Download Document 8171030

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

Hidden variable theory wikipedia , lookup

Density matrix wikipedia , lookup

Matter wave wikipedia , lookup

Aharonov–Bohm effect wikipedia , lookup

Wave–particle duality wikipedia , lookup

Propagator wikipedia , lookup

Coupled cluster wikipedia , lookup

Renormalization group wikipedia , lookup

Theoretical and experimental justification for the Schrödinger equation wikipedia , lookup

Second quantization wikipedia , lookup

Perturbation theory (quantum mechanics) wikipedia , lookup

T-symmetry wikipedia , lookup

Path integral formulation wikipedia , lookup

Resonance wikipedia , lookup

Scalar field theory wikipedia , lookup

Self-adjoint operator wikipedia , lookup

Compact operator on Hilbert space wikipedia , lookup

Coherent states wikipedia , lookup

Relativistic quantum mechanics wikipedia , lookup

Canonical quantum gravity wikipedia , lookup

Symmetry in quantum mechanics wikipedia , lookup

Dirac bracket wikipedia , lookup

Molecular Hamiltonian wikipedia , lookup

Canonical quantization wikipedia , lookup

Transcript
k
g
vz
xz
f
Quantization of the electrical LC harmonic oscillator:
parallel LC oscillator circuit:
voltage across the oscillator:
total energy (Hamiltonian):
with the charge Q stored on the capacitor
a flux f stored in the inductor
properties of Hamiltonian written in variables Q and f
Q and f are canonical variables
see e.g.: Goldstein, Classical Mechanics, Chapter 8, Hamilton Equations of Motion
Quantum version of Hamiltonian
with commutation relation
compare with particle in a harmonic potential:
analogy with electrical oscillator:
- charge Q corresponds to momentum p
- flux f corresponds to position x
Hamiltonian in terms of raising and lowering operators:
with oscillator resonance frequency:
Raising and lowering operators:
number operator
in terms of Q and f
with Z c being the characteristic impedance of the oscillator
charge Q and flux f operators can be expressed in terms of raising and lowering
operators:
Exercise: Making use of the commutation relations for the charge and flux operators,
show that the harmonic oscillator Hamiltonian in terms of the raising and lowering
operators is identical to the one in terms of charge and flux operators.