
MSc Phy App
... Perturbation Theory: Non-degenerate and Degenerate Cases. applications: Zeeman and Stark effects. Induced electric dipole moment of Hydrogen Real Hydrogen Atom: Relativistic correction, spin-orbit coupling, hyperfine interaction, Helium atom, exclusion principle, exchange interaction. Unit-II Schrod ...
... Perturbation Theory: Non-degenerate and Degenerate Cases. applications: Zeeman and Stark effects. Induced electric dipole moment of Hydrogen Real Hydrogen Atom: Relativistic correction, spin-orbit coupling, hyperfine interaction, Helium atom, exclusion principle, exchange interaction. Unit-II Schrod ...
Towards Heisenberg Limit in Magnetometry with
... Stimulated emission enhanced visibility of two-photon counts for various phases of the coherent field with respect to the gain factor g. The pump phase is fixed at . The modulus of the coherent field | 0 | is chosen such that the coincidences coming from SPDC and the coherent fields are equal ...
... Stimulated emission enhanced visibility of two-photon counts for various phases of the coherent field with respect to the gain factor g. The pump phase is fixed at . The modulus of the coherent field | 0 | is chosen such that the coincidences coming from SPDC and the coherent fields are equal ...
Chapter 4 Particle Nature of Matter. Solutions of Selected
... velocity selector, only passing electrons with speed v, where v = V /Bd (Equation 4.6), while in the region where there is only a magnetic field the electron moves in a circle of radius r, with r given by p = Bre. This latter region (E = 0, B = constant) acts as a momentum selector because electrons ...
... velocity selector, only passing electrons with speed v, where v = V /Bd (Equation 4.6), while in the region where there is only a magnetic field the electron moves in a circle of radius r, with r given by p = Bre. This latter region (E = 0, B = constant) acts as a momentum selector because electrons ...
Renormalization

In quantum field theory, the statistical mechanics of fields, and the theory of self-similar geometric structures, renormalization is any of a collection of techniques used to treat infinities arising in calculated quantities.Renormalization specifies relationships between parameters in the theory when the parameters describing large distance scales differ from the parameters describing small distances. Physically, the pileup of contributions from an infinity of scales involved in a problem may then result in infinities. When describing space and time as a continuum, certain statistical and quantum mechanical constructions are ill defined. To define them, this continuum limit, the removal of the ""construction scaffolding"" of lattices at various scales, has to be taken carefully, as detailed below.Renormalization was first developed in quantum electrodynamics (QED) to make sense of infinite integrals in perturbation theory. Initially viewed as a suspect provisional procedure even by some of its originators, renormalization eventually was embraced as an important and self-consistent actual mechanism of scale physics in several fields of physics and mathematics. Today, the point of view has shifted: on the basis of the breakthrough renormalization group insights of Kenneth Wilson, the focus is on variation of physical quantities across contiguous scales, while distant scales are related to each other through ""effective"" descriptions. All scales are linked in a broadly systematic way, and the actual physics pertinent to each is extracted with the suitable specific computational techniques appropriate for each.