Introduction to the "second quantization" formalism for non-relativistic
quantum mechanics: A possible substitution for Sections 6.7 and 6.8 of
Feynman's "Statistical Mechanics"
- URL: http://arxiv.org/abs/1812.10732v5
- Date: Mon, 16 Oct 2023 13:55:42 GMT
- Title: Introduction to the "second quantization" formalism for non-relativistic
quantum mechanics: A possible substitution for Sections 6.7 and 6.8 of
Feynman's "Statistical Mechanics"
- Abstract summary: We define the creation and annihilation operators, discuss their properties, and introduce corresponding representations of states and operators of many-particle systems.
As the title of the note suggests, we cover most topics treated in sections 6.7 and 6.8 of Feynman's "Statistical Mechanics: A Set of Lectures"
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: This is a self-contained and hopefully readable account on the method of
creation and annihilation operators (also known as the Fock space
representation or the "second quantization" formalism) for non-relativistic
quantum mechanics of many particles. Assuming knowledge only on conventional
quantum mechanics in the wave function formalism, we define the creation and
annihilation operators, discuss their properties, and introduce corresponding
representations of states and operators of many-particle systems. As the title
of the note suggests, we cover most topics treated in sections 6.7 and 6.8 of
Feynman's "Statistical Mechanics: A Set of Lectures". As a preliminary, we also
carefully discuss the symmetry of wave functions describing indistinguishable
particles.
We note that all the contents of the present note are completely standard,
and the definitions and the derivations presented here have been known to many.
Although the style of the present note may be slightly more mathematical than
standard physics literatures, we do not try to achieve full mathematical
rigor.(Note to experts: In particular we here DERIVE the (anti)commutation
relations of the creation and annihilation operators, rather than simply
declaring them. In this sense our approach is quite close to that of Feynman's.
But we here focus on the action of creation/annihilation operators on general
$N$ body wave functions, while Feynman makes a heavy use of
Slater-determinant-type states from the beginning. We hope that our
presentation provides a better perspective on the formalism.)
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