Typical subspace: Difference between revisions
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{{short description|Term in quantum information theory}} |
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In [[quantum information theory]], the idea of a '''typical subspace''' plays an important role in the proofs of many coding theorems (the most prominent example being [[Schumacher compression]]). Its role is analogous to that of the [[typical set]] in classical [[information theory]]. |
In [[quantum information theory]], the idea of a '''typical subspace''' plays an important role in the proofs of many coding theorems (the most prominent example being [[Schumacher compression]]). Its role is analogous to that of the [[typical set]] in classical [[information theory]]. |
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== Unconditional |
== Unconditional quantum typicality == |
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Consider a [[density operator]] <math>\rho</math> with the following [[spectral decomposition]]: |
Consider a [[density operator]] <math>\rho</math> with the following [[decomposition of spectrum (functional analysis)|spectral decomposition]]: |
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:<math> |
:<math> |
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\rho=\sum_{x}p_{X} |
\rho=\sum_{x}p_{X}( x) \vert x\rangle \langle |
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x |
x\vert . |
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</math> |
</math> |
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The weakly typical subspace is defined as the span of all vectors such that |
The weakly typical subspace is defined as the span of all vectors such that |
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the sample entropy <math>\overline{H} |
the sample entropy <math>\overline{H}( x^{n}) </math> of their classical |
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label is close to the true [[entropy]] <math>H |
label is close to the true [[entropy]] <math>H( X) </math> of the [[distribution (mathematics)|distribution]] |
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<math>p_{X} |
<math>p_{X}( x) </math>: |
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:<math> |
:<math> |
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T_{\delta}^{X^{n}}\equiv\text{span}\left\{ \left\vert x^{n}\right\rangle |
T_{\delta}^{X^{n}}\equiv\text{span}\left\{ \left\vert x^{n}\right\rangle |
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:\left\vert \overline{H} |
:\left\vert \overline{H}( x^{n}) -H( X) \right\vert |
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\leq\delta\right\} , |
\leq\delta\right\} , |
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</math> |
</math> |
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where |
where |
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:<math> |
:<math> |
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\overline{H} |
\overline{H}( x^{n}) \equiv-\frac{1}{n}\log( p_{X^{n} |
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} |
}( x^{n}) ) ,</math> |
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:<math>H |
:<math>H( X) \equiv-\sum_{x}p_{X}( x) \log p_{X}( |
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x |
x) .</math> |
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The [[projection (linear algebra)|projector]] <math>\Pi_{\rho,\delta}^{n}</math> onto the typical subspace of <math>\rho</math> is |
The [[projection (linear algebra)|projector]] <math>\Pi_{\rho,\delta}^{n}</math> onto the typical subspace of <math>\rho</math> is |
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defined as |
defined as |
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:<math> |
:<math> |
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\Pi_{\rho,\delta}^{n}\equiv\sum_{x^{n}\in T_{\delta}^{X^{n}}} |
\Pi_{\rho,\delta}^{n}\equiv\sum_{x^{n}\in T_{\delta}^{X^{n}}}\vert |
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x^{n} |
x^{n}\rangle \langle x^{n}\vert , |
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</math> |
</math> |
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where we have "overloaded" the symbol |
where we have "overloaded" the symbol |
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:<math> |
:<math> |
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T_{\delta}^{X^{n}}\equiv\left\{ x^{n}:\left\vert \overline{H}\left( |
T_{\delta}^{X^{n}}\equiv\left\{ x^{n}:\left\vert \overline{H}\left( |
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x^{n}\right) -H |
x^{n}\right) -H( X) \right\vert \leq\delta\right\} . |
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</math> |
</math> |
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The three important properties of the typical projector are as follows: |
The three important properties of the typical projector are as follows: |
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:<math>\text{Tr}\left\{ \Pi_{\rho,\delta}^{n}\right\} \leq2^{n\left[ H\left( |
:<math>\text{Tr}\left\{ \Pi_{\rho,\delta}^{n}\right\} \leq2^{n\left[ H\left( |
