Quantum Infinite Potential Well - Probability of Ground-State Energy

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SUMMARY

The discussion focuses on solving a quantum mechanics problem involving a particle in an infinite potential well defined by the wave function \(\psi(x) = Nx(x-L)\) for \(0 < x < L\). The normalization constant \(N\) is determined to be \(\sqrt{\frac{30}{L^{5}}}\). The probability of measuring the ground-state energy is calculated using the amplitude \(\langle \phi_1 | \psi \rangle\), where \(\phi_1(x)\) represents the ground state wave function. Participants emphasize the need to reference eigenstate wave functions or solve the Schrödinger equation for accurate results.

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  • Understanding of quantum mechanics principles, specifically the infinite potential well model.
  • Familiarity with normalization of wave functions in quantum mechanics.
  • Knowledge of the Schrödinger equation and its application to boundary conditions.
  • Ability to compute inner products of wave functions to find probabilities.
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  • Review the derivation of eigenstate wave functions for the infinite potential well.
  • Study the normalization process for quantum mechanical wave functions.
  • Learn how to solve the Schrödinger equation for different potentials.
  • Explore the concept of probability amplitudes and their significance in quantum mechanics.
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Students and professionals in physics, particularly those studying quantum mechanics, as well as educators looking for examples of quantum state normalization and probability calculations in potential wells.

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Homework Statement



A particle in the infinite potential well in the region 0 < x < L is in the state

\psi(x) = \begin{cases}<br /> Nx(x-L) &amp; \text{ if } 0&lt;x&lt;L \\ <br /> 0 &amp; \text{ if } otherwise <br /> \end{cases}

a) Determine the value of N so that the state is properly normalised
b) What is the probability that a measurement of the energy yields the ground-state energy of the
well?
c) What is the expectation value for the Hamiltonian operator for this state?


Homework Equations



\int_{0}^{L}\left | \psi(x) \right |^{2} dx = 1
prob(E_1) = \int_{0}^{L}\left | &lt;\! E_1|\psi(x)\! &gt; \right |^{2} dx

&lt;E_1|=\frac{\hbar^{2}\pi^{2}}{2mL^{2}}

The Attempt at a Solution



For part a, I used the first equation to solve for N, and I got \sqrt{\frac{30}{L^{5}}}. Part b is where I began to get confused.

Given the equations above for prob(E_1), and &lt;E_1|, I'm unable to figure out how to find the probability that the energy state is in the ground state.

Any hints?

Thanks
 
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You found the normalization constant correctly, but the last two of your equations aren't correct. The energy E1 of the ground state |\phi_1\rangle is equal to E_1 = \hbar^2\pi^2/2mL^2.

The amplitude that the particle is in the ground state |\phi_1\rangle is given by

\langle \phi_1 | \psi \rangle = \int \phi_1^*(x)\psi(x)\,dx

where \phi_1(x) is the wave function of the ground state. The probability P that the particle is in the ground state is equal to the modulus of the amplitude squared: P = |\langle \phi_1 | \psi \rangle|^2.
 
Thanks for the reply. How would I go about finding the wave function of the ground state?
 
The infinite square well problem is likely already solved in your textbook or your notes, and you can just look up what the eigenstate wave functions are. If not, you need to solve the Schrödinger equation with the appropriate potential and boundary conditions.
 

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