Chapter 7: Problem 87
An electron with kinetic energy \(2.0 \mathrm{MeV}\) encounters a potential energy barrier of height \(16.0 \mathrm{MeV}\) and width 2.00 nm. What is the probability that the electron emerges on the other side of the barrier?
Chapter 7: Problem 87
An electron with kinetic energy \(2.0 \mathrm{MeV}\) encounters a potential energy barrier of height \(16.0 \mathrm{MeV}\) and width 2.00 nm. What is the probability that the electron emerges on the other side of the barrier?
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Get started for freeAn electron confined to a box of width 0.15 nm by infinite potential energy barriers emits a photon when it makes a transition from the first excited state to the ground state. Find the wavelength of the emitted photon.
Vibrations of the hydrogen molecule \(\mathrm{H}_{2}\) can be modeled as a simple harmonic oscillator with the spring constant \(\quad k=1.13 \times 10^{3} \mathrm{N} / \mathrm{m} \quad\) and \(\quad\) mass \(m=1.67 \times 10^{-27} \mathrm{kg} .\) (a) What is the vibrational frequency of this molecule? (b) What are the energy and the wavelength of the emitted photon when the molecule makes transition between its third and second excited states?
. Estimate the ground state energy of the quantum harmonic oscillator by Heisenberg's uncertainty principle. Start by assuming that the product of the uncertainties \(\Delta x\) and \(\Delta p\) is at its minimum. Write \(\Delta p\) in terms of \(\Delta x\) and assume that for the ground state \(x \approx \Delta x\) and \(p \approx \Delta p\) then write the ground state energy in terms of \(x .\) Finally, find the value of \(x\) that minimizes the energy and find the minimum of the energy.
If a classical harmonic oscillator can be at rest, why can the quantum harmonic oscillator never be at rest? Does this violate Bohr's correspondence principle?
Is it possible to measure energy of \(0.75 \hbar \omega\) for a quantum harmonic oscillator? Why? Why not? Explain.
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