Title: Quantum Shannon Theory
1Quantum Shannon Theory
http//www.cs.mcgill.ca/patrick/QLogic2005.ppt 17
July 2005, Q-Logic Meets Q-Info
2Overview
- Part I
- What is Shannon theory?
- What does it have to do with quantum mechanics?
- Some quantum Shannon theory highlights
- Part II
- Resource inequalities
- A skeleton key
3Information (Shannon) theory
- A practical question
- How to best make use of a given communications
resource? - A mathematico-epistemological question
- How to quantify uncertainty and information?
- Shannon
- Solved the first by considering the second.
- A mathematical theory of communication 1948
The
4Quantifying uncertainty
- Entropy H(X) - ?x p(x) log2 p(x)
- Proportional to entropy of statistical physics
- Term suggested by von Neumann (more on him soon)
- Can arrive at definition axiomatically
- H(X,Y) H(X) H(Y) for independent X, Y, etc.
- Operational point of view
5Compression
Source of independent copies of X
If X is binary 0000100111010100010101100101 About
nP(X0) 0s and nP(X1) 1s
X1
X2
Xn
Can compress n copies of X to a binary string of
length nH(X)
6Quantifying information
H(X)
H(X,Y)
H(YX)
H(XY) H(X,Y)-H(Y) EYH(XYy)
I(XY) H(X) H(XY) H(X)H(Y)-H(X,Y)
7Sending information through noisy channels
Statistical model of a noisy channel
8Shannon theory provides
- Practically speaking
- A holy grail for error-correcting codes
- Conceptually speaking
- A operationally-motivated way of thinking about
correlations - Whats missing (for a quantum mechanic)?
- Features from linear structureEntanglement and
non-orthogonality
9Quantum Shannon Theory provides
- General theory of interconvertibility between
different types of communications resources
qubits, cbits, ebits, cobits, sbits - Relies on a
- Major simplifying assumption
- Computation is free
- Minor simplifying assumption
- Noise and data have regular structure
10Quantifying uncertainty
- Let ? ?x p(x) ?xih?x be a density operator
- von Neumann entropy H(?) - tr ? log ?
- Equal to Shannon entropy of ? eigenvalues
- Analog of a joint random variable
- ?AB describes a composite system A B
- H(A)? H(?A) H( trB ?AB)
11Compression
Source of independent copies of ?AB
?
?
?
A
A
A
B
B
B
Can compress n copies of B to a system of nH(B)
qubits while preserving correlations with A
Schumacher, Petz
12Quantifying information
H(A)?
H(AB)?
H(BA)?
H(AB) H(AB)-H(B)
H(AB)? 0 1 -1
Conditional entropy can be negative!
?B I/2
13Quantifying information
H(A)?
H(AB)?
H(BA)?
H(AB) H(AB)-H(B)
I(AB) H(A) H(AB) H(A)H(B)-H(AB)
0
14Data processing inequality(Strong subadditivity)
Alice
Bob
time
U
?
I(AB)?
I(AB)? I(AB)?
15Sending classical information through noisy
channels
Physical model of a noisy channel (Trace-preservi
ng, completely positive map)
16Sending classical information through noisy
channels
B n
2nH(B)
X1,X2,,Xn
17Sending quantum information through noisy
channels
Physical model of a noisy channel (Trace-preservi
ng, completely positive map)
18Entanglement and privacy More than an analogy
yy1 y2 yn
x x1 x2 xn
p(y,zx)
z z1 z2 zn
How to send a private message from Alice to Bob?
Can send private messages at rate I(XY)-I(XZ)
AC93
19Entanglement and privacy More than an analogy
?iBE U n?xi
UA-gtBE n
?xiA
How to send a private message from Alice to Bob?
Can send private messages at rate I(XA)-I(XE)
D03
20Entanglement and privacy More than an analogy
?x px1/2xiA?xiBE
UA-gtBE n
?x px1/2xiA?xiA
How to send a private message from Alice to Bob?
SW97 D03
Can send private messages at rate
I(XA)-I(XE)H(A)-H(E)
21Notions of distinguishability
Basic requirement quantum channels do not
increase distinguishability
Fidelity
Trace distance
T(?,?)?-?1
F(?,?)Tr(?1/2??1/2)1/22
F0 for perfectly distinguishable F1 for
identical
T2 for perfectly distinguishable T0 for
identical
F(?,?)max h????i2
T(?,?)2maxp(k0?)-p(k0?) where max is
over POVMS Mk
F(?(?),?(?)) F(?,?)
T(?,?) T(?(?,?(?))
Statements made today hold for both measures
22Conclusions Part I
- Information theory can be generalized to analyze
quantum information processing - Yields a rich theory, surprising conceptual
simplicity - Operational approach to thinking about quantum
mechanics - Compression, data transmission, superdense
coding, subspace transmission, teleportation
23Some references Part I Standard textbooks
Cover Thomas, Elements of information
theory. Nielsen Chuang, Quantum computation
and quantum information. (and references
therein) Part II Papers available at
arxiv.org Devetak, The private classical
capacity and quantum capacity of a quantum
channel, quant-ph/0304127 Devetak, Harrow
Winter, A family of quantum protocols,
quant-ph/0308044. Horodecki, Oppenheim
Winter, Quantum information can be
negative, quant-ph/0505062