Role of hermitian and unitary operators in QM

Click For Summary
SUMMARY

Hermitian and unitary operators play crucial roles in quantum mechanics (QM). Observables must be represented by hermitian operators to ensure that eigenvalues, which correspond to measurable values, are real. For any hermitian operator O, a family of unitary operators U(s) = exp(iOs) can be constructed, which act as symmetries in Hilbert space. Notably, the creation and annihilation operators of the harmonic oscillator, as well as ladder operators for angular momentum, are examples of operators that are neither hermitian nor unitary.

PREREQUISITES
  • Understanding of hermitian operators in quantum mechanics
  • Familiarity with unitary operators and their properties
  • Knowledge of Hilbert space concepts
  • Basic principles of quantum observables and eigenvalues
NEXT STEPS
  • Study the mathematical properties of hermitian operators in quantum mechanics
  • Explore the role of unitary operators in quantum state transformations
  • Learn about the significance of the Hamiltonian operator in time evolution
  • Investigate the applications of creation and annihilation operators in quantum field theory
USEFUL FOR

Quantum physicists, students of quantum mechanics, and researchers interested in the mathematical foundations of quantum theory will benefit from this discussion.

Inam
Messages
2
Reaction score
0
Which is the role of hermitian and unitary operators in quantum mechanics and which operator is neither hermitian nor unitary
 
Physics news on Phys.org
Observables must be hermitian operators b/c we associate experimental measurable values with eigenvalues, therefore eigenvalues must be real - which is ensured by hermitian operators.

For every hermitian operator O you can construct a family of unitary operators U(s) = exp(iOs) with a real parameter s. These U(s) may be symmetries which act on Hilbert space states as unitary operators. One example is a hermitian angular momentum operator Li which generates rotations w.r.t. to the i-axis. A special case are time translations which are generated by the hermitian Hamiltonian H, i.e. U(t) = exp(iHt).

Important operators which are neither hermitian nor unitary are a) the creation and annihilation operators of the harmonic oscillator and b) the ladder operators for angular momentum.
 
Thanks Tom
 

Similar threads

  • · Replies 15 ·
Replies
15
Views
880
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 24 ·
Replies
24
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 63 ·
3
Replies
63
Views
8K
  • · Replies 22 ·
Replies
22
Views
2K