Coherent states are quasi-classical states that may be defined in different ways, for instance as eigenstates of the annihilation operator
a | α ⟩ = α | α ⟩ {\displaystyle a|\alpha \rangle =\alpha |\alpha \rangle } , or as a displacement from the vacuum
| α ⟩ = D ( α ) | 0 ⟩ {\displaystyle |\alpha \rangle =D(\alpha )|0\rangle } , where D ( α ) = exp ( α a † − α ∗ a ) {\displaystyle D(\alpha )=\exp(\alpha a^{\dagger }-\alpha ^{*}a)} is the Sudarshan-Glauber displacement operator. One may think of a non-linear coherent state by generalizing the annihilation operator:
A = a f ( a † a ) {\displaystyle A=af(a^{\dagger }a)} , and then using any of the above definitions by exchanging a {\displaystyle a} by A {\displaystyle A} . The above definition is also known as an f {\displaystyle f} -deformed annihilation operator.
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