Chapter 37: Problem 1
The wavelength of an electron in an infinite potential well is \(\alpha / 2\), where \(\alpha\) is the width of the well. Which state is the electron in? a) \(n=3\) b) \(n=6\) c) \(n=4\) d) \(n=2\)
Chapter 37: Problem 1
The wavelength of an electron in an infinite potential well is \(\alpha / 2\), where \(\alpha\) is the width of the well. Which state is the electron in? a) \(n=3\) b) \(n=6\) c) \(n=4\) d) \(n=2\)
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Get started for freeIf a proton of kinetic energy \(18.0 \mathrm{MeV}\) encounters a rectangular potential energy barrier of height \(29.8 \mathrm{MeV}\) and width \(1.00 \cdot 10^{-15} \mathrm{~m},\) what is the probability that the proton will tunnel through the barrier?
An electron is confined in a three-dimensional cubic space of \(L^{3}\) with infinite potentials. a) Write down the normalized solution of the wave function for the ground state. b) How many energy states are available between the ground state and the second excited state? (Take the electron's spin into account.)
Write a wave function \(\Psi(\vec{r}, t)\) for a nonrelativistic free particle of mass \(m\) moving in three dimensions with momentum \(\vec{p}\), including the correct time dependence as required by the Schrödinger equation. What is the probability density associated with this wave?
In the cores of white dwarf stars, carbon nuclei are thought to be locked into very ordered lattices because the temperature is quite cold, $\sim 10^{4} \mathrm{~K}$. Consider the case of a onedimensional lattice of carbon atoms separated by \(20 \mathrm{fm}\) ( \(1 \mathrm{fm}=\) $1 \cdot 10^{-15} \mathrm{~m}$ ). Consider the central atom of a row of three atoms with this spacing. Approximate the Coulomb potentials of the two outside atoms to follow a quadratic relationship, assuming small vibrations; what energy state would the central carbon atom be in at this temperature? (Use $E=3 / 2 k_{\mathrm{B}} T$.)
An approximately one-dimensional potential well can be formed by surrounding a layer of GaAs with layers of \(\mathrm{Al}_{x} \mathrm{Ga}_{1-x}\) As. The GaAs layers can be fabricated in thicknesses that are integral multiples of the single-layer thickness, \(0.28 \mathrm{nm}\). Some electrons in the GaAs layer behave as if they were trapped in a box. For simplicity, treat the box as a onedimensional infinite potential well and ignore the interactions between the electrons and the Ga and As atoms (such interactions are often accounted for by replacing the actual electron mass with an effective electron mass). Calculate the energy of the ground state in this well for these cases: a) 2 GaAs layers b) 5 GaAs layers
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