Show that the operators J(+)-hat and J(-)-hat satisfy the following commutation

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SUMMARY

The discussion focuses on proving the commutation relations for the operators J(+)-hat and J(-)-hat, defined as J(+)-hat = J(x)-hat + i h-bar J(y)-hat and J(-)-hat = J(x)-hat - i h-bar J(y)-hat. Using the established commutation relations of angular momentum operators, it is shown that [J(z)-hat, J(+)-hat] = h-bar J(+)-hat and [J(z)-hat, J(-)-hat] = h-bar J(-)-hat. The calculations confirm that these operators adhere to the expected quantum mechanical behavior.

PREREQUISITES
  • Understanding of angular momentum operators in quantum mechanics
  • Familiarity with commutation relations and their significance
  • Knowledge of complex numbers and their application in quantum mechanics
  • Basic proficiency in manipulating algebraic expressions involving operators
NEXT STEPS
  • Study the derivation of angular momentum commutation relations in quantum mechanics
  • Explore the implications of J(+)-hat and J(-)-hat in quantum state transitions
  • Learn about the role of the h-bar constant in quantum mechanics
  • Investigate the applications of angular momentum operators in quantum field theory
USEFUL FOR

Quantum mechanics students, physicists specializing in angular momentum, and researchers exploring quantum operator algebra will benefit from this discussion.

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Homework Statement



The operators J(subscript x)-hat, J(subscript y)-hat and J(subscript z)-hat are Cartesian components of the angular momentum operator obeying the usual commutation relations ([J(subscript x)-hat, J(subscript y)-hat]=i h-bar J(subscript z) etc). Use these commutation relations to show that the operators J(subscript +)-hat=J(subscript x)-hat +i h-bar J(subscript y)-hat and J(subscript -)-hat=J(subscript x)-hat -i h-bar J(subscript y)-hat satisfy the following commutation relations:

[J(subscript z)-hat, J(subscript +)-hat]=h-bar J(subscript +)-hat
[J(subscript z)-hat, J(subscript -)-hat]=h-bar J(subscript -)-hat

The Attempt at a Solution



[J(z),J(+)]
=J(z)(J(x)+(i)J(y)-(J(x)+i(J(y))J(z)
=-i h-bar J(y) +(i)(-i) h-bar J(z)- i h-bar J(y) - (i)(i)h-bar J(z)
=2h-bar J(x) -2i h-bar J(y)
=2h-bar (J9x) -i J(y) =2 h-bar J(-)
 
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never mind i found the answer now
 

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