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X\right) +\delta\right] },</math> |
X\right) +\delta\right] },</math> |
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:<math>2^{-n\left[ H |
:<math>2^{-n\left[ H( X) +\delta\right] }\Pi_{\rho,\delta}^{n} |
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\leq\Pi_{\rho,\delta}^{n}\rho^{\otimes n}\Pi_{\rho,\delta}^{n}\leq2^{-n\left[ |
\leq\Pi_{\rho,\delta}^{n}\rho^{\otimes n}\Pi_{\rho,\delta}^{n}\leq2^{-n\left[ |
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H |
H( X) -\delta\right] }\Pi_{\rho,\delta}^{n},</math> |
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where the first property holds for arbitrary <math>\epsilon,\delta>0</math> and |
where the first property holds for arbitrary <math>\epsilon,\delta>0</math> and |
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sufficiently large <math>n</math>. |
sufficiently large <math>n</math>. |
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== Conditional |
== Conditional quantum typicality == |
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Consider an ensemble <math>\left\{ p_{X} |
Consider an ensemble <math>\left\{ p_{X}( x) ,\rho_{x}\right\} |
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_{x\in\mathcal{X}}</math> of states. Suppose that each state <math>\rho_{x}</math> has the |
_{x\in\mathcal{X}}</math> of states. Suppose that each state <math>\rho_{x}</math> has the |
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following [[spectral decomposition]]: |
following [[decomposition of spectrum (functional analysis)|spectral decomposition]]: |
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:<math> |
:<math> |
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\rho_{x}=\sum_{y}p_{Y|X} |
\rho_{x}=\sum_{y}p_{Y|X}( y|x) \vert y_{x}\rangle |
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\langle y_{x}\vert . |
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</math> |
</math> |
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Consider a [[density operator]] <math>\rho_{x^{n}}</math> which is conditional on a classical |
Consider a [[density operator]] <math>\rho_{x^{n}}</math> which is conditional on a classical |
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We define the weak conditionally typical subspace as the span of vectors |
We define the weak conditionally typical subspace as the span of vectors |
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(conditional on the sequence <math>x^{n}</math>) such that the sample conditional entropy |
(conditional on the sequence <math>x^{n}</math>) such that the sample conditional entropy |
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<math>\overline{H} |
<math>\overline{H}( y^{n}|x^{n}) </math> of their classical labels is close |
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to the true [[conditional entropy]] <math>H |
to the true [[conditional entropy]] <math>H( Y|X) </math> of the [[distribution (mathematics)|distribution]] |
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<math>p_{Y|X} |
<math>p_{Y|X}( y|x) p_{X}( x) </math>: |
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:<math> |
:<math> |
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T_{\delta}^{Y^{n}|x^{n}}\equiv\text{span}\left\{ \left\vert y_{x^{n}} |
T_{\delta}^{Y^{n}|x^{n}}\equiv\text{span}\left\{ \left\vert y_{x^{n}} |
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^{n}\right\rangle :\left\vert \overline{H} |
^{n}\right\rangle :\left\vert \overline{H}( y^{n}|x^{n}) |
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-H |
-H( Y|X) \right\vert \leq\delta\right\} , |
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</math> |
</math> |
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where |
where |
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:<math> |
:<math> |
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\overline{H} |
\overline{H}( y^{n}|x^{n}) \equiv-\frac{1}{n}\log\left( |
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p_{Y^{n}|X^{n}} |
p_{Y^{n}|X^{n}}( y^{n}|x^{n}) \right) ,</math> |
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:<math>H |
:<math>H( Y|X) \equiv-\sum_{x}p_{X}( x) \sum_{y} |
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p_{Y|X} |
p_{Y|X}( y|x) \log p_{Y|X}( y|x) . |
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</math> |
</math> |
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The [[projection (linear algebra)|projector]] <math>\Pi_{\rho_{x^{n}},\delta}</math> onto the weak conditionally typical |
The [[projection (linear algebra)|projector]] <math>\Pi_{\rho_{x^{n}},\delta}</math> onto the weak conditionally typical |
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:<math> |
:<math> |
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\Pi_{\rho_{x^{n}},\delta}\equiv\sum_{y^{n}\in T_{\delta}^{Y^{n}|x^{n}} |
\Pi_{\rho_{x^{n}},\delta}\equiv\sum_{y^{n}\in T_{\delta}^{Y^{n}|x^{n}} |
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} |
}\vert y_{x^{n}}^{n}\rangle \langle y_{x^{n}}^{n}\vert , |
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</math> |
</math> |
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where we have again overloaded the symbol <math>T_{\delta}^{Y^{n}|x^{n}}</math> to refer |
