Chapter 37: Problem 65
A neutron moves between rigid walls \(8.4 \mathrm{fm}\) apart. What is the energy of its \(n=1\) state?
Chapter 37: Problem 65
A neutron moves between rigid walls \(8.4 \mathrm{fm}\) apart. What is the energy of its \(n=1\) state?
All the tools & learning materials you need for study success - in one app.
Get started for freeA 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?
A proton with a mass of \(1.673 \cdot 10^{-27} \mathrm{~kg}\) is trapped inside a onedimensional infinite potential well of width \(23.9 \mathrm{nm}\). What is the quantum number, \(n\), of the state that has an energy difference of \(1.08 \cdot 10^{-3} \mathrm{meV}\) with the \(n=2\) state?
Consider a square potential, \(U(x)=0\) for \(x<-\alpha, U(x)=-U_{0}\) for \(-\alpha \leq x \leq \alpha,\) where \(U_{0}\) is a positive constant, and \(U(x)=0\) for \(x>\alpha .\) For \(E>0,\) the solutions of the time-independent Schrödinger equation in the three regions will be the following: For \(x<-\alpha, \psi(x)=e^{i \kappa x}+R e^{-i \kappa x},\) where \(\kappa^{2}=2 m E / \hbar^{2}\) and \(R\) is the amplitude of a reflected wave. For \(-\alpha \leq x \leq \alpha, \psi(x)=A e^{i \kappa^{\prime} x}+B e^{-i \kappa^{\prime} x},\) and \(\left(\kappa^{\prime}\right)^{2}=2 m\left(E+U_{0}\right) / \hbar^{2}\) For \(x>\alpha, \psi(x)=T e^{i \kappa x}\) where \(T\) is the amplitude of the transmitted wave. Match \(\psi(x)\) and \(d \psi(x) / d x\) at \(-\alpha\) and \(\alpha\) and find an expression for \(R\). What is the condition for which \(R=0\) (that is, there is no reflected wave)?
Consider an electron approaching a potential barrier \(2.00 \mathrm{nm}\) wide and \(7.00 \mathrm{eV}\) high. What is the energy of the electron if it has a \(10.0 \%\) probability of tunneling through this barrier?
Calculate the ground-state energy for an electron confined to a cubic potential well with sides equal to twice the Bohr radius \((R=0.0529 \mathrm{nm})\). Determine the spring constant that would give this same ground- state energy for a harmonic oscillator.
What do you think about this solution?
We value your feedback to improve our textbook solutions.