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CMI CM-I Problem Sheet MidSem 2013

Node id: 6368page
hsmani's picture 24-08-07 16:08:26 n

CMI CM-I Problem Sheet 113

Node id: 6367page
hsmani's picture 24-08-07 16:08:27 n

CMI CM-I Problem Sheet 112

Node id: 6366page
hsmani's picture 24-08-07 16:08:56 n

CMI CM-I Problem Sheet 111

Node id: 6365page
hsmani's picture 24-08-07 16:08:24 n

CMI CM-I Problem Sheet 110

Node id: 6364page
hsmani's picture 24-08-07 16:08:53 n

CMI CM-I Problem Sheet 109

Node id: 6363page
hsmani's picture 24-08-07 16:08:17 n

CMI CM-I Problem Sheet 108

Node id: 6362page
hsmani's picture 24-08-07 16:08:52 n

CMI CM-I Problem Sheet 107

Node id: 6361page
hsmani's picture 24-08-07 16:08:22 n

CMI CM-I Problem Sheet 106

Node id: 6360page
hsmani's picture 24-08-07 16:08:53 n

CMI CM-I Problem Sheet 105

Node id: 6359page
hsmani's picture 24-08-07 16:08:15 n

CMI CM-I Problem Sheet 104

Node id: 6358page
hsmani's picture 24-08-07 16:08:48 n

CMI CM-I Problem Sheet 103

Node id: 6357page
hsmani's picture 24-08-07 16:08:19 n

CMI CM-I Problem Sheet 102

Node id: 6356page
hsmani's picture 24-08-07 16:08:39 n

CMI CM-I Problem Sheet 101

Node id: 6355page
hsmani's picture 24-08-07 16:08:02 n

Problems in Physics (with solutions)

Node id: 6354page
hsmani's picture 24-08-07 16:08:58 n

[QUE/QFT-03005] QFT-PROBLEM

Node id: 4013page

Show that conformal transformations consisting of dilations \[x^\mu \to x^\mu = e^{-\rho} x^\mu \] and special conformal transformations (SCT) \[x^\mu \to x^{\prime\,\mu}= \frac{x^\mu + c^\mu x^2}{ 1 + 2c \cdot x + c^2 x^2},\] and usual Poincaré transformations form a group. Find the commutation relations for the generators of infinitesimal transformations of this group.

ashok's picture 24-07-31 08:07:18 n

[NOTES/QM-13004] General Properties of Motion in One Dimension

Node id: 2088page

A discussion of nature of energy eigenvalues and eigenfunctions are discussed for general potentials in one dimension. General conditions when to expect the energy levels to be degenerate, continuous or form bands are given. Also the behaviour of eigenfunctions under parity and for also for large distances etc. are discussed.

kapoor's picture 24-07-17 05:07:46 n

[LECS/QM-13] Potential Problems in One Dimension

Node id: 6334page
kapoor's picture 24-07-17 05:07:02 n

[CHAT/QM-13002] LET's TALK --- NATURE OF ENERGY SPECTRUM

Node id: 6320page

For a potential problem in one dimension there are three types of energy levels. These are (a) discrete, (b) continuous doubly degenerate energy eigenvalues, and (c) continuous and non degenerate. In this talk we explain the thumb rules to find out which of this cases apply for a given potential and a specified energy value.

kapoor's picture 24-07-17 04:07:26 n

Sample Content Pages

Node id: 815slideshow
ranjan's picture 24-07-13 11:07:11

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