mirror of
https://github.com/vale981/master-thesis
synced 2025-03-05 10:01:43 -05:00
6.9 KiB
6.9 KiB
- Literature
- Important Basics
- Todo
- Tasks
- Implement Basic HOPS
- Quantify Heat Transfer
- TeX notes
- verify that second hops state vanishes
- NEXT Adapt New HOPS
- Time Derivative in stocproc
- Generalize to Nonzero Temp
- Try to get Richards old HOPS working
- Test Nonlinear hops
- Generalize to two Baths
- Analytic Verification
- figure out why means involving the stoch. process are so bad
- VORTRAG
- Compare with Rivas Method
- Find Rivas Paper
- NEXT Make proper library
- Three Bath Fridge
- Find the Steady State
- Matrix Eigenvals
- Relation between coerrelation time and hops depth
- Ideas
Literature
Stochastic Processes
Open Systems
- Open Quantum Systems by Rivas
- Fundamentals of quantum optics benjamin by Klauder
Stochastic Unravelings
- The quantum-state diffusion model applied to open systems one of the first applications
- Decoherent histories and quantum state diffusion
NMQSD
HOPS
Numerik
Important Basics
Todo
RESEARCH Quantum Fluctuation theorems?
Tasks
DONE Implement Basic HOPS
CLOCK: [2021-10-08 Fri 08:51] CLOCK: [2021-10-07 Thu 13:38]–[2021-10-07 Thu 17:50] => 4:12
- see my stoch. proc experiments
- ill use richards package
Quantify Heat Transfer
- not as easy as in the cite:Kato2015Aug paper
- maybe heisenberg picture useful
- see my notes. just calculate the time derivative of the bath energy expectation
- my first experiments yield bogus numerics…
- richards code makes it work
-
for derivations see
- the energy balance checks out System + Interaction Energy and my notes
- i've generalized to multiple exponential in this document
DONE TeX notes
- done with nonlinear
DONE verify that second hops state vanishes
NEXT Adapt New HOPS
- Zero Temperature Checks out
- stocproc can generate the time derivative with fft
TODO Time Derivative in stocproc
- done for fft
TODO Generalize to Nonzero Temp
- in cite:RichardDiss the noise hamiltonian method is described
- b.c. only on system -> calculation should go through :)
- not that easy, see notes
- includes time derivative of stoch proc
- idea: sample time derivative and integrate
- not as bad as thought: no exponential form needed -> process smooth
- one can get around the time derivative
- i have implemented finite temperature here
TODO Think about transform
DONE Try to get Richards old HOPS working
- code downloaded from here
- it works see Energy Flow
- interestingly with this model: only one aux state
DONE Test Nonlinear hops
- see here
TODO Generalize to two Baths
- bath-bath correlations
TODO Analytic Verification
- cummings
- and pseudo-mode
TODO Valentin's QMB Gaussian states
DONE figure out why means involving the stoch. process are so bad
- maybe y is wrong -> no
- then: not differentiable + too noisy
- other term is integral and continous, converges faster?
- my test with the gauss process was tupid -> no sum of exponentials
- it works with proper smooth process: Energy Flow in the linear case with smooth correlation…
DONE VORTRAG
- https://www.youtube.com/watch?v=5bRii85RT8s&list=PLJfdTiUFX4cNiK44-ScthZC2SNNrtUGu1&index=33;
- where do i find out more about \(C^\ast\) algebras?
- power \(\dot{W}(t):=\frac{d}{d t}\langle H(t)\rangle=\operatorname{Tr}\left[\dot{H}_{\mathrm{S}}(t) \rho_{\mathrm{SR}}(t)\right]=\operatorname{Tr}\left[\dot{H}_{\mathrm{S}}(t) \rho_{\mathrm{S}}(t)\right]\)
- work is just the change of total energy
- Definitions \(H_{\mathrm{S}}^{\circledast}(t, \beta):=-\beta^{-1} \log \left[\Lambda_{t} \mathrm{e}^{-\beta H_{\mathrm{S}}}\right]\left\{\begin{array}{l}E_{\mathrm{int}}(t):=\operatorname{Tr}\left\{\rho_{\mathrm{S}}(t)\left[H_{\mathrm{S}}^{\circledast}(t, \beta)+\beta \partial_{\beta} H_{\mathrm{S}}^{\circledast}(t, \beta)\right]\right\} \\ F(t):=\operatorname{Tr}\left\{\rho_{\mathrm{S}}(t)\left[H_{\mathrm{S}}^{\circledast}(t, \beta)+\beta^{-1} \log \rho_{\mathrm{S}}(t)\right]\right\} \\ S(t):=\operatorname{Tr}\left\{\rho_{\mathrm{S}}(t)\left[-\log \rho_{\mathrm{S}}(t)+\beta^{2} \partial_{\beta} H_{\mathrm{S}}^{\circledast}(t, \beta)\right]\right\}\end{array}\right.\)
- Properties
- Initial time: \(E_{\text {int }}(0):=\operatorname{Tr}\left[\rho_{\mathrm{S}}(0) H_{\mathrm{S}}\right] \quad\left(H_{\mathrm{S}}^{\circledast}(0, \beta)=H_{\mathrm{S}}\right)\)
TODO Compare with Rivas Method
DONE Find Rivas Paper
NEXT Make proper library
TODO Three Bath Fridge
Mail from Konstantin
here is the paper I had in mind when we talked about the three-bath fridge.
https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.108.070604
I don't know if this scenario has been considered in a strong coupling framework.
This fridge is working continuously. Maybe for HOPS a stroke-based model could be better to avoid long propagation to the steady state. Just as an example, here is an Otto-Fridge with strong coupling (I have not thou thoroughly read this paper)
https://link.springer.com/article/10.1140%2Fepjs%2Fs11734-021-00094-0
Find the Steady State
Matrix Eigenvals
- see cite:Pan1999May
Relation between coerrelation time and hops depth
Ideas
- tune stocproc tansinh with fft