
Displacement operator
Encyclopedia
The displacement operator for one mode in quantum optics
is the operator
,
where
is the amount of displacement in optical phase space
,
is the complex conjugate of that displacement, and
and
are the lowering and raising operators
, respectively.
The name of this operator is derived from its ability to displace a localized state in phase space by a magnitude
. It may also act on the vacuum state by displacing it into a coherent state
. Specifically,
where
is a coherent state.
Displaced states are eigenfunctions of the annihilation (lowering) 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.


Quantum optics
Quantum optics is a field of research in physics, dealing with the application of quantum mechanics to phenomena involving light and its interactions with matter.- History of quantum optics :...
is the operator

where

Optical phase space
In quantum optics, an optical phase space is a phase space in which all quantum states of an optical system are described. Each point in the optical phase space corresponds to a unique state of an optical system. For any such system, a plot of the quadratures against each other, possibly as...
,



Creation and annihilation operators
Creation and annihilation operators are mathematical operators that have widespread applications in quantum mechanics, notably in the study of quantum harmonic oscillators and many-particle systems. An annihilation operator lowers the number of particles in a given state by one...
, respectively.
The name of this operator is derived from its ability to displace a localized state in phase space by a magnitude

Coherent state
In quantum mechanics a coherent state is a specific kind of quantum state of the quantum harmonic oscillator whose dynamics most closely resembles the oscillating behaviour of a classical harmonic oscillator...
. Specifically,


Displaced states are eigenfunctions of the annihilation (lowering) operator.
Properties
The displacement operator is a unitary operatorUnitary operator
In functional analysis, a branch of mathematics, a unitary operator is a bounded linear operator U : H → H on a Hilbert space H satisfyingU^*U=UU^*=I...
, and therefore obeys

where I is the identity matrix. Since




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

Alternative expressions
Two alternative ways to express the displacement operator are:
