Properties
The displacement operator is a unitary operator, and therefore obeys, where I is the identity matrix. Since, the hermitian conjugate of the displacement operator can also be interpreted as a displacement of opposite magnitude . The effect of applying this operator in a similarity transformation of the ladder operators results in their displacement.
The product of two displacement operators is another displacement operator, apart from a phase factor, has the total displacement as the sum of the two individual displacements. This can be seen by utilizing the Baker-Campbell-Hausdorff formula.
which shows us that:
When acting on an eigenket, the phase factor appears in each term of the resulting state, which makes it physically irrelevant.
Read more about this topic: Displacement Operator
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