possible states for identicle particles are (2,2) (2,-2) (2,0) (1,1) (1,-1) (1,0) (0,0) (2,1) (2,-1)
Exercise 8.3 (a) Write down all possible states of two nonidentical particles of spin 1 (i.e.,...
For a system of two particles with spin 3/2 and 1/2 write out all the possible |j1m1> x |j2m2> states. how many states should exist?
Problem2 Two possible wave functions for two spin 1 /2 particles with Sz = 0 are Apply the operator S+ to both states as many times as needed to find the largest possible value for m and hence determine the value of S2 for each state Problem2 Two possible wave functions for two spin 1 /2 particles with Sz = 0 are Apply the operator S+ to both states as many times as needed to find the largest possible value...
System A consists of two spin-1/2 particles, and has a four-dimensional Hilbert space. 1. Write down a basis for the Hilbert space of two spin-1/2 particles. 2. Calculate the matrix of the angular momentum operator, Sfot = (ŜA, ŠA, ŜA) for system A, in the basis of question 4A.1, and express them in this basis. 3. Calculate the square of the total angular momentum of system A , Spotl?, and express this operator in the basis of question 4A.1. 4....
2. Addition of Angular Momentum a) (8pts) Given two spin 1/2 particles, what are the four possibilities for their spin configuration? Put your answer in terms of states such as | 11). where the first arrow denotes the z-component of the particle's spin. Identify the m values for each state. b)(7pts) If you apply the lowering operator to a state you get Apply the two-state lowering operator S--S(,) +S(), where sti) acts on the first state and S acts on...
Consider one dimensional lattice of N particles having a spin of 1 /2 with an associated magnetic moment μ The spins are kept in a magnetic field with magnetic induction B along the z direction. The spin can point either up, t, or down, , relative to the z axis. The energy of particle with spin down is e B and that of particle with spin up is ε--B. We assume that the system is isolated from. its environment so...
Exercise 1: addition of angular momentum a) Explicitly construct the states of total spin for a system of two spin-z particles b) Use the table (given below) to verify the Clebsch-Gordan coefficients c) Construct the 1, 12;1, m) 1, 1;0, 0) state explicitly and by using the table Table 1: Clebsch-Gordan coefficients (1,mi, m2ljm) m2 =- ji 2 131-m+ Table 2: Clebsch-Gordan coefficients (j1,1;m, m2jm) m20 1-m+1)01+m+1 2j1101+ j11 (21 +1) (21+2) 71 231 (ว่า+ (31+ (1-m)1-m+1)12 Exercise 1: addition...
(14 points) Write Slater determinants for all possible spin states of the first excited state of He (one electron in the 1s orbital, the other in the 2s orbital). Indicate the S (sum of all e spins) and Ms (vector sum of e spins) values of the corresponding wavefunctions. Evaluate the Slater determinants to obtain the total wavefunctions we wrote in class. Hint: The wavefunctions with σ (1,2) and σ (1,2) require two Slater determinants to correctly represent them.
If the spin angular momenta of two spin-1 particles are added, the possible m valnes for the z-component of the total spin angular momentum (such that Š ) m)are a) m=-1,0, or 1 b) m= c) m=2.0, or-2 d) m--2-3/2,-1,-1/2, 0, 1/2, 1, 3/2, or2 e) m 2, 1, or f) none of the above 2,1, 0,1, or 2
A proton has tWo posslble spins States, spin up With energies e+ and Spin down with energies e e+ is positive and e. is negative. The spin partition function for a collection of N non-interacting spins is kTexp Show All Your Work! a) Derive the expression for b) As the temperature, T, of the system decreases, the average energy decreases. Why is that? (E)-- In(QCN, V, β)] Cv aP эт
Exercise 1: addition of angular momentum a) Explicitly construct the states of total spin for a system of two spin-^ particles b) Use the table (given below) to verify the Clebsch-Gordan coefficients c) Construct the , 12;l, m)- 1,1;0,0) state explicitly and by using the table Table 1: Clebsch-Gordan coefficients (ji, 1, m2ljm) m2 =- Clebsch-Gordan coefficients 〈J1, 1; m1, m2|JM》 Table 2: 1 +1 71 2j1i+ 1-m)(i-m+1 2j1 (2j1+1 2j1 (2j1+ 11 (21+