a) Derive the following commutator relationships between the components of angular momentum L and of p:
(i) [Ly, px] = −ih(bar)pz
(ii) [Ly, pz] = ih(bar)px
(iii) [Ly, p2x ] = −2ih(bar)pxpz
(iiii) [Ly, p2z ] = 2ih(bar)pxpz
(b) Hence show that the square L2 of the angular momentum operator L commutes with the kinetic energy operator
p2/2m = (p2x + p2y + p2z )/2m.
a) Derive the following commutator relationships between the components of angular momentum L and of p:...
1. Given that angular momentum is given by L=(r)(p), the components of the angular momentum can be found to be: Lx=ypz-zpy Ly=zpx-xpz Lz=xpy-ypx (a) What are the corresponding angular momentum operators Lx, Ly, and Lz? (b) write communation relations [Lx, Ly], [Ly, Lz], and [Lz, Lx]. What does these expressions say about the ability to measure components of angular momentum simultaneously? plz explain part B in depth dont do derivation of commutation relation explain the second part also do part...
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....
Classically, orbital angular momentum is given by L = r times p, where p is the linear momentum. To go from classical mechanics to quantum mechanics, replace p by the operator -i nabla (Section 14.6). Show that the quantum mechanical angular momentum operator has Cartesian components L_x = -i (y partial differential/partial differential z - z partial differential/partial differential y L_y = -i(z partial differential/partial differential x - x partial differential/partial differential z L_z = -i (x partial differential/partial differential...
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...
3 Angular Momentum and Spherical Harmonics For a quantum mechanical system that is able to rotate in 3D, one can always define a set of angular momentum operators J. Jy, J., often collectively written as a vector J. They must satisfy the commutation relations (, ] = ihſ, , Îu] = ihſ, J., ſu] = ihỈy. (1) In a more condensed notation, we may write [1,1]] = Žiheikh, i, j= 1,2,3 k=1 Here we've used the Levi-Civita symbol, defined as...