Show that the angular momentum operator, Îz = (ħ/i) d/dφ, is hermitian.
Hint: consider the wavefunction ψ(φ), where φ varies from 0 to 2π
We can show that LxLx is Hermitian by directly evaluating its adjoint and showing that it’s equal to LxLx, using the fact that the adjoint operator is antilinear and antidistributive:
L†x=(ypz−zpy)†=(ypz)†−(zpy)†=p†zy†−p†yz†=pzy−pyz=ypz−zpy=LxLx†=(ypz−zpy)†=(ypz)†−(zpy)†=pz†y†−py†z†=pzy−pyz=ypz−zpy=Lx
We have used the fact that (AB)†=B†A†(AB)†=B†A†.
Similarly Ly,LzLy,Lz are Hermitian.
Show that the angular momentum operator, Îz = (ħ/i) d/dφ, is hermitian. Hint: consider the wavefunction...
2.The angular momentum is L = p a) What is the representation of the angular momentum operator b)Use the polar coordinates to compute L o)Show that the eigenfunction forp) m(p),where mis integer. What is the Τηφ(p),where What mis integer. is the eigenfunction φ(p), assume 0 (p) 2π
2.The angular momentum is L = p a) What is the representation of the angular momentum operator b)Use the polar coordinates to compute L o)Show that the eigenfunction forp) m(p),where mis integer. What...
Consider the function y(φ)-e",-ie h2 d where I is a constant? If so, what is the a) Is it an eigenfunctions of the operator O-- eigenvalue? (answer: no) b) Normalize the function on the domain 0 φś2π (in this case, normalization implies | | ψ(0) 12 dφ= 1 ). Euler's identity, etimp-cos(mo) ± isin(mo), where m is a constant, will be useful (φ)-F(e"-ie")) to evaluate the normalization constant. (answer: ya normalized
Consider the function y(φ)-e",-ie h2 d where I is...
Show that momentum space is equivalent to position space knowing that the operator X̂=i(hbar)(∂/∂p). ( ∫(-∞ --> ∞) Ψ•(x) x Ψ(x)dx = ( ∫(-∞ --> ∞) Φ•(p) (i(hbar)(∂/∂p)) Φ(p)dp Please show detailed steps. Thank you.
qm 09.3
3. An operator  is Hermitian if it satisfies the condition $ $(y) dx = (Ap) u dx, for any wavefunctions $(x) and y(x). (i) The time dependent Schrödinger equation is ih au = fu, at where the Hamiltonian operator is Hermitian. Show that the equation of mo- tion for the expectation value of any Hermitian operator  is given by d(A) IH, Â]), dt ħi i = where the operator  does not depend explicitly on time....
1. Show y = sin ax is not an eigenfunction of the operator d/dx, but is an eigenfunction of the operator da/dx. 2. Show that the function 0 = Aeimo , where i, m, and A are constants, is an eigenfunction of the angular momentum operator is the z-direction: M =; 2i ap' and what are the eigenvalues? 3. Show the the function y = Jź sin MA where n and L are constants, is an eigenfunction of the Hamiltonian...
Consider a particle with mass m described by the Hamilton operator for a one-dimensional harmonic oscillator 2 Zm 2 The normalized eigenfunctions for Hare φη (x) with energies E,,-(n + 2) ha. At time t-0 the wavefunction of the particle is given by у(x,0)- (V3іфі (x) + ф3(x)). Now let H' be an operator given by where k is a positive constant. 1) Show that H' is Hermitian. 2) Express H' by the step-operators a+ and a 3) Calculate the...
1. The wavefunction corresponding to Im> energy and angular momentum eigenstate of a particle rotating in a ring for m-l and m--1 are, respectively N2T where ? is the angular position of the particle relative to thex axis (see slide 15 of lecture 74a). (a) show that the probability density does not depend on 0. (b) Show that P,(o)-sin() where p, (0) rticle in the quantum state V, (d) p, (0) obviously resembles one of the orbitals of the is...
8. (9 pts: 3 per part) Consider an operator 1/3 i (a) Calculate the Hermitian adjoint R (b) Is the operator R Hermitian or not? Explain. What can you conclude about its eigenvectors? What can you conclude about its eigenvalues? (c) Calculate the eigenvalue(s) of R (hint: it is non-degenerate)
qm 09.4
4. The commutation relations defining the angular momentum operators can be written [Îx, Îy] = iħẢz, with similar equations for cyclic permutations of x, y and z. Angular momentum raising and lowering operators can be defined as În = Îx ihy (i) Show that [Lz, L.] = +ħL. [6 marks] (ii) If øm is an eigenfunction of ł, with eigenvalue mħ, show that the state given by L+øm is also an eigenfunction of L, but with an eigenvalue...
3. Consider a rigid rotor whose Hamiltonian is given by H L2(21) where L is the angular momentum operator and I is the moment of inertia of the rotator. Its rotation is described by a wave function: (0, N{Yo0(0,6)(1 3i) Y1-1(0,6) 2 Y21(0.0) Y20(0.) Find the normalization constant, N. (i) Find the probability to occupy state Yo0- (ii Find the expectation value of L2 of this state (iii Find the expectation value of L2 of this state (iv) Find (L2L2/21...