N$.

Problem 4: BSC superconductor in Zeeman field

Consider a thin film superconductor whose thickness is small enough to allow the penetration of the magnetic field into the interior, while any coupling of magnetic field to orbital degrees of freedom is neglected. Its BCS Hamiltonian in the presence of a magnetic field $\mathbf{𝐁}=B{\mathbf{𝐞}}_z$, coupling only to the spin, can then be written as:

$\hat{H}=\sum _{\mathbf{𝐤},\sigma }({\epsilon }_{\mathbf{𝐤}}-\mu -\sigma {\mu }_{B}B){\hat{c}}_{\mathbf{𝐤}\sigma }^{†}{\hat{c}}_{\mathbf{𝐤}\sigma }+\sum _{\mathbf{𝐤},{\mathbf{𝐤}}^{\prime }}{V}_{\mathbf{𝐤},{\mathbf{𝐤}}^{\prime }}{\hat{c}}_{{\mathbf{𝐤}}^{\prime }\uparrow }^{†}{\hat{c}}_{-{\mathbf{𝐤}}^{\prime }\downarrow }^{†}{\hat{c}}_{-\mathbf{𝐤}\downarrow }{\hat{c}}_{\mathbf{𝐤}\uparrow }$

Here $V_{\mathbf{𝐤},{\mathbf{𝐤}}^{\prime }}=-V_0/\mathrm{\Omega }$ ($\mathrm{\Omega }$ is volume) for $\mathbf{𝐤},{\mathbf{𝐤}}^{\prime }$ within a shell of energy width Failed to parse (unknown function "\math"): {\displaystyle \hbar \omega_D <\math> on either side of the Fermi surfaace and zero otherwise; <math> \mu_B } is the Bohr magneton; and $\sigma =+1$ for $\uparrow$ spin and $\sigma =-1$ for $\downarrow$ spin.