2016-02-24 20:38:17 +00:00
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Two operators' matrix representations are known in the |1〉, |2〉, |3〉 basis, where and b are real numbers:
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2016-02-25 05:03:45 +00:00
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 ≐ B̂ ≐
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⎛ a 0 0 ⎞ ⎛ b 0 0 ⎞
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⎜ 0 -a 0 ⎟ ⎜ 0 0 -ιb ⎟
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⎝ 0 0 -a ⎠ and ⎝ 0 ιb 0 ⎠.
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2016-02-24 20:38:17 +00:00
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B exhibits a degenerate spectrum when it has repeated eigenvalues. The eigenvalues of B are obtained from its characteristic equation.
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|⎛ b-λ 0 0 ⎞|
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|⎜ 0 -λ -ιb ⎟| = 0, i.e.
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|⎝ 0 ιb -λ ⎠|
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(b - λ)(λ² + ι²b²) = (b - λ)(λ² - b²) = (b - λ)(b - λ)(b + λ) = 0.
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(a) The eigenvalues for this operator are therefore λ = b,b,-b. Since b appears twice, the operator exhibits a degenerate spectrum.
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To find if A and B commute, their commutator need be evaluated. They commute if the value is 0. The commutator of two operators is defined as
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[Â,B̂] = Â B̂ - B̂ Â.
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For the given operators, then, the commutator is
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⎛ a 0 0 ⎞ ⎛ b 0 0 ⎞ ⎛ b 0 0 ⎞ ⎛ a 0 0 ⎞
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⎜ 0 -a 0 ⎟ ⎜ 0 0 -ιb ⎟ - ⎜ 0 0 -ιb ⎟ ⎜ 0 -a 0 ⎟
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⎝ 0 0 -a ⎠ ⎝ 0 ιb 0 ⎠ ⎝ 0 ιb 0 ⎠ ⎝ 0 0 -a ⎠,
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which reduces to
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2016-02-25 05:03:45 +00:00
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⎛ ab 0 0 ⎞ ⎛ ab 0 0 ⎞
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⎜ 0 0 ιab ⎟ - ⎜ 0 0 ιab ⎟ = 0.
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⎝ 0 -ιab 0 ⎠ ⎝ 0 -ιab 0 ⎠
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2016-02-24 20:38:17 +00:00
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(b) Therefore, these operators commute.
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2016-02-25 05:03:45 +00:00
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Since the operators commute, they share a set of common eigenstates. The eigenstates of  are apparent from inspection:
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|a₁〉 ≐ ⎛1⎞ |a₂〉 ≐ ⎛0⎞ and |a₃〉 ≐ ⎛0⎞
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⎜0⎟ ⎜1⎟ ⎜0⎟
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⎝0⎠, ⎝0⎠, ⎝1⎠.
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2016-02-24 20:38:17 +00:00
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The eigenvalues are already known (λ = b,b,-b.), and using the eigenvalue equations, the eigenstates can be determined. The eigenvalue equation
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2016-02-25 05:03:45 +00:00
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⎛ b 0 0 ⎞ ⎛ α₁ ⎞ ⎛ b α₁ ⎞ ⎛ α₁ ⎞
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⎜ 0 0 -ιb ⎟ ⎜ β₁ ⎟ = ⎜ -ι b γ₁ ⎟ = b ⎜ β₁ ⎟
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⎝ 0 ιb 0 ⎠ ⎝ γ₁ ⎠ ⎝ ι b β₁ ⎠ ⎝ γ₁ ⎠
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2016-02-24 20:38:17 +00:00
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2016-02-25 05:03:45 +00:00
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reveals -ι γ₁ = β₁, which, combined with the normalization condition, will allow the determination of two eigenstates of the B̂.
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2016-02-24 20:38:17 +00:00
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