One-dimensional linear harmonic oscillator perturbation

In terms of the spring constant and reduced mass, you should find that ##a^2 = m\omega/\hbar##. Other notations are possible.In summary, the conversation discusses the calculation of the first-order correction to the groundstate energy and the energy of the first excited state for a one-dimensional linear harmonic oscillator perturbed by a Gaussian perturbation. The equations and attempt at a solution involve the calculation of the first-order energy correction and the wavefunction, which is missing a Hermite polynomial. The quantity "a" is the characteristic length scale for the harmonic oscillator and can be defined in terms of the spring constant and reduced mass.
  • #1
Firben
145
0

Homework Statement



Consider a one-dimensional linear harmonic oscillator perturbed by a Gaussian perturbation H' = λe-ax2. Calculate the first-order correction to the groundstate energy and to the energy of the first excited state

Homework Equations



ψn(x) = [itex]\frac{α}{√π*2n*n!}[/itex]1/2 * e2x2[itex]\frac{1}{2}[/itex]

E1n = <ψ0n|H'|ψ0n>

The Attempt at a Solution




E10 = <ψ00|H'|ψ00> =

∫[itex]\frac{α}{√π*2n*n!}[/itex]1/2 * e2x2[itex]\frac{1}{2}[/itex]*[itex]\frac{α}{√π*2n*n!}[/itex]1/2 * e2x2[itex]\frac{1}{2}[/itex]*H'* dx

Is this right ? What is α in this case ?
 
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  • #2
Firben said:

Homework Statement



Consider a one-dimensional linear harmonic oscillator perturbed by a Gaussian perturbation H' = λe-ax2. Calculate the first-order correction to the groundstate energy and to the energy of the first excited state

Homework Equations



ψn(x) = [itex]\frac{α}{√π*2n*n!}[/itex]1/2 * e2x2[itex]\frac{1}{2}[/itex]

E1n = <ψ0n|H'|ψ0n>

The Attempt at a Solution

E10 = <ψ00|H'|ψ00> =

∫[itex]\frac{α}{√π*2n*n!}[/itex]1/2 * e2x2[itex]\frac{1}{2}[/itex]*[itex]\frac{α}{√π*2n*n!}[/itex]1/2 * e2x2[itex]\frac{1}{2}[/itex]*H'* dx

Is this right ? What is α in this case ?
Your expression for the n-th wavefunction is missing the Hermite polynomial Hn(x). It should be
$$\psi_n(x) = \left(\frac{a}{\sqrt{\pi}2^n n!}\right)^{1/2} e^{-a^2x^2/2} H_n(ax).$$ Your expression for the first-order energy correction for the ground state turns out to be fine because H0(x)=1. The quantity ##a## should be defined in your notes or textbook. It's the characteristic length scale for the harmonic oscillator.
 

Related to One-dimensional linear harmonic oscillator perturbation

1. What is a one-dimensional linear harmonic oscillator?

A one-dimensional linear harmonic oscillator is a physical system that exhibits simple harmonic motion, where its position is a sinusoidal function of time. It is characterized by a restoring force that is directly proportional to the displacement from its equilibrium position.

2. What is perturbation in the context of a linear harmonic oscillator?

Perturbation refers to a small change or disturbance in the system that causes it to deviate from its simple harmonic motion. This can be due to external forces or changes in the system's parameters.

3. How is perturbation analyzed in a one-dimensional linear harmonic oscillator?

Perturbation in a one-dimensional linear harmonic oscillator is typically analyzed using the method of perturbation theory. This involves breaking down the system into two parts: the unperturbed system, which represents the simple harmonic motion, and the perturbed system, which represents the deviation caused by the perturbation. The two systems are then combined to determine the overall behavior of the perturbed system.

4. What is the significance of studying perturbations in a linear harmonic oscillator?

Studying perturbations in a linear harmonic oscillator allows us to understand how small changes can affect the behavior of a system. This is important in many fields of science, such as physics, chemistry, and engineering, where systems are often subject to external disturbances that can impact their performance.

5. Can perturbation in a linear harmonic oscillator be used to model real-world systems?

Yes, perturbation in a linear harmonic oscillator can be used to model real-world systems. Many physical systems, such as a mass-spring system, can be approximated as a linear harmonic oscillator. By studying the effects of perturbations on these systems, we can gain insights into the behavior of more complex systems in the real world.

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