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4.1 For the thermal state : For the pure state : 4.2 By mathematical induction, you can prove: Hence: 4.4 Current conservation: Branch currents: Hence: Without the register: With the register: 4.5 4.6 This is very rough apporximation. I'm â¦
In the following discussion, we assume that the quantum states are quasi-static. We solve the time-independent Schrödinger equation supposing that external potentials are independent of time . When we change them slowly enough, the correspâ¦
The effective wavefunction and the charge current are given as: --- (3.4) ---(3.13)The wavefunction follows the Schrödinger equation: --- (3.5)Without losing the generality, we can take the Coulomb gauge: --- (1)Now, we assume that the chaâ¦
Quantum Information and Quantum Optics with Superconducting Circuitsä½è :GarcÃa Ripoll, Juan JoséCambridge University PressAmazon Derivation of the Lindblad master equation (2.26) I found the following paper is useful to understand the genâ¦
Effective wavefunction describing the flow of superconducting elections (Cooper pairs): Schrödinger equation for : --- (3.5)I will show that this model is invariant under the gauge transformation: [Proof](3.5) is equivalent to --- (1)A simâ¦
arxiv.orgp.8 Equation (24) p.10 Equation (30) p.11 Equation (31) p.13 Derivation of (45) from (44)First, in (44), we change the integral variable from (without any approximation) to get: Then, we assume that the kernel in the integration iâ¦