Entanglement Entropy, QFT and Holography
Entanglement Entropy, QFT and Holography
Or what some string theorists do nowadays? Julio Virrueta
Stony Brook University
April 5, 2017
Entanglement Entropy, QFT and Holography Or what some string - - PowerPoint PPT Presentation
Entanglement Entropy, QFT and Holography Entanglement Entropy, QFT and Holography Or what some string theorists do nowadays? Julio Virrueta Stony Brook University April 5, 2017 Entanglement Entropy, QFT and Holography Outline Introduction
Entanglement Entropy, QFT and Holography
Or what some string theorists do nowadays? Julio Virrueta
Stony Brook University
April 5, 2017
Entanglement Entropy, QFT and Holography
1
Introduction
2
Entanglement in QM
3
Entanglement in QFT
4
Entanglement in String Theory
Entanglement Entropy, QFT and Holography Introduction
Entanglement Entropy, QFT and Holography Introduction
Since it’s first proposal, Entanglement Entropy has been a topic
Validity test for quantum mechanics: Bell inequalities. Many-body quantum mechanics: Tensor networks and phase transitions. Quantum Information and Computing: Practically the whole field. QFT and String Theory
Entanglement Entropy, QFT and Holography Entanglement in QM
Entanglement Entropy, QFT and Holography Entanglement in QM
Basics of QM States and Hilbert space: |ψ = α |↑ + β |↓ ∈ H Probabilities: P(↑) = |α|2 P(↓) = |β|2 (Einstein: this is bullshit...hidden variables)
Entanglement Entropy, QFT and Holography Entanglement in QM
Multi-Body QM H = HA ⊗ HB: |ψAB =
ωij |φiA ⊗ |χjB For instance: |ψAB = 1 √ 2 (|↑, ↓ ± |↓, ↑)
Entanglement Entropy, QFT and Holography Entanglement in QM
EPR paradox If we measure the state on A and observe it to be in the state |↑ the state on B will be, with probability 1, in the state |↓, |ψAB is said to be entangled. Entangled state are such that cannot be written as: |ψAB = |ψA ⊗ |ψB (Einstein: You see? Bullshit)
Entanglement Entropy, QFT and Holography Entanglement in QM
Bell’s theorem No physical theory of local hidden variables can ever reproduce all of the predictions of quantum mechanics. Entanglement is the quintessential QM phenomena! (Eintein’s attemp to show QM is wrong... show QM is the only choice)
Entanglement Entropy, QFT and Holography Entanglement in QM
Density Matrix and Mix States For state |ψ: ρ = |ψ ψ| A generalization, mixed states: ρ =
piρi =
pi |ψi ψi| How mixed is a state? SV N = −Trρ log ρ = −
pi log pi
Entanglement Entropy, QFT and Holography Entanglement in QM
Example: binary state with p1 = p and p2 = 1 − p: SV N = −p log p − (1 − p) log(1 − p)
0.2 0.4 0.6 0.8 1.0 p 0.1 0.2 0.3 0.4 0.5 0.6 0.7 SVN
Entanglement Entropy, QFT and Holography Entanglement in QM
Entanglement Entropy Suppose H = HA ⊗ HB and ρ = |ψ ψ| Define the reduced density matrix: ρA = TrBρ |ψ = |φA ⊗ |χB ⇔ ρA = |φA φA|
Entanglement Entropy, QFT and Holography Entanglement in QM
Entangled ⇔ Mixed Define the Entanglement Entropy as: S(A) = −TrρA log ρA Some properties: S(A) = S(−A) Strong Subadditivity: S(ABC) + S(B) ≤ S(AB) + S(BC)
Entanglement Entropy, QFT and Holography Entanglement in QM
If you like this and want to know more about it: http://www.theory.caltech.edu/people/preskill/ph229/ Steven Weinberg. Lectures on quantum mechanics. 2013.
quantum-mechanical description of physical reality be considered complete? Phys. Rev., 47:777–780, May 1935.
Entanglement Entropy, QFT and Holography
(QFT and String Theory to follow)
Entanglement Entropy, QFT and Holography Entanglement in QFT
Entanglement Entropy, QFT and Holography Entanglement in QFT
Density matrix in QFT Real scalar field theory, ˆ φ( x, t). The Hilbert space is spanned by {|α(x)} ˆ φ(x) |α(x) = α(x) |α(x)
Entanglement Entropy, QFT and Holography Entanglement in QFT
Ground state functional: Φ(α) = 0|α ∼ φ(
x,0)=α( x) φ( x,−∞)=0
Dφ(x)e−SE[φ] x t α( x)
Entanglement Entropy, QFT and Holography Entanglement in QFT
Ground state density matrix: ρ = |0 0| and matrix elements: ρ(α′, α) = α′|0 0|α = Φ(α′)∗Φ(α) t α( x) α′( x)
Entanglement Entropy, QFT and Holography Entanglement in QFT
For H = HA ⊗ H ¯
A, α = αA × β ¯ A:
ρA(α′
A, αA) = TrBρ ∼
∼ φ(
x,0+)=α′
A(
x); x∈A φ( x,0−)=αA( x); x∈A
Dφ(x)e−SE[φ]
Entanglement Entropy, QFT and Holography Entanglement in QFT
t αA( x) α′
A(
x) With compact time: t αA( x) α′
A(
x)
Entanglement Entropy, QFT and Holography Entanglement in QFT
The trace is: TrρA ∼
t
Entanglement Entropy, QFT and Holography Entanglement in QFT
Entanglement and R´ enyi entropies: Evaluating S(A) = −TrρA log ρA is well... a pain in the ass. Instead: Sn(A) = 1 1 − n log Trρn
A
lim
n→1 Sn(A) = S(A)
Entanglement Entropy, QFT and Holography Entanglement in QFT
Trρn
A ∼
= Z(n) Z(1)n
Entanglement Entropy, QFT and Holography Entanglement in QFT
Entanglement entropy: S(A) = lim
n→1
1 1 − n log Z(n) Z(1)n (1)
Entanglement Entropy, QFT and Holography Entanglement in QFT
If you liked EE in QFT: Pasquale Calabrese and John L. Cardy. Entanglement entropy and quantum field theory. J.Stat.Mech., 0406:P06002, 2004. Pasquale Calabrese and John Cardy. Entanglement entropy and conformal field theory. J.Phys., A42:504005, 2009.
