Solve for Probability of Particle Energy E_n in Infinite Square Well"

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Homework Help Overview

The problem involves a particle of mass m in an infinite square well, with a given wave function at time t = 0. Participants are tasked with finding the probability of obtaining specific energy eigenvalues associated with the particle's state.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the normalization of the wave function and the expansion over the eigenstates of the Hamiltonian. Questions arise regarding the use of sine and cosine functions for different values of n and the implications for the coefficients c_n.

Discussion Status

Some participants have provided guidance on the method to find the coefficients c_n using orthonormality, while others are exploring the implications of the wave function's symmetry on the probabilities for even and odd n. There is acknowledgment of the relationship between the probability and the energy eigenvalues, but no consensus on specific calculations has been reached.

Contextual Notes

Participants are working under the assumption of a well-defined infinite square well from x = -a to x = +a, and are considering the implications of the wave function's symmetry on the calculated probabilities.

Logarythmic
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Please help me with this problem:

"A particle of mass m moves in one dimension in the infinite square well. Suppose that at time t = 0 its wave function is

PSI(x,t=0) = A(a^2 - x^2)

where A is a normalisation constant.

Find the probability P_n of obtaining the value E_n of the particle energy, where E_n is one of the energy eigenvalues."


I know how to find A and I know how to find the time-dependent wave function, but what then?
 
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Logarythmic said:
Please help me with this problem:

"A particle of mass m moves in one dimension in the infinite square well. Suppose that at time t = 0 its wave function is

PSI(x,t=0) = A(a^2 - x^2)

where A is a normalisation constant.

Find the probability P_n of obtaining the value E_n of the particle energy, where E_n is one of the energy eigenvalues."


I know how to find A and I know how to find the time-dependent wave function, but what then?

I notice that you are using a well going from x=-a to x=+a, right?

You have to expand your wavefunction over the eigenstates of the Hamiltonian (which are simply the sine and cos functions with their normalization factors).
[tex]\Psi(x) = \Sum c_n \psi_n(x)[/tex]
where the [itex]\psi_n[/itex] are the normalized sin/cos functions.
To find the c_n, just use the orthonormality of the psi_n,

[tex]c_n = \int_{-a}^a dx \, \psi_n^*(x) \Psi(x)[/tex]

and, finally, the probability of the energy being measured to be a specific value E_n is given by |c_n|^2.
 
Yeah that does it, thank you. =)
 
I use the sin function for even n and the cos function for odd n, right? But then c_n for even n gets zero..? Is that correct?

For odd n I get P(E_n) = 15/((n^4)(pi^4))
 
Logarythmic said:
I use the sin function for even n and the cos function for odd n, right? But then c_n for even n gets zero..? Is that correct?

For odd n I get P(E_n) = 15/((n^4)(pi^4))
I did not check your result for odd n but it makes sense that for even n you would get zero. Your wavefunction is symmetric function (it is even in the sense of Psi(-x) = Psi(x)) so that it does not "contain" any of the sin functions which are odd themselves.

Your answer seems also to make sense since, as expected, the probabibility goes down with increasing n. Also, your function ressembles the most the ground state so one expects a very quick decrease with n.
Lastly, one double check would be to verify that the sum to infinity over odd n of 1/n^4 gives pi^4/15.

Good job!

Pat
 

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