Brane Brain (Neuroscience) (Superstring theory) 2 Deep Learning cat - - PowerPoint PPT Presentation

brane brain neuroscience superstring theory
SMART_READER_LITE
LIVE PREVIEW

Brane Brain (Neuroscience) (Superstring theory) 2 Deep Learning cat - - PowerPoint PPT Presentation

KIAS, 26 March, 2018 Cquest, Sogang u., 29 March, 2018 MIT, CTP, 4 Apr, 2018 MPI, AEI, 13 Apr, 2018 H ET group, Osaka, 30 May, 2018 DLAP2018 workshop, 1 June, 2018 Deep Learning and AdS/CFT Koji Hashimoto (Osaka u) ArXiv:1802.08313 w/ S.


slide-1
SLIDE 1

Deep Learning and AdS/CFT

Koji Hashimoto (Osaka u)

ArXiv:1802.08313 w/ S. Sugishita (Osaka),

  • A. Tanaka (RIKEN AIP),
  • A. Tomiya (CCNU)

KIAS, 26 March, 2018 Cquest, Sogang u., 29 March, 2018 MIT, CTP, 4 Apr, 2018 MPI, AEI, 13 Apr, 2018 HET group, Osaka, 30 May, 2018 DLAP2018 workshop, 1 June, 2018

slide-2
SLIDE 2

2

Brane Brain (Superstring theory) (Neuroscience)

slide-3
SLIDE 3

Deep Learning

Black hole CFT AdS

AdS/CFT “cat”

[Maldacena ‘97]

slide-4
SLIDE 4

4

  • 1. Formula`on of

AdS/DL correspondence

  • 2. Implementa`on of AdS/DL

and emerging space

slide-5
SLIDE 5

Solving inverse problem

1-1

AdS/CFT: quantum response from geometry Deep learning: op=mized sequen=al map From AdS to DL Dic=onary of AdS/DL correspondence

review review

1-2 1-3

  • 1. Formula`on of

AdS/DL correspondence

slide-6
SLIDE 6

Conven`onal holographic modeling Metric

Experiment data

Model

gµν

Predic`on Predic`on Comparison Experiment data

Solving inverse problem

1-1

AdS/CFT (No proof, no deriva`on) Classical gravity in d+1 dim. space`me Quantum field theory in d dim. space`me (Strong coupling limit)

||

slide-7
SLIDE 7

Conven`onal holographic modeling Metric

Experiment data

Model

gµν

Predic`on Predic`on Comparison Experiment data

Solving inverse problem

1-1

Our deep learning holographic modeling Metric Model

gµν

Predic`on Experiment data Experiment data

slide-8
SLIDE 8

8

AdS/CFT: quantum response from geometry

Classical scalar field theory in (d+1) dim. geometry

S =

  • dd+1x
  • − det g
  • (∂ηφ)2 − V (φ)
  • f ∼ η2, g ∼ const.

f ∼ g ∼ exp[2η/L] AdS boundary ( ) :

η ∼ ∞

Black hole horizon ( ) :

η ∼ 0 ds2 = −f(η)dt2 + dη2 + g(η)(dx2

1 + · · · + dx2 d−1)

Solve EoM, get response . Boundary condi`ons: ∂ηφ

  • η=0= 0

AdS boundary ( ) :

η ∼ ∞

Black hole horizon ( ) :

η ∼ 0 φ = Je−∆−η + 1 ∆+ ∆− Oe−∆+η OJ

review

[Klebanov, Wiken]

slide-9
SLIDE 9

Deep learning : op=mized sequen=al map

F = fix(N)

i

Layer 1 Layer 2 Layer N

“Weights” (variable linear map)

ϕ(x)

“Ac`va`on func`on” (fixed nonlinear fn.) 1) Prepare many sets : input + output 2) Train the network (adjust ) by lowering “Loss func`on”

{x(1)

i , F}

Wij W (1)

ij

x(1)

i

x(2)

i = ϕ(W (1) ij x(1) j )

x(N)

i

review

E ≡

  • data
  • fi(ϕ(W (N−1)

ij

ϕ(· · · ϕ(W (1)

lm x(1) m )))) − F

slide-10
SLIDE 10

10

From AdS to DL

Discre`za`on, Hamilton form

π(η + ∆η) = π(η) + ∆η

  • h(η)π(η) − δV (φ(η))

δφ(η)

  • φ(η + ∆η) = φ(η) + ∆η π(η)

φ π

η

η = 0

Neural-Network representa`on

π(η = 0) η = ∞

Bulk EoM

∂2

ηφ + h(η)∂ηφ − δV [φ]

δφ = 0

h(η) ≡ ∂η

  • log
  • f(η)g(η)d−1
  • metric

1-2

slide-11
SLIDE 11

11

From AdS to DL

Discre`za`on, Hamilton form

π(η + ∆η) = π(η) + ∆η

  • h(η)π(η) − δV (φ(η))

δφ(η)

  • φ(η + ∆η) = φ(η) + ∆η π(η)

Neural-Network representa`on Bulk EoM

∂2

ηφ + h(η)∂ηφ − δV [φ]

δφ = 0

h(η) ≡ ∂η

  • log
  • f(η)g(η)d−1
  • metric

1-2

φ π

η

η = 0

η = ∞

π

  • η=0= 0
slide-12
SLIDE 12

12

Dic=onary of AdS/DL correspondence AdS/CFT Deep learning

Emergent space Depth of layers Bulk gravity metric Network weights Nonlinear response Input data Horizon condi`on Output data Interac`on Ac`va`on func`on

