EPR Pairs, Lo Local Projection and Quantum Tele leportation in - - PowerPoint PPT Presentation

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EPR Pairs, Lo Local Projection and Quantum Tele leportation in - - PowerPoint PPT Presentation

Strings and Fields 2016, 2016/08/10 @ YITP, Kyoto EPR Pairs, Lo Local Projection and Quantum Tele leportation in Holography in Kento Watanabe (YITP, Kyoto) arXiv: 1604.01772 [hep-th] with Tokiro Numasawa (YITP -> KITP) Noburo


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SLIDE 1

Kento Watanabe (YITP, Kyoto)

Tokiro Numasawa Noburo Shiba Tadashi Takayanagi arXiv: 1604.01772 [hep-th] (YITP -> Harvard U) (YITP) (YITP -> KITP)

EPR Pairs, Lo Local Projection and Quantum Tele leportation in in Holography

with

Strings and Fields 2016, 2016/08/10 @ YITP, Kyoto

(will appear in JHEP)

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SLIDE 2

motivated by Quantum Information theory

Entanglement Measures & Related Phenomena

Hot topics in QFT & its Holographic Dual

Big Collaboration !! Big Workshop !!

EE, MI, Relative Entropy, Negativity, Complexity, Information metric Scrambling, Quantum Error Correction, Distillation …

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SLIDE 3

motivated by Quantum Information theory

Entanglement Measures & Related Phenomena Quantum Operations

Hot topics in QFT & its Holographic Dual However, so far, NOT investigated well in QFT & Holography ….

Big Collaboration !! Big Workshop !!

EE, MI, Relative Entropy, Negativity, Complexity, Information metric Scrambling, Quantum Error Correction, Distillation …

How about Operational Aspects ?

Also important in many quantum process

  • r protocols

in QI

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SLIDE 4

‘s

Example : : Quantum Tele leportation in in QM

sends ’s qubit to Projection measurement on & Protocol : Classically communication between & Appropriate unitary operation to Finally, can obtain the same qubit as Task : The protocol consists of LOCCs Local Operations & Classical Communications

[Bennet et al ‘93]

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SLIDE 5

Let’s Try 3 Quantum Operations !!

Partial Entangling

Partially exchange two CFTs (also EPR pairs) Partially project out a CFT

Vol (operated region)

(Can) Reduce EE

??

Partial Swapping

Partially prepare EPR pairs between two CFTs

Entangled

Local (Partial) Projection

Swapped Projected to products Focus on

(# of EPR pairs crossing the edges)

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SLIDE 6

Let’s Try 3 Quantum Operations !!

Partial Entangling

Partially exchange two CFTs (also EPR pairs) Partially project out a CFT

Vol (operated region)

(Can) Reduce EE

??

Partial Swapping

Partially prepare EPR pairs between two CFTs

Entangled

Local (Partial) Projection

Swapped Projected to products

“Quantum Teleportation” QFT Analog & Holographic Dual of

Focus on

(# of EPR pairs crossing the edges)

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SLIDE 7

Entangling & & S Swapping between tw two CFT FTs

Path-Integral Pictures EEs after these operations

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SLIDE 8

Path th-Integral Pict ictures: En Entangli ling

Entangled

Path-integral picture for density matrix:

Entangling

( cf: replica method, TFD state )

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SLIDE 9

En Entangle lement En Entr tropy aft fter En Entangli ling

Non-contractive for solid torus Volume of the region we operated EE between two CFTs

Conformal Map

Torus with period

BTZ BH Dual

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SLIDE 10

Path th-Integral Pict ictures: Swappin ing

Path-integral picture for density matrix: Swapping

( cf: replica method, TFD state )

Swapped

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SLIDE 11

Entan anglement Entr tropy aft fter er Swap apping

Contractive for solid torus EE between two CFTs # of EPR pairs crossing the edges

Conformal Map

Different cycle as Entangling

Torus

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SLIDE 12

Lo Local Projection Measurement in in a CFT FT

Path-Integral Pictures EEs after the operation Local Projection as Boundary State

