Schedule: Difference between revisions

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* 09/19: B. K. Nikolic, ''One-dimensional models''
===Fall 2022===
* 09/26: J. A. Fernandez Sanchez, ''Schwinger-Keldysh path integral for dissipative harmonic oscillator''.
* B. K. Nikolić, [https://wiki.physics.udel.edu/wiki_qttg/images/3/35/Spin_pumping_mtj.pdf One-dimensional models of adiabatic charge and spin pumping].
* 09/??: L. H. Mai, ''Introduction to the Lindblad master equation'' with QuTiP (Quantum Toolbox in Python) examples.
* 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 examples [[Media:Lindblad_Master_equation_QuTiP.ipynb|[Jupyter Notebook]]].
* L. Herrera, Numerically “exact” approach to open quantum dynamics: The hierarchical equations of motion. [[Media:heom_qutip_herrera.ipynb|[Jupyter Notebook]]].
 
===Spring 2023===
* J. Varela-Manjarres, Floquet engineering of quantum systems.
* S. J. V. Urbano, Application of the Helfrich elasticity theory to the morphology of red blood cells.
 
===Fall 2023===
*B. K. Nikolić, [[Media:PHYS800_hubbard_dimer.pdf|From Hubbard dimer to effective antiferromagnetic Hubbard model for two spins]]
*B. K. Nikolić, [[Media:PHYS800_magnons.pdf|Ground state and low-energy magnon excitations of ferro- and antiferromagnets]]
* F. Garcia-Gaitan, Introduction to DMRG.
* F. Garcia-Gaitan, Antiferromagnetic and altermagnetic magnons.
* F. Garcia-Gaitan, Effective spin Hamiltonian from light-driven Hubbard model.
 
===Spring 2024===
* F. Reyes-Osorio, Schwinger-Keldysh field theory.
* K. J. Rueda-Espinosa, Jaynes–Cummings model.

Latest revision as of 11:27, 29 February 2024

Fall 2022

Spring 2023

  • J. Varela-Manjarres, Floquet engineering of quantum systems.
  • S. J. V. Urbano, Application of the Helfrich elasticity theory to the morphology of red blood cells.

Fall 2023

Spring 2024

  • F. Reyes-Osorio, Schwinger-Keldysh field theory.
  • K. J. Rueda-Espinosa, Jaynes–Cummings model.