Infinite one-dimensional oscillators

In summary, the conversation discusses a system of N particles in a line with periodic boundary conditions and pairwise interactions. The Hamiltonian is given in terms of the particles' displacements and conjugate momentums. The Fourier transformed variables are introduced and shown to not be Hermitian. It is then shown that the Fourier modes describe a set of decoupled harmonic oscillators. The Hilbert space of this theory is described in terms of raising and lowering operators of the harmonic oscillators, and the spectrum of the Hamiltonian is discussed. The conversation also explores when it would be appropriate to approximate the displacements by a continuous field and for which observables this would be a good approximation. The sum in the inverse Fourier transforms is finite because the system
  • #1
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Homework Statement



Consider a series of ##N## particles in a line, with the displacement of each particle from its equilibrium position labelled by ##q_{n}## and it conjugate momentum labelled by ##p_n##. Assume that the interaction between the particles is pairwise, so that the Hamiltonian is given by

##H = \Sigma_{n}\ \frac{1}{2m}\ (p_{n}^{2})+ \frac{1}{2}m\omega^{2}(q_{n}-q_{n+1})^{2}##.

Throughout the problem, assume that the boundary conditions are periodic so that ##q_{N+1}=q_{1}##.

(a) Explain why the Fourier transformed variables ##\tilde{q}_{n}## and ##\tilde{p}_{n}## given by

##q_{n}=\frac{1}{\sqrt{N}}\sum\limits_{k=0}^{N-1}\tilde{q}_{k}e^{2\pi ink/N}## and ##p_{n}=\frac{1}{\sqrt{N}}\sum\limits_{k=0}^{N-1}\tilde{p}_{k}e^{2\pi ink/N}##

are not Hermitian. Show that ##\tilde{q}_{N-k}^{\dagger}=\tilde{q}_{k}## and ##\tilde{p}_{N-k}^{\dagger}=\tilde{p}_{k}##.

(b) Show that the Fourier modes describe a set of ##N## decoupled harmonic oscillators (Hint: Write the Hamiltonian in terms of the Fourier modes.)

(c) Describe the Hilbert space of this theory in terms of the raising and lowering operators of these ##N## harmonic oscillators. What is the spectrum of this Hamiltonian?

This is a very simple non-relativistic quantum field theory in the large ##N## limit. Under what circumstances would it be appropriate to approximate the displacements ##q_{n}(t)## by a continuous field ##\phi(x,t)##? For what observables would this be a good approximation?

Homework Equations



The Attempt at a Solution



(a) The inverse Fourier transforms are

##\tilde{q}_{k}=\frac{1}{\sqrt{N}}\sum\limits_{n=0}^{N-1}q_{n}e^{-2\pi ink/N}## and ##\tilde{p}_{k}=\frac{1}{\sqrt{N}}\sum\limits_{n=0}^{N-1}p_{n}e^{-2\pi ink/N}##.

I understand that Fourier series can be written as complex exponentials, but I don't understand why the sum is finite. Can someone please explain?
 
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  • #2

The sum is finite because we are considering a system with a fixed number of particles, N. Therefore, the sum over n runs from 0 to N-1. If we were considering an infinite system, the sum would be infinite as well.
 

1. What is an infinite one-dimensional oscillator?

An infinite one-dimensional oscillator is a theoretical model used in physics to describe a system of particles that are connected by springs and can oscillate back and forth along a single line. It is assumed that the particles have no mass and the springs have no damping, allowing for infinite oscillations to occur.

2. How is an infinite one-dimensional oscillator different from a regular oscillator?

An infinite one-dimensional oscillator is different from a regular oscillator in that it does not have any boundaries or limits in terms of the number of particles or the amplitude of oscillations. This allows for an infinite number of particles to be included in the system and for the oscillations to continue indefinitely.

3. What are some real-life examples of infinite one-dimensional oscillators?

While infinite one-dimensional oscillators are primarily used as theoretical models in physics, they can also be seen in certain physical systems such as a chain of atoms connected by springs, a line of pendulums, or a series of connected electrical circuits.

4. How is the behavior of an infinite one-dimensional oscillator described mathematically?

The behavior of an infinite one-dimensional oscillator is described using the equations of motion for each individual particle in the system, taking into account the forces acting on each particle and the initial conditions of the system. This results in a set of coupled differential equations that can be solved to determine the motion of the particles over time.

5. What are some practical applications of studying infinite one-dimensional oscillators?

Studying infinite one-dimensional oscillators can provide insights into the behavior of other systems that exhibit similar properties, such as wave propagation in solids and fluids, as well as electrical circuits. It can also be used to model and understand the behavior of materials and structures under stress, such as bridges and buildings.

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