Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Consider an electron that is confined to the \(x y\) -plane by a twodimensional rectangular infinite potential well. The width of the well is \(w\) in the \(x\) -direction and \(2 w\) in the \(y\) -direction. What is the lowest energy that is shared by more than one distinct state, that is, two different states having the same energy?

Short Answer

Expert verified
Answer: The lowest shared energy is \(2\left(\dfrac{h^2}{8m}\right)\dfrac{1}{w^2}\).

Step by step solution

01

Understand the energy formula

For an electron in a two-dimensional infinite potential well, the energy formula is given by: \(E_{n_x, n_y} = \dfrac{h^2}{8m} \left(\dfrac{n_x^2}{w^2} + \dfrac{n_y^2}{(2w)^2} \right)\) where \(E_{n_x, n_y}\) is the energy corresponding to energy levels \((n_x, n_y)\), \(h\) is Planck's constant, \(m\) is the mass of the electron, and \(w\) is the width of the well in the \(x\) direction.
02

List the energy levels

To find the lowest energy shared by more than one distinct state, let's find the energy values for the first few energy levels \((n_x, n_y)\). We start from \((1,1)\) and increase \(n_x\) and \(n_y\) by 1 until we find a shared energy. We can simplify the energy formula by replacing \(\frac{h^2}{8m}\) with constant \(A\) and taking \(w=1\) to analyze the energy levels: \(E_{n_x, n_y} = A \left(\dfrac{n_x^2}{1^2} + \dfrac{n_y^2}{(2)^2} \right) = A \left(n_x^2 + \dfrac{n_y^2}{4} \right)\) Let's list the energy levels \((n_x, n_y)\) and their corresponding energies: \((1,1): E_{11} = A(1^2 + \dfrac{1^2}{4}) = A\left(1 + \dfrac{1}{4}\right) = \dfrac{5}{4}A\) \((1,2): E_{12} = A(1^2 + \dfrac{2^2}{4}) = A\left(1 + 1\right) = 2A\) \((2,1): E_{21} = A(2^2 + \dfrac{1^2}{4}) = A\left(4 + \dfrac{1}{4}\right) = \dfrac{17}{4}A\) \((2,2): E_{22} = A(2^2 + \dfrac{2^2}{4}) = A\left(4 + 1\right) = 5A\)
03

Identify the lowest shared energy

Analyzing the energy levels listed above, we find that energy levels \((1,2)\) and \((2,1)\) have the same energy (\(E_{12}=E_{21}=2A\)). Since no other shared energy values are found for these energy levels, the lowest shared energy is \(2A\). In terms of the original energy expression: \(E = 2\left(\dfrac{h^2}{8m}\right)\dfrac{1}{w^2}\)

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

An electron with a mass of \(9.109 \cdot 10^{-31} \mathrm{~kg}\) is trapped inside a onedimensional infinite potential well of width \(13.5 \mathrm{nm}\). What is the energy difference between the \(n=5\) and the \(n=1\) states?

A particle is trapped inside a one-dimensional infinite potential well of width \(19.3 \mathrm{nm}\). The energy difference between the \(n=2\) and the \(n=1\) states is \(2.639 \cdot 10^{-25} \mathrm{~J}\). What is the mass of the particle?

An oxygen molecule has a vibrational mode that behaves approximately like a simple harmonic oscillator with frequency \(2.99 \cdot 10^{14} \mathrm{rad} / \mathrm{s} .\) Calculate the energy of the ground state and the first two excited states.

A surface is examined using a scanning tunneling microscope (STM). For the range of the gap, \(L\), between the tip of the probe and the sample surface, assume that the electron wave function for the atoms under investigation falls off exponentially as \(|\psi|=e^{-\left(10.0 \mathrm{nm}^{-1}\right) a}\). The tunneling current through the tip of the probe is proportional to the tunneling probability. In this situation, what is the ratio of the current when the tip is \(0.400 \mathrm{nm}\) above a surface feature to the current when the tip is \(0.420 \mathrm{nm}\) above the surface?

Think about what happens to wave functions for a particle in a square infinite potential well as the quantum number \(n\) approaches infinity. Does the probability distribution in that limit obey the correspondence principle? Explain.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free