OJ

∂ηφ

  • η=0= 0

h(η)

W (a)

ij

1-3

x(1)

i

F

ϕ(x)

V (φ)

∞ > η ≥ 0

i = 1, 2, · · · , N

slide-13
SLIDE 13

Solving inverse problem

1-1

Deep learning : op=mized sequen=al map AdS/CFT: quantum response from geometry From AdS to DL Dic=onary of AdS/DL correspondence

review review

1-2 1-3

  • 1. Formula`on of

AdS/DL correspondence

slide-14
SLIDE 14

14

  • 1. Formula`on of

AdS/DL correspondence

  • 2. Implementa`on of AdS/DL

and emerging space

slide-15
SLIDE 15

Emergent geometry in deep learning

2-1

Can AdS Schwarzschild be learned? Emergent space from real material? Numerical experiment summary Machines learn…, what do we learn?

2-2

2-3

2-4 2-5

  • 2. Implementa`on of AdS/DL

and emerging space

slide-16
SLIDE 16

16

Experiment 1: “Can AdS Schwarzschild be learned?” Experiment 2: “Emergent space from real material?” 1) Use AdS Schwarzschild and generate input data. 2) Prepare network with unspecified metric. 3) Let the network learn it by the data. 4) Check if AdS Schwarzschild is reproduced. 1) Use material experimental data. Ex) Magne`za`on curve of strongly correlated material 2) 3) (same as above.) 4) Watch how space emerges!

Emergent geometry in deep learning

2-1

slide-17
SLIDE 17

17

Exp1: Can AdS Schwarzschild be learned?

2-2

1) Use AdS Schwarzschild and generate input data. 2) Prepare network with unspecified metric. 3) Let the network learn it by the data. 4) Check if AdS Schwarzschild is reproduced. AdS Schwarzschild metric in the unit of AdS radius

∂2

ηφ + h(η)∂ηφ − δV [φ]

δφ = 0

V [φ] = −φ2 + 1 4φ4

h(η) = 3 coth(3η)

L = 1

slide-18
SLIDE 18

18

Exp1: Can AdS Schwarzschild be learned?

2-2

1) Use AdS Schwarzschild and generate input data. 2) Prepare network with unspecified metric. 3) Let the network learn it by the data. 4) Check if AdS Schwarzschild is reproduced.

φ π

η

η = 0

η = ∞ π(η + ∆η) = π(η) + ∆η

  • h(η)π(η) − δV (φ(η))

δφ(η)

  • φ(η + ∆η) = φ(η) + ∆η π(η)

π

  • η=0= 0
slide-19
SLIDE 19

19

Exp1: Can AdS Schwarzschild be learned?

2-2

1) Use AdS Schwarzschild and generate input data. 2) Prepare network with unspecified metric. 3) Let the network learn it by the data. 4) Check if AdS Schwarzschild is reproduced.

φinput πinput

Horizon condi`on : true : false

slide-20
SLIDE 20

20

Exp1: Can AdS Schwarzschild be learned?

2-2

1) Use AdS Schwarzschild and generate input data. 2) Prepare network with unspecified metric. 3) Let the network learn it by the data. 4) Check if AdS Schwarzschild is reproduced. Unspecified metric (10 layers, to be trained) Generated data from AdS Schwarzschild (10000 data points)

φinput

πinput

π

  • η=0= 0
slide-21
SLIDE 21

21

Exp1: Can AdS Schwarzschild be learned?

2-2

1) Use AdS Schwarzschild and generate input data. 2) Prepare network with unspecified metric. 3) Let the network learn it by the data. 4) Check if AdS Schwarzschild is reproduced.

slide-22
SLIDE 22

22

Exp1: Can AdS Schwarzschild be learned?

2-2

1) Use AdS Schwarzschild and generate input data. 2) Prepare network with unspecified metric. 3) Let the network learn it by the data. 4) Check if AdS Schwarzschild is reproduced. With a regulariza`on

slide-23
SLIDE 23

23

Experiment 1: “Can AdS Schwarzschild be learned?” Experiment 2: “Emergent space from real material?” 1) Use AdS Schwarzschild and generate input data. 2) Prepare network with unspecified metric. 3) Let the network learn it by the data. 4) Check if AdS Schwarzschild is reproduced. 1) Use material experimental data. Ex) Magne`za`on curve of strongly correlated material 2) 3) (same as above.) 4) Watch how space emerges!

Emergent geometry in deep learning

2-1

slide-24
SLIDE 24

24

Exp2: Emergent space from real material?

2-3

1) Use material experimental data. Ex) Magne`za`on curve of strongly correlated material 2) 3) (same as above.) 4) Watch how space emerges!

slide-25
SLIDE 25

25

Numerical experiment summary

2-4

Experiment 1

AdS Schwarzschild is successfully learned.

Experiment 2

Experimental data is explained by emergent space.

slide-26
SLIDE 26

26

Machines learn…, what do we learn?

2-5

Conven&onal holographic modeling Our deep learning holographic modeling Metric

Experiment data

Model

gµν

Experiment data Predic&on Predic&on Comparison

Metric

Experiment data

Model

gµν

Experiment data Predic&on

slide-27
SLIDE 27

27

  • 1. Formula`on of

AdS/DL correspondence

  • 2. Implementa`on of AdS/DL

and emerging space