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Many-body Quantum Mechanics
Many-body Quantum Mechanics

... the method of using annihilation and creation operators acting on a Fock space as ”second quantization”. As should be clear from the above, this terminology is misleading in the sense that ψ̂ is not a once more quantized version of the wave function, but an object which is directly (or via a Fourier ...
LOYOLA COLLEGE (AUTONOMOUS), CHENNAI – 600 034
LOYOLA COLLEGE (AUTONOMOUS), CHENNAI – 600 034

ph 2811 / 2808 - quantum mechanics
ph 2811 / 2808 - quantum mechanics

... 6. State and prove Ehernfest’s theorem 7. Solve the Schrodinger equation for a linear harmonic oscillator. Sketch the first two eigenfunctions of the system. 8. Determine the eigenvalue spectrum of angular momentum operators Jz and Jz 9. What are symmetric and antisymmetric wave functions? Show that ...
Notations for today’s lecture (1 ) A complete set of ;
Notations for today’s lecture (1 ) A complete set of ;

... where i and j are labels for single particle states and ci☨ is an electron creation operator. Determine the 2-particle wave function. (b) Write down a reasonable approximation for the wave function of a helium atom in its ground state. (c ) Verify that the wave function in (b) is antisymmetric under ...
Quantum Theory of Condensed Matter: Problem Set 1 Qu.1
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Exercises in Statistical Mechanics
Exercises in Statistical Mechanics

... Exercises in Statistical Mechanics Based on course by Doron Cohen, has to be proofed Department of Physics, Ben-Gurion University, Beer-Sheva 84105, Israel This exercises pool is intended for a graduate course in “statistical mechanics”. Some of the problems are original, while other were assembled ...
Problem set 7
Problem set 7

You are going to read the chapter at home.
You are going to read the chapter at home.

< 1 ... 8 9 10 11 12

Second quantization

Second quantization is a formalism used to describe and analyze quantum many-body systems. It is also known as canonical quantization in quantum field theory, in which the fields (typically as the wave functions of matters) are thought of as field operators, in a similar manner to how the physical quantities (position, momentum etc.) are thought of as operators in first quantization. The key ideas of this method were introduced in 1927 by Dirac, and were developed, most notably, by Fock and Jordan later.In this approach, the quantum many-body states are represented in the Fock state basis, which are constructed by filling up each single-particle state with a certain number of identical particles. The second quantization formalism introduces the creation and annihilation operators to construct and handle the Fock states, providing useful tools to the study of the quantum many-body theory.
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