Capacity of quantum channels from subfactors Pieter Naaijkens - - PowerPoint PPT Presentation

capacity of quantum channels from subfactors
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Capacity of quantum channels from subfactors Pieter Naaijkens - - PowerPoint PPT Presentation

Capacity of quantum channels from subfactors Pieter Naaijkens Universidad Complutense de Madrid 8 May 2019 This work was funded by the ERC (grant agreement No 648913) Infinite quantum systems Quantum systems with infinitely many d.o.f.:


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This work was funded by the ERC (grant agreement No 648913)

Capacity of quantum channels from subfactors

Pieter Naaijkens Universidad Complutense de Madrid 8 May 2019

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Infinite quantum systems

Can we do quantum information?

Quantum systems with infinitely many d.o.f.: Quantum field theory Systems in thermodynamic limit… e.g. quantum spin systems with topological order

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Infinite quantum systems

Take an operator algebraic approach

E.g.: infinitely many spins: Superselection sectors Stone-von Neumann uniqueness

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Outline

Classical information theory Subfactors and QI Von Neumann algebras

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Von Neumann algebras

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Von Neumann algebras

*-subalgebra and closed in norm Equivalent definition: It is a von Neumann algebra if closed in w.o.t.: A factor Can be classified into Type I, Type II, Type III

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Normal states

with A state is a positive linear functional Normal if

If a factor is not of Type I, there are no normal pure states

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Quantum information

work mainly in the Heisenberg picture

  • bservables modelled by von Neumann algebra

consider normal states on channels are normal unital CP maps Araki relative entropy

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use quantum systems to communicate main question: how much information can I transmit? will consider infinite systems here… … described by subfactors channel capacity is given by Jones index

Quantum information

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Classical wiretapping channels

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Image source: Alfred Eisenstaedt/The LIFE Picture Collection

Information theory Alice wants to communicate with Bob using a noisy channel. How much information can Alice send to Bob per use of the channel?

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Setup

Alice Bob input space

  • utput space

How well can Bob recover the messages sent by Alice (small error allowed)?

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Relative entropy

Compare two probability distributions P, Q: Vanishes iff P=Q, otherwise positive

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Mutual information

`information’ due to noise here the conditional entropy is defined: some algebra gives:

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Operational approach

encode n channels N messages decode Maximum error for all possible encodings:

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Coding theorem

Def: R is called an achievable rate if The supremum of all R is called the capacity C. Theorem: the capacity is the Shannon capacity

  • f the channel, defined as:

This is a single-letter formula!

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Wiretapping channels

Alice Bob Eve

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Quantum information

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Distinguishing states Alice prepares a mixed state : …and sends it to Bob Can Bob recover ?

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Holevo 𝜓 quantity In general not exactly: Generalisation of Shannon information

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Araki relative entropy

Let be faithful normal states: Def: Def:

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Infinite systems

Suppose is an infinite factor, say Type III, and a faithful normal state where

Better to compare algebras!

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Subfactors

A subfactor is an inclusion of factors It is irreducible if The Jones index gives the “relative size”

Jones, Invent. Math. 72 (1983) Kosaki, J. Funct. Anal. 66 (1986) Longo, Comm. Math. Phys. 126 (1989)

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A quantum channel

For finite index inclusion , say irreducible, quantum channel, describes the restriction of operations

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Comparing algebras

Want to compare and , with subfactor Shirokov & Holevo, arXiv:1608.02203

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Jones index and entropy

gives an information-theoretic interpretation to the Jones index

Hiai, J. Operator Theory, ’90; J. Math. Soc. Japan, ‘91

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Quantum wiretapping

Alice Bob Eve

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Theorem (Devetak, Cai/Winter/Yeung) The rate of a wiretapping channel is given by

lim

n→∞

1 n max

{px,ρx}

  • χ({px}, Φ⊗n

B (ρx)}) − χ({px}, Φ⊗n E (ρx)})

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A conjecture

The Jones index of a subfactor gives the classical capacity of the wiretapping channel that restricts from to .

[M : N] M N

  • L. Fiedler, PN, T.J. Osborne, New J. Phys 19:023039 (2017)

PN, Contemp. Math. 717, pp. 257-279 (2018), arXiv:1704.05562

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Some remarks

use entropy formula by Hiai together with properties of the index averaging drops out: single letter formula coding theorem is missing

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RAB = RA ∨ RB RA = π0(A(A))00 RB

b RAB = π0(A((A ∪ B)c))0

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Locality: RAB ⊂ b RAB but: RAB $ b RAB