where we have again overloaded the symbol <math>T_{\delta}^{Y^{n}|x^{n}}</math> to refer |
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:<math> |
:<math> |
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T_{\delta}^{Y^{n}|x^{n}}\equiv\left\{ y^{n}:\left\vert \overline{H}\left( |
T_{\delta}^{Y^{n}|x^{n}}\equiv\left\{ y^{n}:\left\vert \overline{H}\left( |
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y^{n}|x^{n}\right) -H |
y^{n}|x^{n}\right) -H( Y|X) \right\vert \leq\delta\right\} . |
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</math> |
</math> |
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The three important properties of the weak conditionally typical projector are |
The three important properties of the weak conditionally typical projector are |
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\rho_{X^{n}}\right\} \right\} \geq1-\epsilon,</math> |
\rho_{X^{n}}\right\} \right\} \geq1-\epsilon,</math> |
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:<math>\text{Tr}\left\{ \Pi_{\rho_{x^{n}},\delta}\right\} \leq2^{n\left[ |
:<math>\text{Tr}\left\{ \Pi_{\rho_{x^{n}},\delta}\right\} \leq2^{n\left[ |
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H |
H( Y|X) +\delta\right] },</math> |
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:<math>2^{-n\left[ H |
:<math>2^{-n\left[ H( Y|X) +\delta\right] }\ \Pi_{\rho_{x^{n}} |
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,\delta} \leq\Pi_{\rho_{x^{n}},\delta}\ \rho_{x^{n}}\ \Pi_{\rho_{x^{n} |
,\delta} \leq\Pi_{\rho_{x^{n}},\delta}\ \rho_{x^{n}}\ \Pi_{\rho_{x^{n} |
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},\delta} \leq2^{-n\left[ H |
},\delta} \leq2^{-n\left[ H( Y|X) -\delta\right] }\ \Pi |
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_{\rho_{x^{n}},\delta}, |
_{\rho_{x^{n}},\delta}, |
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</math> |
</math> |
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where the first property holds for arbitrary <math>\epsilon,\delta>0</math> and |
where the first property holds for arbitrary <math>\epsilon,\delta>0</math> and |
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sufficiently large <math>n</math>, and the expectation is with respect to the |
sufficiently large <math>n</math>, and the expectation is with respect to the |
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distribution <math>p_{X^{n}} |
distribution <math>p_{X^{n}}( x^{n}) </math>. |
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== See also == |
== See also == |
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== References == |
== References == |
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* Wilde, Mark M., 2017, [http://www.cambridge.org/us/academic/subjects/computer-science/cryptography-cryptology-and-coding/quantum-information-theory-2nd-edition Quantum Information Theory, Cambridge University Press], Also available at [https://arxiv.org/abs/1106.1445 eprint arXiv:1106.1145] |
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* Mark M. Wilde, [http://arxiv.org/abs/1106.1445 "From Classical to Quantum Shannon Theory", arXiv:1106.1445]. |
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{{Quantum computing}} |
{{Quantum computing}} |
Latest revision as of 00:33, 15 May 2021
In quantum information theory, the idea of a typical subspace plays an important role in the proofs of many coding theorems (the most prominent example being Schumacher compression). Its role is analogous to that of the typical set in classical information theory.
Unconditional quantum typicality
[edit]Consider a density operator with the following spectral decomposition:
The weakly typical subspace is defined as the span of all vectors such that the sample entropy of their classical label is close to the true entropy of the distribution :
where
The projector onto the typical subspace of is defined as
where we have "overloaded" the symbol to refer also to the set of -typical sequences:
The three important properties of the typical projector are as follows:
where the first property holds for arbitrary and sufficiently large .
Conditional quantum typicality
[edit]Consider an ensemble of states. Suppose that each state has the following spectral decomposition:
Consider a density operator which is conditional on a classical sequence :
We define the weak conditionally typical subspace as the span of vectors (conditional on the sequence ) such that the sample conditional entropy of their classical labels is close to the true conditional entropy of the distribution :
where
The projector onto the weak conditionally typical subspace of is as follows:
where we have again overloaded the symbol to refer to the set of weak conditionally typical sequences:
The three important properties of the weak conditionally typical projector are as follows:
where the first property holds for arbitrary and sufficiently large , and the expectation is with respect to the distribution .
See also
[edit]References
[edit]- Wilde, Mark M., 2017, Quantum Information Theory, Cambridge University Press, Also available at eprint arXiv:1106.1145