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\(\S\S\) 7.6 Q[4] \(\int_0^\infty \frac{x^p}{x^2+a^2}\, dx\)Node id: 1865page |
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\(\S\S\) 7.6 Q[3] \(\int_0^\infty \frac{x^{p-1}}{(x+1)^2}\, dx\)Node id: 1864page |
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\(\S\S\) 7.6 Q[1] \(\int_0^\infty \frac{x^{\frac{1}{2}}}{(x+4)(x+25)}\)Node id: 1862page |
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\(\S\S\) 7.9 Q[6] \(\int_0^\infty \frac{x\{\exp(-qx) + \exp[(q-p)x]\}}{1- \exp(-px)}\, dx \)Node id: 1892page |
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VS-Problem Sets-06 -- Matrix RepresentationNode id: 1819page |
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VS-Problem Sets-03 -- Linear FunctionalsNode id: 1817page |
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VS-Problem Sets-02 Linear Independence, Basis and DimesnsionNode id: 1816page |
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VS-Problem Sets-01 -- Groups, Fields Vector Spaces Node id: 1815page |
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\(\S 14.1\) Particle in Three Dimensional Box Node id: 1095page |
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LEC/QM-Mod19 Partial Wave Analysis Node id: 1059page |
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LEC/QM-Mod18 Integral Equation, Born ApproximationNode id: 1058page |
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I-1 Overview of Module-INode id: 4559pageSyllabus Classical fields; Functional derivatives; Action principle for fields. Lagrangian form of dynamics; Noether's theorem; Hamiltonian dynamics; Poisson brackets.
Prerequisites An Elementary exposure to the following topics will be sufficient to get started on this unit.
Classical fields; Examples of Classical fields; Eelectromagnetic field as example of fields; Maxwell's equations as field equations.
Relativistic quantum mechanics; Klein Gordon equation; Dirac equation;
Quantum mechanics of a point particle; Time dependent Schrodinger equation.
Different resources are planned to be made available in multiple formats [ audio / video / article style / Slides style etc] |
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Submit a WebForm:: Classical and Quantum SystemsNode id: 4576page |
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ODE Special Purpose PacksNode id: 1668page |
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Chemistry formulae and equationsNode id: 4580pageThe site supports typesetting chemical formulae and equation using MathJax extension mhchem.
Here are a few examples taken from the mhchem manual site.
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MM-Sub-01 Topics in Set TheoryNode id: 4579draftnode |
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Help and Information --- About Lessons in Proofs ProjectNode id: 4574page |
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Submit A WebForm:: Why Interpret Schrodinger Equation as Classical Field Equation?Node id: 4577page |
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Submit A WebForm :: Describe What is a Classical Fields?Node id: 4575page |
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Lesson/CM03-01 Action PrincipleNode id: 4396page $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}\newcommand{\dd}[2][]{\frac{d#1}{d#2}}${}$\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}${}$\newcommand{\ket}[1]{|#1\rangle}$ {} $\newcommand{\bra}[1]{\langle #1|}$ |
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