This question consists of the basic calculations which are often referred to as "trivial" in most references in circuit-QED. However, are not so trivial for anyone who starts fresh into the quantum optics involved for studying the input/output (I/O), and therefore the measurements in actual architecture of QC. (With some quality answer this can become a resource for starters to refer to). The starting point is to study the Quantum Langevin Equations from some 'rare' quantum optics texts. The notation is standard:

$\Omega:$ Cavity Frequency

$\Gamma$: Dissipation/decay rate

$b_{\text{in/out}}$: Input/Output field operators

$a$ & $a^\dagger$: Cavity modes

The solution to the Langevin equation reads:

$a(t)=a(0)\text{e}^{-(i\Omega +\Gamma/2)}-\sqrt{\Gamma}\int_0^tds$ $\text{e}^{-(i\Omega+\Gamma/2)(t-s)}b_{\text{in}}(s)$.

(1) Prove the commutators:

$[a^\dagger(t),b_{\text{in}}(t')]=0 \quad$ for $t<t'$

$[a^\dagger(t),b_{\text{in}}(t)]=-\frac{1}{2}\sqrt{\Gamma} \quad$

$[a^\dagger(t'),b_{\text{in}}(t')]=-\sqrt{\Gamma}\text{e}^{-(i\Omega+\Gamma/2)(t-t')} \quad$ for $t>t'$


(2) Given the time reversed Langevin equation


find the solution for $a(t)$ in terms of the output field at a future time $T$.

(3) Prove the relation


where the standard Fourier transform is defined as: $\tilde{f}(\omega)=\frac{1}{2\pi} \int_{-\infty}^{\infty}\text{e}^{i\omega t}f(t)dt$

(4) Given the I/O relation and boundary condition:


Prove the simpler relation:


where $\delta(\omega)$ is a phase shift which preserves the commutation relations for the I/O operators under the Fourier transform.

  • $\begingroup$ each question should contain a single, laser-focused question. Feel free to edit this question to focus on a single aspect of it, providing as many details about what you understand/know about it etc $\endgroup$
    – glS
    Feb 2 at 10:47