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SLIDE 13

Lo Local l Projection desc scribed by y Bou

  • undary

ry States

Local (Partial) Projection

Local Projection can be described by Boundary States No real space entanglement [Miyaji-Ryu-Takayanagi-Wen ‘14] No real space entanglement at each point in Factrization of n-pt function on Conformal Boundary states close each other

[Rajabpour‘15]

More generally,

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SLIDE 14

Path th-Integral Pict ictures: Loc

  • cal Proje
  • jectio

ion

[Rajabpour‘15] 1 interval jointed with 1-cut

: UV cut-off : Boundary entropy (ignore in this talk) UHP with a twist operator

Its Dual Picture [ Takayanagi’11] [ Fujita-Tonii-Takayanagi’11]

AdS/BCFT : Minimal Geodesic

Dual

: Totally Geodesic Surface

(ignore the tension in this talk)

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SLIDE 15

2-cu cuts, 1-dis isjo joint in inter erval al an and Tim Time-evolutions

Cylinder

Identify

Annulus

Identify

Half of Torus Half of BTZ BH Dual

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SLIDE 16

Ex Exam ample le: EE EE in in 2D Fr Free ee Fer ermio ion CFT FT

EE reduces by local projection at grows linearly in time (like quantum quench) After saturation, goes to zero (projection effect goes out)

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SLIDE 17

Holo

  • lographic EE

EE aft fter Proje

  • jectio

ion or

  • r En

Entangli ling

(Geodesic Length ) Disconnected Connected Disconnected Connected Reduced

Generated

Connected Geodesic Disconnected Geodesics

BH Horizon Entangling Projection

Only Connected Connected Disconnected

  • r

(Whole Torus) (Half of Torus)

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SLIDE 18

Analogue of Quantum Teleportation in CFT & Holography

“Quantum Teleportation” of Local Operator Partial Entangling + Local Projection + Local Unitary Transformation

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SLIDE 19

Path th-Integral Pict ictures: Qua uantum Tele eleportatio ion

Final state in

Euclidean Lorentzian Euclidean Lorentzian Projection Entangling to Projection to

Teleported !

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SLIDE 20

Hol

  • lographic Mod
  • del of
  • f Quantum Tele

leportation

2-sided AdS BH

Projection

Effective Temperature reduces by half 1-sided AdS BH Collapse

Projecting out

Teleportation to through the Euclidean BH

Collapse of the holographic geometry

Traversable channel created by Swapping ??

( The topology can change )

“Classical Communication” part ??

  • cf. [Susskind ‘14, ‘16]

Need more detail understandings ….

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SLIDE 21

Summary Further Directions …

Partial Swapping Local (Partial) Projection

3 Quantum Operations

Partial Entangling

in CFTs & Holographic Duals

?? CFT Analogue & Holographic Model of “Quantum Teleportation” of Local Operators Higher dim. Generalizations New Entanglement Measures in QFT & Holography for Multi-partite Entanglement More details on “Quantum Teleportation” in QFT & Holography Interpretation in Tensor Networks (Quantum Discord,…?) from Local Operations …etc for Mixed States … (GHZ, …?)

Vol( operated region )

(# of EPR pairs crossing the edges )

BTZ BH

Dual

Torus

Time evolution

Torus

Different Cycle as Entangling

(Can) Reduce EE

Half of BTZ BH Dual

Half of Torus

But, Generate EE sometime

(Growth like Quantum Quench)

Time evolution

1604.01772 [hep-th]

THANKS !!

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SLIDE 22

Appendix

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SLIDE 23

Some Details on QFT Analogue of “Quantum Teleportation”

The state after Entangling between and Act on the state Projecting the state by

Final state in Teleported !

Projecting the state by Projecting the state by

with some conditions for the linearity

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SLIDE 24

Tim Time Evol

  • lutio

ion of

  • f

Holo

  • lographic EE

EE aft fter En Entangli ling

log t growth & decay Similar to locally excited state (local operator quench) in holographic CFTs

Gravity dual : [Nozaki-Numasawa-Takayanagi ‘13]

No quasi-particle picture ??

[Caputa-Nozaki-Takayanagi ‘14] [Asplund-Bernamonti-Galli-Hartman ‘14]