experimental detection of the anomalous...

1
? r A = B Z B · darea 6= I A · d` σ xx / T (d+2Φ-2)/z xx / T (d+Φ-2)/z xx / T (d+z -2)/z σ xy / BT (d+3Φ-4)/z xy / BT (d+z +Φ-4)/z =1+2/3=5/3 : Philip W. Phillips and Kridsanaphong Limtragool (arxiv.org/1601.02340) Strange Metal Experimental Detection of the Anomalous Dimension of the Current in the Strange Metal from the Fractional Aharonov-Bohm Effect σ (! )= C ! - 2 3 ne 2 m 1 1 - i!⌧ T-linear resistivity L xy = xy /T σ xy 6=# / T 1 -2/3 single-parameter scaling / T (2-d)/z σ (! ,T ) / ! (d-2)/z C v / T d/z / z does not work solution fractional not d-1 [J ]= Φ What does interwined order have to do with the Strange Metal? So lets focus on the Strange Metal? why an anomalous dimension? ac transport Limtragool/PWP dc transport Karch/Hartnoll σ i (! )= n i e 2 i i m i 1 1 - i!⌧ i σ (! )= M Z 0 (m)e 2 (m)(m) m 1 1 - i!⌧ (m) dm continuous mass dσ (m)= σ (m)dm a +2b - 1 c = - 1 3 σ (! )= 0 e 2 0 1 3 0 M 1 ! 2 3 !⌧ 0 Z 0 dx x - 1 3 1 - ix !⌧ 0 !1 σ (! )= 1 3 ( p 3+3i)0 e 2 0 1 3 0 M ! 2 3 tan σ = p 3 60 momentum loss anomalous dimension hyperscaling violation (m)= 0 m a-1 M a e(m)= e 0 m b M b (m)= 0 m c M c the Lorenz ratio is not a constant L H = xy T σ xy T T -2Φ/z Φ = bz = -2/3 choose solution Experiment: Probe scaling dimension of vector field how can an anomalous dimension be detected independent of any Aharonov- Bohm flux ΔΦ = e ~ I ~ A · d` ΔΦ = eB r 2 ~ what if B has an anomalous [B ]= L -26=1 ΔΦ = eB r 2 ~ is no longer ΔΦ = eB r 2 ~ F (L, ) non-locality of the solution gauge invariance field strength a i [@ i ,I i A i ]= @ i I i A i a μ ! a μ + @ μ - ~ 2 2m (@ i - i e ~ a i ) 2 = i~@ t . F μ=2@ [μ A ] , A μ ! A μ + @ μ G ~ r · ~ J + @ t =0 continuity eq. F μ= @ μ μ A - @ A μ A μ ! A μ + @ μ G proof compute AB phase ΔΦ = e ~ I ~ a(r 0 ) · ~ d` 0 use fractional calculus Δφ R = eB ` 2 ~ b -1 d -1 Γ 2 () c l, d l AB phase has to change Δφ D = e ~ r 2 BR 2-2 p 2 1-Γ(2 - )Γ(1 - 2 ) Γ()Γ( 3 2 - 2 ) sin 2 ⇡↵ 2 2 F 1 (1 - , 2 - ; 2; r 2 R 2 ) ! is the correction large? yes! ΔΦ D = eB ` 2 ~ L 5/3 /Γ(5/3) 2 combine AC+DC fixes all exponents a,b,c [J ]= d U probe with Aharonov-Bohm effect b 6=0 Monday, February 1, 16

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Page 1: Experimental Detection of the Anomalous …qpt.physics.harvard.edu/abs/Phillips-poster.pdfExperiment: Probe scaling dimension of vector field how can an anomalous dimension be detected

?

r↵ ⇥A = BZ

B · darea 6=I

A · d`

�xx

/ T (d+2��2)/z

↵xx

/ T (d+��2)/z

xx

/ T (d+z�2)/z

�xy

/ BT (d+3��4)/z

xy

/ BT (d+z+��4)/z

↵ = 1 + 2/3 = 5/3

:

Philip W. Phillips and Kridsanaphong Limtragool (arxiv.org/1601.02340)

Strange Metal

Experimental Detection of the Anomalous Dimension of the Current in the Strange Metal from the Fractional Aharonov-Bohm Effect

�(!) = C!� 23

n⌧e2

m

1

1� i!⌧

T-linear resistivity

Lxy

= xy

/T�xy

6= # / T

1

�2/3

single-parameter scaling

⇢ / T (2�d)/z

�(!, T ) / !(d�2)/z

Cv / T d/z

⇠⌧ / ⇠z

does not work

solution

fractionalnot d-1

[J ] = �

What does interwined order have todo with the Strange Metal?

So lets focus on the Strange Metal?

why an anomalous dimension?

ac transportLimtragool/PWP

dc transportKarch/Hartnoll

�i(!) =nie2i ⌧imi

1

1� i!⌧i

�(!) =

MZ

0

⇢(m)e2(m)⌧(m)

m

1

1� i!⌧(m)dm

continuous mass d�(m) = �(m)dm

a+ 2b� 1

c= �1

3

�(!) =⇢0e

20⌧

130

M

1

!

23

!⌧0Z

0

dx

x

� 13

1� ix

!⌧0 ! 1

�(!) =1

3(p3 + 3i)⇡

⇢0e20⌧130

M!23

tan� =p3

60�

momentum loss

anomalous dimension

hyperscaling violation⇢(m) = ⇢0

ma�1

Ma

e(m) = e0mb

M b

⌧(m) = ⌧0mc

M c

the Lorenz ratio is not a constant

LH =xy

T�xy⇠ T ⌘ T�2�/z

� = bz = �2/3choose solution

Experiment: Probe scaling dimensionof vector field

how can an anomalous dimension be detected

independent of any

Aharonov- Bohm

flux

�� =e

~

I~A · d`

�� =eB⇡r2

~

what if B has an anomalous [B] = L�2↵ ↵ 6= 1

�� =eB⇡r2

~

is no longer

�� =eB⇡r2

~ F (L,↵)

non-locality of the

solution

gauge invariance field strength

ai ⌘ [@i, I↵i Ai] = @iI

↵i Ai

aµ ! aµ + @µ⇤

� ~22m

(@i � ie

~ai)2 = i~@t .

Fµ⌫ = 2@[µA⌫],Aµ ! Aµ + @µG

~r↵ · ~J + @t⇢ = 0 continuity eq.

F↵µ⌫ = @↵µ

µ A⌫ � @↵⌫⌫ AµAµ ! Aµ + @↵

µG

proof

compute AB phase�� =

e

~

I~a(r0) · ~d`0

use fractional calculus

��R =eB`2

~

✓b↵�1d↵�1

�2(↵)

◆c � l, d � l

AB phase has to change

��D =e

~⇡r2BR2↵�2

p⇡21�↵�(2� ↵)�(1� ↵

2 )

�(↵)�( 32 � ↵2 )

sin2⇡↵

22F1(1� ↵, 2� ↵; 2;

r2

R2)

!

is the correction large?

yes!

��D =eB`2

~ L5/3/�(5/3)2

combine AC+DC

fixes all exponentsa,b,c

[J ] = dU

probe withAharonov-Bohm effect

b 6= 0

Monday, February 1, 16