quantum field theory. J.Phys., A42:504007, 2009.
Entanglement Entropy, QFT and Holography Entanglement in String Theory
Entanglement Entropy, QFT and Holography Entanglement in String Theory
AdS/CFT correspondence Striking String Theory result: (Quantum) Gravity in d + 1 = Super Yang-Mills in d
Entanglement Entropy, QFT and Holography Entanglement in String Theory
String Theory QFT Type IIB Strings in AdS5 × S5 N = 4 SYM with SU(N) AdS isometries SO(4, 2) Conformal symmetry SO(4, 2) S5 isometries SO(6) R-symmetry SU(4) 32 Killing spinors 32 super-charges of N = 4
ls
4 λ = Ng2
Y M
Entanglement Entropy, QFT and Holography Entanglement in String Theory
AdS geometry Locus: −X2
−1 − X2 0 +
X2 = −L2 Coordinate patches: ds2 = L4 z2
x2 ds2 = − r2 L2 + 1
dr2
r2 L2 + 1 + r2dΩ2
Entanglement Entropy, QFT and Holography Entanglement in String Theory
Entanglement Entropy, QFT and Holography Entanglement in String Theory
Boundary conditions and sources Field equations:
φ(z, x) = 0 m2 = ∆(∆ − d) Boundary conditions: lim
z→0 φ(z, x) = z∆φ0(x)
Correlation functions: e
Entanglement Entropy, QFT and Holography Entanglement in String Theory
Holographic Entanglement Recall S(A) = lim
n→1
1 1 − n log Z(n) Z(1)n (2)
Z(n) Z(1)n =
Entanglement Entropy, QFT and Holography Entanglement in String Theory
Vacuum CFT ⇒ AdS geometry ⇒ R = −d(d+1)
L2
Green surface ⇒ 2π(n−1) angle deficit ⇒ R = 4π(1−n)δ(γA) Gravitational action: S = − 1 16πGN
4GN
ddx√g + ... = −1 − n 4GN Area(γA) + ...
Entanglement Entropy, QFT and Holography Entanglement in String Theory
Z(n) Z(1)n = ZSUGRA[γA] = exp 1 − n 4GN Area(γA)
n→1
1 1 − n 1 − n 4GN Area(γA)
Entanglement Entropy, QFT and Holography Entanglement in String Theory
S(A) = 1 4GN Area(γA) z γA A ¯ A CFTd AdSd+1
Entanglement Entropy, QFT and Holography Entanglement in String Theory
If you remember something from this talk, let’s that be: Entanglement ⇔ Minimal Surface Or even better: QFT Information ⇔ Geometrical information
Entanglement Entropy, QFT and Holography Entanglement in String Theory
Current problem and research opportunities: EE for dynamical spacetime (time dependent entanglement) Higher Curvature corrections EE for gauge and chiral theories Beyond EE: Geometrization of QFT (Kinematic Space) AdS/MERA
Entanglement Entropy, QFT and Holography Entanglement in String Theory
If you like... AdS/CFT
Phys.Rept.323:183-386,2000 Edward Witten. Anti-de Sitter space and holography. Adv.Theor.Math.Phys., 2:253–291, 1998. Eric D’Hoker, Daniel Z. Freedman. Supersymmetric Gauge Theories and the AdS/CFT Correspondence. UCLA/02/TEP/3, MIT-CTP-3242
Entanglement Entropy, QFT and Holography Entanglement in String Theory
Or Holographic EE Shinsei Ryu and Tadashi Takayanagi. Aspects of Holographic Entanglement Entropy. JHEP, 0608:045, 2006. Veronika E. Hubeny. Extremal surfaces as bulk probes in AdS/CFT. JHEP, 1207:093, 2012 Matthew Headrick and Tadashi Takayanagi. A Holographic proof of the strong subadditivity of entanglement entropy. 10.1103/PhysRevD.76.106013
Entanglement Entropy, QFT and Holography
Note: When the speaker is a overly large mexican, courtesy demands to offer him a beer.