Calculating Probabilities for Quantum Spin Measurements

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SUMMARY

The discussion focuses on calculating probabilities for quantum spin measurements using Hamiltonians in a magnetic field. The Hamiltonians for the z, x, and y directions are defined as H_z = -γBcosθ1/2ħ (1 0, 0 -1), H_x = -γBsinθ1/2ħ (0 1, 1 0), and H_y = 0. Eigenvalues and eigenspinors are derived, with eigenvalues of H_z being ±γBcosθ1/2ħ and those of H_x being ±γBsinθ1/2ħ. The participant expresses confusion regarding the normalization of eigenspinors and the calculation of probabilities for subsequent measurements along different axes.

PREREQUISITES
  • Understanding of quantum mechanics, specifically spin-1/2 particles
  • Familiarity with Hamiltonian operators in quantum physics
  • Knowledge of eigenvalues and eigenspinors
  • Basic grasp of probability theory in quantum measurements
NEXT STEPS
  • Study the normalization of quantum states and eigenspinors
  • Learn about the measurement postulate in quantum mechanics
  • Explore the concept of quantum state evolution and transition probabilities
  • Investigate the role of magnetic fields in quantum spin systems
USEFUL FOR

Students and researchers in quantum mechanics, particularly those studying spin systems and quantum measurements, will benefit from this discussion.

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Homework Statement


The problem is a series of problems all relating to each other. I have gotten most of this done but I will add my answers and continue until the last part which is my main question: We choose a magnetic field in the z direction. Use your knowledge of 2-dimensional representations of 1. Sx, Sy, and Sz to express the Hamiltonian as a matrix:
My answer to this:
H_z = -γBcosθ1/2\hbar (1 0, 0 -1)
H_x = -γBsinθ1/2\hbar (0 1, 1 0 )
H_y= 0


Part 2: Find the eigenvalues and eigenspinors of the Hamiltonian matrix:
My answer to this:
Eigenvalues of H_z= \lambda=\pmγBcosθ1/2\hbar
Eigenvalues of H_x= \lambda=\pmγBsinθ1/2\hbar
Eigenvalues of H_y= 0

__________________________
Eigenspinor of Hz using those eigenvalues: [0 1] and [1 0]
Eigenspinor of Hx using those eigenvalues: [1 -1] and [1 1]
Eigenspinor of Hy using those eigenvalues: [0 0] <---what is up with all my "y" answers??


Part 3: Normalize the eigenspinors

My answer: Everything that I am doing is saying that these are already normalized? Is that not correct?

Part 4: Get back to experimental measurements. Suppose we collect the atoms that are in the state after going through the region of magnetic field described above. With what probability would a subsequent measurement of the spin in each of the following directions yield ? (The measurements are not consecutive.)
a. z-axis
b. x-axis
c. y-axis

MY answer: Here is where I am stuck.

Homework Equations



I know I have my eigenspinors for my 1/2 spin particles, I have the eigenvalues also. I know the probabilities having read multitude of experiment data on what is going on, and I know I am supposed to measure starting from ONE state, to get the result to the WANTED state.

The Attempt at a Solution


I know this is not in line with the forum guidelines but I really do mean it when I say I am dead stuck. I only know that I have to start with one state to get the other, or perhaps I am confused in this sense?
 
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Please tell us the original problem statement as originally given to you. I have no idea what you mean by H_x, H_y, and H_z.
 
vela said:
I have no idea what you mean by H_x, H_y, and H_z.
Whew! I'm glad you said that. I had no idea either. :rolleyes:
 

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