Bloch's theorem
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Q: 1. A particle of m moves in the attractive central potential: V(r) = ax6, where a is a constant and…
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A: suppose the normalization constant is A,therefore,
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A: Solution attached in the photo
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Q: e Schrodinger equation
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1) Make use of a translation operator and prove Bloch's theorem in the form :
y (F+R)=e¹ky (7).
An alternative equivalent form for Bloch's theorem is that the wavefunction has the form
7)=eku (F) where u (F) is lattice periodic. By substituting this into the Schrodinger equation
explain the origin of energy bands.
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- For quantum harmonic insulators Using A|0) = 0, where A is the operator of the descending ladder, look for 1. Wave function in domain x: V(x) = (x|0) 2. Wave function in the momentum domain: $(p) = (p|0)solve the problem An electron with angular momentum {= 1 exists in the state X = A Where A is the normalization constant. A) Find the value of A B) If a measurement of Ldis made, what values will be obtained, and with what probabilities?40. The first excited state of the harmonic oscillator has a wave function of the form y(x) = Axe-ax². (a) Follow the
- A conduction electron is confined to a metal wire of length (1.46x10^1) cm. By treating the conduction electron as a particle confined to a one-dimensional box of the same length, find the energy spacing between the ground state and the first excited state. Give your answer in eV. Note: Your answer is assumed to be reduced to the highest power possible. Your Answer: x10 Answer7. Consider a particle in an infinite square well centered at x = 0 in one of its stationary states. For this problem, you may look up any integrals. Some useful ones are given in Harris. a) Compute (x) and (pr) for arbitrary n. Do this by direct computation but then describe how you could have found these results using symmetry (the symmetry can either be symmetry in the physical system, such as the shape of the wave function, or symmetry related to the expectation value integral, such as the shape of the integrand). b) Using your answer to part a), show that the uncertainty in the momentum is Apx nh for arbitrary n. Do this two ways: (i) first by using your answer to part a) and directly computating (p2) (via an integral) and (ii) by using your answer to part a) and relating (p2) to the kinetic energy operator. c) Show that the uncertainty principle holds for the ground state. 2L -Problem: In the problem of cubical potential box with rigid walls, we have: p² + m? + n? = 9, Write down: 1- Schrödinger equation for the particle inside the box. 2- The possible values of: a- e,m,n. b-Eemn c- Pemn d-degree of degeneracy.
- A particular two-level quantum system has two eigenstates given by Ig) := (9) le) := (¿) where |g) is the ground state and le) is the excited state. The Hamiltonian operator is given by Îû = () O A a. Write down the density matrix and calculate for the partition function. b. Calculate for the mean energy of the system. c. Calculate for the expectation value of the operator 1 0 0-1A particle moves in an attractive central potential V(r) = -9²/r3/2. Use the variational principle to find an upper bound to the lowest s-state energy. Use a hydrogenic wave function as your trial function. %3D4) Consider the one-dimensional wave function given below. (a) Draw a graph of the wave function for the region defined. (b) Determine the value of the normalization constant. (c) What is the probability of finding the particle between x = o and x = a? (d) Show that the wave function is a solution of the non-relativistic wave equation (Schrodinger equation) for a constant potential. (e) What is the energy of the wave function? (x) = A exp(-x/a) for x > o (x) = A exp(+x/a) for x < o
- QUESTION 6 Consider a 1-dimensional particle-in-a-box system. How long is the box in radians if the wave function is Y =sin(8x) ? 4 4л none are correct T/2 O O O3. Plane waves and wave packets. In class, we solved the Schrodinger equation for a "free particle" (e.g. when U(x,t) = 0). The correct[solution is (x, t) = Ae(px-Et)/ħ This represents a "plane wave" that exists for all x. However, there is a strange problem with this: if you try to normalize the wave function (determine A by integrating * for all x), you will find an inconsistency (A has to be set equal to 0?). This is because the plane wave stretches to infinity. In order to actually represent a free particle, this solution needs to be handled carefully. Explain in words (and/or diagrams) how we can construct a "wave packet" from the plane wave solution. (Hint 1: consider a superposition of plane waves for a limited range of momentum/energy. Hint 2: have a look at the brief discussion in the middle of pg. 278 and especially pg. 308-309 of the text.)Here are the properties of the GaAs quantum well in the figure. v0 = 100 ??? L = 200 Å ?∗ = 0.067 m* Find the energy values of the first three levels of this well. Corresponding wave functions Draw the graph. It is assumed that the effective mass m* given for the well is also valid for barriers. please. The material of the barrier is not important here. The important thing is the V0 potential.