Course of lectures on quantum fluctuations
Course content
Maxwell equations for macroscopic electrodynamics
Separation of electric and magnetic modes
Action and Lagrangian for macroscopic electrodynamics
Quantum vacuum energy
Green's function, Green's dyadic
Multiple scattering formalism, Stress tensor method
Lifshitz energy
Elbaum-Schick systems
Attendance list: Mathias Boström, Iver Brevik, Prachi Parashar, K. V. Shajesh, Subhojit Pal, John Joseph Marchetta, Niranjan Warnakulasooriya, Venkat Abhignan, and Aryan Illiat.
Lecture 1: Kramers-Kronig relation for response functions, Feb. 10, 2024
Presenter: Prof. K. V. Shajesh
Southern Illinois University--Carbondale, USA
Lecture content
Contents of first ten equations in emthin.
Examples, like Drude model, plasma model, and Drude-Lorentz model, were not discussed in detail.
Discussion
In axion electrodynamics, the electric (magnetic) polarization gets a response from the magnetic (electric) field. The implications of the causal nature of this response should be investigated. Look up literature.
Lecture 2: Correlation function, Feb. 17, 2024
Presenter: Prof. K. V. Shajesh
Southern Illinois University--Carbondale, USA
Lecture content
Schwinger's quantum action principle
Correlations are described by Green's function
Zero-dimension example: Harmonic oscillator forced by a noise (not satisfactorily completed)
Discussion
The divergences in the single-body Casimir energy of a dielectric ball are known to cancel out for mediums εμ=1. Could this feature be derived as a generic statement at the formalism level for an arbitrary single body?
Use our ideas in arXiv:1709.06284 and arXiv:2105.05507 to evaluate conclusions similar to those by Barrow in arXiv:2004.09444. For example, can we derive the horizon radius of a blackhole constructed out of self-similar concentric spheres?
Lecture 3: Maxwell equations, Feb. 24, 2024
Presenter: Prof. K. V. Shajesh
Southern Illinois University--Carbondale, USA
Lecture content
Maxwell equations
Lagrangian for macroscopic electrodynamics
Dielectric function is Hermitian
Discussion
What is the physical interpretation of the external Polarization source?
Are fluctuations in polarization sources or the fluctuations in the fields the origins of zero point energy?
How is the dielectric function being Hermitian compatible with Kramers-Kronig relation? The hermitianity requires the principal dielectric components to be real. Thus, it does not allow dissipation. However, we will assume a small amount of dissipation to accommodate causality. This will then lead to a fluctuation-dissipation theorem.
Lecture 4: Quantum vacuum energy, March. 2, 2024
Presenter: Prof. K. V. Shajesh
Southern Illinois University--Carbondale, USA
Lecture content
Variation in dynamical fields, source function, and background potential.
Green's dyadic
Quantum vacuum energy
Discussion
Derive the expression for quantum vacuum energy, presuming magnetic monopoles are allowed in the theory, and the magnetic source function is switched on.
Does the action formulation in terms of frequency allow one to attend problems that are out of equilibrium? Is Schwinger-Keldysh method about this.
The variation in the action due to variation in the background potential is functional. For a given body, can we use the idea of the calculus of variation to find the surface that minimizes the Casimir energy?