Degeneracy in Quantum Mechanics

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SUMMARY

Degeneracy in quantum mechanics refers to the phenomenon where multiple quantum states share the same energy level, particularly evident in systems described by the Schrödinger Equation. For instance, in a three-dimensional box, states characterized by quantum numbers (nx, ny, nz) can be degenerate, such as (2, 1, 1), (1, 2, 1), and (1, 1, 2). Bosons exhibit infinite degeneracy, allowing multiple particles to occupy the same energy state, while fermions are non-degenerate due to the Pauli exclusion principle, although they can occupy states when spin is considered. Understanding these concepts is crucial for grasping the behavior of quantum systems.

PREREQUISITES
  • Understanding of the Schrödinger Equation
  • Familiarity with quantum numbers (nx, ny, nz)
  • Knowledge of bosons and fermions
  • Basic principles of quantum mechanics
NEXT STEPS
  • Study the implications of the Pauli exclusion principle on fermionic systems
  • Explore the concept of infinite degeneracy in bosonic systems
  • Learn about the mathematical formulation of quantum states and their energy levels
  • Investigate applications of degeneracy in quantum computing and condensed matter physics
USEFUL FOR

Students of quantum mechanics, physicists, and researchers interested in the properties of quantum systems and particle statistics.

hc91
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Can anyone explain to me what Degeneracy is properly. I know its something to do with having different eigenvalues on the same energy level or something like that, but have not been able to find a good explanation in any textbooks or anywhere online. And how does something have infinite degeneracy?
 
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When you solve the Schrödinger Equation for a particular potential, you sometimes get different states that have the same energy. For example consider a particle in a 3D box. The energy is labeled by 3 quantum numbers (nx, ny, nz). The 3 numbers are equivalent so (2 1 1), (1 2 1), and (1 1 2) are three independent quantum states that have the same energy. It is said they are degenerate. Notice that because the states are linearly independent, you can have fermions at the same energy because one can occupy each on of these states (if you include spin, then two fermions can actually occupy each one of those states, so spin doubles the number of degenerate states if it does not appear in the hamiltonian.)
 

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