Sakurai 1.17 - Operators and Complete Eigenkets

In summary, the problem is about two observables, A_1 and A_2, that do not commute but both commute with the Hamiltonian. The goal is to prove that the energy eigenstates are generally degenerate, with the exception of possible energy eigenstates that are not degenerate. The attempt at a solution involves using the fact that A_1 and H share complete eigenkets, as do A_2 and H. However, generally, two observables that do not commute do not have shared eigenkets. The question then asks if there are exceptions to this, meaning there could be energy eigenstates that are not degenerate.
  • #1
Domnu
178
0
I'm pretty sure this is correct, but could someone verify for rigor?

Problem
Two observables [tex]A_1[/tex] and [tex]A_2[/tex], which do not involve time explicitly, are known not to commute, yet we also know that [tex]A_1[/tex] and [tex]A_2[/tex] both commute with the Hamiltonian. Prove that the energy eigenstates are, in general, degenerate. Are there exceptions?

The attempt at a solution
Since [tex][H,A_1]=0[/tex], we know that there are complete eigenkets that [tex]A_1[/tex] and [tex]H[/tex] share. The same is true for [tex]A_2[/tex]. Now, generally, two observables that do not commute do not share eigenkets. Thus, we know that there exist two distinct eigenstates such that [tex]H|a\ket = e|a\ket[/tex]; particularly, each [tex]|a\ket[/tex] can be brought from the eigenkets of [tex]A_1,A_2[/tex].
 
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  • #2
come on 25 views and no post? :(
 
  • #3
Impatience is not a virtue. Can't A1 and A2 commute on a subspace without commuting on the whole space?
 
  • #4
Heh, it was more of a bump since it was already on the second page :) Yes, they can, but the question asks "generally," and "generally" this doesn't happen, right?
 
  • #5
Ok, considered as a teasing bump. But the question asks, are there exceptions? I.e. could there be energy eigenstates that aren't degenerate? At least that's how I read it.
 

Related to Sakurai 1.17 - Operators and Complete Eigenkets

1. What is Sakurai 1.17?

Sakurai 1.17 is a reference to the 17th chapter of the textbook "Modern Quantum Mechanics" written by physicist Jun John Sakurai. It covers the topic of operators and complete eigenkets in quantum mechanics.

2. What are operators in quantum mechanics?

Operators in quantum mechanics are mathematical tools used to describe the behavior and properties of quantum systems. They represent physical observables such as position, momentum, and energy, and they act on quantum states to produce measurable results.

3. What are complete eigenkets?

Complete eigenkets are a set of eigenvectors of a Hermitian operator that form a basis for the Hilbert space of a quantum system. They represent the possible states of the system and can be used to express any state of the system as a linear combination of these eigenkets.

4. Why are operators and complete eigenkets important in quantum mechanics?

Operators and complete eigenkets are fundamental concepts in quantum mechanics and are essential for understanding and predicting the behavior of quantum systems. They allow us to calculate the probabilities of different outcomes for measurements and to describe the evolution of quantum states over time.

5. How can operators and complete eigenkets be applied in real-world situations?

Operators and complete eigenkets can be applied in a wide range of real-world situations, including the study of atomic and molecular systems, the behavior of subatomic particles, and the development of quantum technologies such as quantum computing and cryptography. They also have applications in fields such as chemistry, materials science, and engineering.

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