Quantum instrument

In physics, a quantum instrument is a mathematical abstraction of a quantum measurement, capturing both the classical and quantum outputs. It combines the concepts of measurement and quantum operation.

Definition

Let 
X
be the countable set describing the outcomes of a measurement and 
\{\mathcal{E}_x \}_{x\in X}
a collection of subnormalized completely positive maps, given in such a way that the sum of all 
\mathcal{E}_x
is trace preserving, i.e. {\textstyle 
\operatorname{tr}\left(\sum_x\mathcal{E}_x(\rho)\right)=\operatorname{tr}(\rho)
} for all positive operators 
\rho
.

Now for describing a quantum measurement by a instrument 
\mathcal{I}
, the maps 
\mathcal{E}_x
are used to model the mapping from an input state 
\rho
to the outputstate of a measurement conditioned on an classical measurement outcome 
x
. Thereby the probability of measuring an specific outcome 
x
on a state 
\rho
is given by

{\displaystyle 
p(x|\rho)=\operatorname{tr}(\mathcal{E}_x(\rho))
}.

The state after a measurent with the specific outcome 
x
is given by

{\displaystyle 
\rho_x=\frac{\mathcal{E}_x(\rho)}{\operatorname{tr}(\mathcal{E}_x(\rho))}
}

If the measurement outcomes are recorded in a classical register, i.e. this can be modelled by a set of orthonormal projections {\textstyle 
|x\rangle\langle x| \in \mathcal{B}(\mathbb{C}^{|x|})
} , the action of a instrument 
\mathcal{I}
is given by an channel 
\mathcal{I}:\mathcal{B}(\mathcal{H}_1) \rightarrow \mathcal{B}(\mathcal{H}_2)\otimes \mathcal{B}(\mathbb{C}^{|x|})
with

{\displaystyle 
\mathcal{I}(\rho):=
\sum_x \mathcal{E}_x
\left( \rho\right)\otimes \vert x \rangle \langle x|
}

Here 
\mathcal{H}_1
and 
\mathcal{H}_2
are the Hilbert spaces corresponding to the input and the output quantum system of a measurement.

A quantum instrument is more general than a quantum operation because it records the outcome 
x
of which operator acted on the state. An expanded development of quantum instruments is given in quantum channel.

References

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