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0 votes
1 answer
99 views

Action-angle variables for three-dimensional harmonic oscillator using cylindrical coordinates

I am solving problem 19 of ch 10 of Goldstein mechanics. The problem is: A three-dimensional harmonic oscillator has the force constant k1 in the x- and y- directions and k3 in the z-direction. Using ...
SYD's user avatar
  • 13
6 votes
1 answer
252 views

Symmetry group of a two-dimensional isotropic harmonic oscillator

The Lagrangian and the Hamiltonian of a two-dimensional isotropic oscillator (with $m=\omega=1$) are $$L=\frac{1}{2}(v^2_1+v_2^2-q_1^2-q_2^2)\tag{1}$$ and $$H=\frac{1}{2}(p^2_1+p_2^2+q_1^2+q_2^2),\tag{...
Solidification's user avatar
1 vote
0 answers
71 views

Order $\epsilon^2$ mean rate of change in action variable for adiabatic oscillator

In adiabatic theory of classical mechanics, considering a linear oscillator with a slowly changing frequency $\omega=\omega(t)$, Percival and Richards's nice book (pp. 144-147) discusses how it is ...
user135626's user avatar
3 votes
1 answer
113 views

Interpretation of this Hamiltonian

I'm studying a system with the following Hamiltonian $$ H = \frac{1}{2}P^TAP + \frac{1}{2}Q^T B Q$$ where $P,Q$ are canonical variables (4-vectors) and $A,B$ matrices such that $A = A^\dagger$ and $B =...
Gyro's user avatar
  • 143
3 votes
2 answers
293 views

Meaning of "the symmetry group of an $N$-dimensional quantum isotropic oscillator is $U(N)$"

Symmetry of this system has been discussed here but I'm still confused. Consider a $N$-dimensional isotropic harmonic oscillator, with hamiltonian $$H = \hbar \omega \left(a^\dagger_i a_i + \frac{N}{2}...
confused_nevin's user avatar
2 votes
1 answer
183 views

Using the EoM in the canonical quantization of EM field

Starting from the classical electromagnetic field, there two approaches to quantization that I want to compare. The problem arises when I write the classical fields in terms of $a$ and $a^*$, which ...
Mr. Feynman's user avatar
  • 1,989
4 votes
1 answer
132 views

Almost all Liouville torus is preserved for small oscillation problems even if we don't use second-order approximation to potential energy, right?

In small oscillation problems, we use a second-order approximation to the potential energy function (suppose the oscillation is around the point $(0,\cdots, 0)$), $$ V(x) = V(0) + \frac{\partial^2 V(0)...
Mr. Egg's user avatar
  • 81
1 vote
1 answer
128 views

Separation of Hamilton's Principal Function

In Goldstein's "Classical Mechanics", at page 437, a two-dimensional anisotropic harmonic oscillator is studied by means of Hamilton-Jacobi formalism. In particular, Goldstein claims that: ...
Matteo Menghini's user avatar
0 votes
1 answer
370 views

Hamiltonian constraint

I am having some difficulties regarding this wikipedia article. I can't understand why the action (for the harmonic oscilator) is written as it is. That is, why is the Hamiltonian followed by a $\...
LSS's user avatar
  • 980
0 votes
1 answer
184 views

Hamilton's equations of motion for damped oscillator

Consider a parallel RLC oscillator. Kirchhoff's equations of motion are $$ \ddot{\Phi} + \frac{1}{\tau}\dot{\Phi} + \omega_0^2 \Phi = 0 $$ where $\tau = RC$ and $\omega_0 = 1 / \sqrt{LC}$. What is ...
DanielSank's user avatar
  • 24.6k
1 vote
0 answers
72 views

Canonical transformation of the harmonic oscillator‘s Hamiltonian [closed]

I could deduce the Hamiltonian of the damped harmonic oscillator: $$ H=\frac{p^2}{2m}e^{-2 \gamma t}+\frac{m \omega_0^2 q^2}{2}e^{2 \gamma t} $$ Using the canonical transformation $Q=e^{\gamma t}q, P=...
Henry T.'s user avatar
  • 512
0 votes
1 answer
51 views

Existence of a unitary transform $(q,p) \rightarrow (-q, p)$

If $q$ and $p$ are the canonical position and momentum operators of a quantum harmonic oscillator, is there a unitary that transforms $(q,p)$ into $(-q, p)$? For instance, denoting the annihilation ...
Ronan's user avatar
  • 433
2 votes
1 answer
53 views

Symmetry associated to a part of a separable Hamiltonian

The harmonic oscillator in 3D is: $$H=\frac{p_x^2+p_y^2+p_z^2}{2m}+ \frac{k}{2} (x^2+y^2+z^2) = H_x + H_y + H_z,$$ where $H_x$, $H_y$ and $H_z$ are all constants of motion (alongside $\vec{L}$). Time ...
Syrocco's user avatar
  • 1,168
5 votes
0 answers
158 views

Why does metaplectic correction fix the vacuum energy?

In geometric quantization we want to go from a symplectic manifold $\left( M, \omega \right)$ to a Hilbert space $H$. If $M$ is prequantizable, we find a prequantum bundle $L \rightarrow M$ with ...
leob's user avatar
  • 559
0 votes
1 answer
1k views

Simple (classical, non-damped) 1D harmonic oscillator - how to represent phase space elliptical trajectory in polar form for an ellipse?

Considering a classical, non-damped 1D harmonic oscillator (e.g. mass $m$ oscillating along $x$-axis attached to spring with constant $k$) -- described by Hamiltonian (for constant energy $E$) $$E=p^2/...
Dave's user avatar
  • 97

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