LOYOLA COLLEGE (AUTONOMOUS), CHENNAI – 600 034
... 12) Evaluate ( um, x un) where un’s are the eigenfunctions of a linear harmonic oscillator. 13) Prove that “the momentum operator in quantum mechanics is the generator of infinitesimal translations”. 14) (a) Prove that ( σ.A) (σ.B) = A.B + i σ. ( A xB) where σ’s are the Pauli spin matrices , if the ...
... 12) Evaluate ( um, x un) where un’s are the eigenfunctions of a linear harmonic oscillator. 13) Prove that “the momentum operator in quantum mechanics is the generator of infinitesimal translations”. 14) (a) Prove that ( σ.A) (σ.B) = A.B + i σ. ( A xB) where σ’s are the Pauli spin matrices , if the ...
Course Topics for EEE 631
... Prerequisite: EEE531, EEE637 and basics of quantum mechanics, solid states and semiconductor physics Course Description: Principles of heterojunctions and quantum well structures, band lineups, optical, and electrical properties. Introduces heterojunction devices. Knowledge of transport and recombin ...
... Prerequisite: EEE531, EEE637 and basics of quantum mechanics, solid states and semiconductor physics Course Description: Principles of heterojunctions and quantum well structures, band lineups, optical, and electrical properties. Introduces heterojunction devices. Knowledge of transport and recombin ...
Quantum Condensed Matter Field Theory
... more exposed than in the study of strongly interacting classical and quantum manyparticle systems. The aim of this course is to introduce modern methods of theoretical physics tailored to the description of collective phenomena where microscopic (and, often, perturbative) approaches fail. The fundam ...
... more exposed than in the study of strongly interacting classical and quantum manyparticle systems. The aim of this course is to introduce modern methods of theoretical physics tailored to the description of collective phenomena where microscopic (and, often, perturbative) approaches fail. The fundam ...
synopsis of the Elegant Universe and other stuff
... geometry of space-time so completely that not even light can escape the “hole.” With the advent of the idea of black holes, a gaping disparity between the two major theories of physics have become glaringly evident. Specifically, because black holes are so massive and affect the geometry of space-ti ...
... geometry of space-time so completely that not even light can escape the “hole.” With the advent of the idea of black holes, a gaping disparity between the two major theories of physics have become glaringly evident. Specifically, because black holes are so massive and affect the geometry of space-ti ...
Jan. 23, 2006
... from excited-state atoms emitting a photon and falling down to a lower quantum-number ...
... from excited-state atoms emitting a photon and falling down to a lower quantum-number ...
Atomic Structure
... spectra of hydrogen in gas phase. Line spectra due to the excitation of electrons from lower energy level to a higher one. When the electron falls to a lower energy level or ground state it emits a specific amount of energy. The line spectra are not restricted to the visible range but also extend in ...
... spectra of hydrogen in gas phase. Line spectra due to the excitation of electrons from lower energy level to a higher one. When the electron falls to a lower energy level or ground state it emits a specific amount of energy. The line spectra are not restricted to the visible range but also extend in ...
TAP 413- 6: Charged particles moving in a magnetic field
... Some astrophysicists believe that the radio signals of 109 Hz reaching us from Jupiter are emitted by electrons orbiting in Jupiter’s magnetic field. Assuming the frequency of the radio emission is identical to the cyclotron frequency; find the strength of the magnetic field around Jupiter. ...
... Some astrophysicists believe that the radio signals of 109 Hz reaching us from Jupiter are emitted by electrons orbiting in Jupiter’s magnetic field. Assuming the frequency of the radio emission is identical to the cyclotron frequency; find the strength of the magnetic field around Jupiter. ...
Charged particles moving in a magnetic field
... Some astrophysicists believe that the radio signals of 10 Hz reaching us from Jupiter are emitted by electrons orbiting in Jupiter’s magnetic field. Assuming the frequency of the radio emission is identical to the cyclotron frequency; find the strength of the magnetic field around Jupiter. ...
... Some astrophysicists believe that the radio signals of 10 Hz reaching us from Jupiter are emitted by electrons orbiting in Jupiter’s magnetic field. Assuming the frequency of the radio emission is identical to the cyclotron frequency; find the strength of the magnetic field around Jupiter. ...
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.