Schedule: Difference between revisions
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===Fall 2022=== | ===Fall 2022=== | ||
* B. K. Nikolic, | * B. K. Nikolic, One-dimensional models of adiabatic charge and spin pumping. | ||
* J. A. Fernandez Sanchez, | * J. A. Fernandez Sanchez, Schwinger-Keldysh ("in-in") vs. Feynman ("in-out") path integral with harmonic oscillator examples. | ||
* L. H. Mai, | * L. H. Mai, Introduction to the Lindblad master equation with QuTiP and/or HOQST examples with accompanying [[Media:Lindblad_Master_equation_QuTiP.ipynb|Jupyter Notebook]]. | ||
* L. Herrera, Numerically “exact” approach to open quantum dynamics: The hierarchical equations of motion. | |||
* L. Herrera, | * J. M. Varela, Quantum to classical crossover of Floquet engineering in correlated quantum systems. | ||
* J. Kim, Measurement-induced decoherence and information in double-slit interference. |
Revision as of 13:12, 29 November 2022
Fall 2022
- B. K. Nikolic, One-dimensional models of adiabatic charge and spin pumping.
- J. A. Fernandez Sanchez, Schwinger-Keldysh ("in-in") vs. Feynman ("in-out") path integral with harmonic oscillator examples.
- L. H. Mai, Introduction to the Lindblad master equation with QuTiP and/or HOQST examples with accompanying Jupyter Notebook.
- L. Herrera, Numerically “exact” approach to open quantum dynamics: The hierarchical equations of motion.
- J. M. Varela, Quantum to classical crossover of Floquet engineering in correlated quantum systems.
- J. Kim, Measurement-induced decoherence and information in double-slit interference.