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DYK-04 Who Revived the Klein Gordon Equation?Node id: 1828pageThe Klein Gordon equation in its original interpretation suffered from problem of negative probabilities. After quantum electrodynamics was successfully formulated, the second quantized Klein Gordon equation was shown to give a consistent formulation for spin zero particles. WHO DID THIS WORK?
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LFM/QM-13 :: Normalization of Continuous Energy SolutionsNode id: 3112page |
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Sample Quiz : Identities in QM Node id: 286page |
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Bits and PiecesNode id: 3327pageAs the name itself suggests, pages in this heirarchy are Bits and Pieces of resources. Most of these are targets of links in other pages on this site and also in pdf files distributed by email. Links may be provided to students, and friends alike for quickly checking some points.
The contant of most of resources will be obvious to the experts and also an experienced students
Some Bits and Pieces are collected to fill gaps left in text books and may serve useful purpose for a beginner. Many of these might be moved or removed completely in future.
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DYK-06 Position Operator in Relativistic Quantum Mechanics Node id: 1831page |
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Sample Rapid Fire QuizNode id: 288page |
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Quick ReminderNode id: 3332pageMiscelleaneous pages of quick reminder, need as prerequisite as some where else, will appear here
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Books - Not SortedNode id: 3163page |
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Random Mix-03 What all information does state of a quantum system give?Node id: 227pageRandom Mix-03 "What all information does state of a quantum system give?"
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PTR/QM-06002 --- Dynamical Variables as hemitian operators Node id: 1969page |
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Quiz Sample [ Ask a question to answer to another question ]Node id: 252page |
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DYK-08 Who proposed electron spin first and what happened to the proposal?Node id: 2114page |
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Works of Masters always have something to offerNode id: 723pageI take the best from every one. But GOLD FROM OLD, There is always something to learn from MASTERS;
In this age of internet, there is a tendency to open internet and learn from Wikipedia and similar sites. While this has its own advantages for a mature learner, I recommend that a beginner must learn from the masters even though the learning curve may look very steep.
This collection is an attempt to encourage younger generation to leart role of contibuting to the subject and from the very best.
There are many who contributed to pedgogy and teaching. Many old texts become 'obsolete' simply because is it fashionable to go for the latest. It would be foolhardy to ignore these and other works, so we include here snippets and quotes etc. from many other sources too.
It is hoped this will provide incentive to the younger generations to ask for more.
"Choose the very best from every one"
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DYK-12 :: What is a gauge? as Explained by Pankaj SharanNode id: 3103page The following (from notes for a lecture I was preparing) might help explain the context: The first gauge theory was Hermann Weyl's extension of Einstein's general theory of relativity with a parallel transport that can change the scale or 'gauge' of lengths of the transported vector. About this one can read in P. G. Bergman's book on Relativity. The Hamiltonian formulation of electrodynamics, and in particular, the replacement of \(\vec{p}\) by \(\vec{p}-e\vec{A}/c \) was given by Larmor in his book "Aether and Matter", Cambridge (1900). [quoted by Pauli in ''General Principles of Quantum Mechanics" , Section 4. (Tr. by P. Achuthan and K. Venkatesan of 1958 German edition) Allied, New Delhi 1980.] In quantum mechanics the 'canonical momentum' \(\vec{p}-e\vec{A}/c\) becomes \(-i\hbar[\nabla-ie\vec{A}/(\hbar c)]\). The gauge invariance of the Schrodinger theory under \(\vec{A}\to \vec{A}+\nabla f\) and \(\phi\to \phi-(e/c)\frac{\partial f}{\partial t} \) when \(\Psi\) is changed by a phase was first given by V. Fock (1927). The analogy of this group of transformations to the Weyl theory on gravitation and electricity was pointed out by F. London (1927). The connection of this group to charge conservation was pointed out by Weyl while writing variational principle for the wave equation. [See Pauli as above.]
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Random Mix-04 Coordinate Representation Node id: 281pageRandom Mix-04 Coordinate Representation
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PTR/EM-04001 Properties of ConductorsNode id: 2235page |
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From Masters :: Is friction a force of constraint or applied force?Node id: 3289page |
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DYK-03 Jacobi Action PrincipleNode id: 1827pageJacobi Action Principle A Second Variational Principle for Conservative Systems
Hamilton.'s action principle in classical mechanics is widely taught. There is a lesser known, but important Jacobi principle which is like Fermat's principle for waves. This form of action principle was used by Schrodinger to arrive at his hafous equation for qunatum mechanics of a point particles.
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Sample Quiz Focussed on a Key ConceptNode id: 285page |
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DYK-05 Change in Sign of Fermion Wave Function under 2$\pi$ RotationNode id: 1830pageIt is well known the wave function of a fermion changes sign under rotation by \(2\pi\). Has this been verified experimentally?
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