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Which identity of the following does not hold true for Poisson bracket ?

(Where all the symbols have their usual meaning)

  • A.\([x_{i}, p_{j}] = \delta_{ij}\)
  • B.\([L_{i}, L_{j}] = \delta_{ij}\)
  • C.\([L_{i}, p_{j}] = \epsilon_{ijk}\, p_{k}\)
  • D.\([x_{i}, L_{j}] = \epsilon_{ijk}\, x_{k}\)

Answer: B

The identity that does not hold is \([L_{i}, L_{j}] = \delta_{ij}\).

The components of angular momentum do not have a Kronecker-delta bracket with each other; they form the rotation algebra:

\[ [L_{i}, L_{j}] = \epsilon_{ijk}L_{k} \]

In particular \([L_{i}, L_{i}] = 0\) for any single component, whereas \(\delta_{ii} = 1\), so the stated identity fails even for \(i = j\).

The other three are the standard results: \([x_{i}, p_{j}] = \delta_{ij}\) is the fundamental bracket, and \([L_{i}, p_{j}] = \epsilon_{ijk}p_{k}\) and \([x_{i}, L_{j}] = \epsilon_{ijk}x_{k}\) express that \(\vec{p}\) and \(\vec{r}\) transform as vectors under rotations.

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