new compressible phases from gravity and their entanglement
TRANSCRIPT
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New Compressible Phases From Gravity And Their Entanglement
Sandip Trivedi, TIFR, Mumbai Simons Workshop, Feb 2013
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Kevin Goldstein, Nori Iizuka,
Shamit Kachru, Nilay Kundu,
Prithvi Nayaran, Shiroman Prakash,
Nilanjan Sircar, Alexander Westphal
Collaborators:
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More recent work:
Tadashi Takayanagi, K. Narayan
Nilay Kundu, Nilanjan Sircar,
Collaborators:
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Outline 1. Introduction
2. Einstein-Dilaton-Maxwell System and Branes
3. String Realisations
4. Conclusions
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Introduction
AdS/CFT correspondence has opened the possibility for a dialogue between the study of gravity and condensed matter physics (more generally the study of strongly coupled field theories).
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Introduction
At this early stage it is useful to ask about qualitative insights from the ``other side’’.
An important qualitative feature about any system is the different phases it exhibits.
On the gravity side this corresponds to different kinds of brane solutions.
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Introduction
Already insights from condensed matter physics are proving useful in understanding the various phases which can arise in gravity.
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Example: Holographic Superconductor (Gubser; Hartnoll, Herzog, Horowitz …)
Gravity Field Theory
Gauge Symmetry Global Symmetry
Broken Gauge Broken Global Sym Symmetry?
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Example : Holographic Superconductor
Intuition from field theory lead to the discovery of Holographic Superconductors. Despite tension with no-Hair theorems.
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Introduction
Black Hole With Charged Scalar Hair
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New Phases in Gravity
Other examples where phases known in nature helped motivate new brane solutions in gravity will also be discussed in Shamit Kachru’s talk.
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• In this talk we will try to run the correspondence the other way around.
• Are there phases in gravity which might be of interest in condensed
matter physics?
Introduction
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In particular we will look at field theories with a global U(1) symmetry
which is unbroken.
Introduction
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Introduction
An important property is compressibility:
n: charge density : chemical potential
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Question we will ask:
Are there compressible phases where the symmetry is unbroken which occur on the gravity side?
Introduction:
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Introduction
Essentially only one phase is well understood in condensed matter physics which is compressible with the symmetry being unbroken:
Fermi liquid.
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Introduction
Studying other compressible phases might be helpful from the point of view of understanding non-Fermi liquid behaviour and the properties of interesting classes of materials which exhibit this behaviour.
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New Compressible Phases From Gravity
It turns out that in gravitational systems such compressible phases can arise quite easily!
Most of this talk will focus on zero temperature phases (extremal branes), Or small temperatures:
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New Compressible Phases From Gravity
And mostly (till we come to string embeddings) we will work in 4 dimensions in the gravity description.
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New Compressible Phases From Gravity
The simplest example is the extremal Reissner Nordstrom Brane. This is a ``unphysical’’ though due to the large entropy at zero temperature.
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New Compressible phases
• Interesting but too exotic!
• Compressible:
• Entropy density:
• Possibly unstable.
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Einstein-Dilaton-Maxwell System
Instead let us consider a system with an additional neutral scalar, the dilaton.
: an important parameter Rocha, Gubser; Goldstein, Kachru, Prakash, SPT
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Dilatonic Extremal Branes
Intuition: For fixed charge the stress energy of the Maxwell field can change as the dilaton changes.
If the dilaton ``runs off’’ to the gauge coupling could go to zero and the gravitational radius could vanish.
Leading to zero entropy.
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Example 2: New Compressible Phases From Gravity
Indeed this turns out to be true.
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boundary AdS
Near horizon
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Dilatonic Extremal Brane
AdS:
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Dilatonic Extremal Brane
Horizon:
Area vanishes.
determined by parameter
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Dilatonic Extremal Brane
Lifshitz type Kachru, Liu, Mulligan
Scale Invariant:
Dynamical exponent:
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Dilatonic Extremal Brane
Compressible:
Specific heat:
Conductivity:
Not Fermi liquid.
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Dilatonic Extremal Brane
Tidal forces can diverge.
Can be controlled by heating the system to a small temperature:
Horowitz, Way
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Dilatonic Extremal Brane
Generalisation: Charmosis, Goteraux, Kim, Kiritsis, Mayer
Now two parameters
Asymptotic form of
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Extremal Dilatonic Black Branes
Black Brane solutions with sensible thermodynamics arise for a range of the parameters
Charmosis, Goteraux, Kim, Kiritsis, Mayer
Iizuka, Kundu, Narayan, Trivedi
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Extremal Dilatonic Black Branes
• Compressible
• Specific Heat and conductivity: Non Fermi liquid.
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Dilatonic Black Branes
Near horizon:
: are determined by
Not scale invariant for
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Dilatonic Black Branes
Near horizon:
Not scale invariant for
Has a conformal killing vector.
Of Hyperscaling violating type. Huijse, Sachdev, Swingle
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Dilatonic Black Branes
One can probe the behaviour of the system in more detail. Probe Fermions.
Iizuka, Kundu, Narayan, SPT
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Dilatonic Black Branes
Turning on a small magnetic field.
Gives rise an IR geometry.
Extensive entropy For
Kundu, Narayan, Sircar, SPT
Universal exponent
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s an attractor for a large class of situations!
Other worries:
Friedel Oscillations?
Supressed weight in current-current correlator
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Dilatonic Branes
Key question: Is there a Fermi surface?
Key insight: Ogawa, Takyanagi, Ugajin
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Key Insight: Use Entanglement
Boundary has area A
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Entanglement
Fermi surface:
This behaviour arises for some set of values in
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Dilatonic Branes
Another coordinate system:
z : dynamical exponent : Hyperscaling violation exponent
Huijse, Sachdev, Swingle
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Entanglement
Fermi surface:
This behaviour arises when
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Dilatonic Branes
Specific heat can be understood in terms of gapless excitations which disperse with a dynamic exponent z.
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Dilatonic Black Branes
Turning on a small magnetic field.
Gives rise an IR geometry.
Extensive entropy For
Kundu, Narayan, Sircar, SPT
Universal exponent
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s an attractor for a large class of situations!
Other worries:
Friedel Oscillations?
Supressed weight in current-current correlator
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String Embeddings
Interesting possibility.
We will study it further in a string embedding.
Important issue: Does imply a Fermi surface?
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String Embedding
K. Narayan
Harvendra Singh
String Construction is simple and promising. And its field theory dual is known.
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String Embedding
The dilaton and gauge field arise from Kaluza Klein reduction of a 5-dimensional theory.
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String Embedding
5 dim. Description: plane wave
R: Radius of AdS
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String Embedding
Dual Description:
CFT in a state with
E.g. N=4 SYM.
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String Embedding
Compactifying on direction gives rise to a 4 dimensional metric.
With
In field theory Null direction.
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Five Dimensions
To avoid any complications we will work directly in 5 dimensions.
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Five Dimensions: Strip Geometry
z,y
x
L
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Entanglement: 5 Dim
For
Entanglement : 4 Dim Plane wave:
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Picture:The plane wave is an excited state which continues to be highly ordered in the transverse directions.
Any CFT with a gravity dual will have this behaviour.
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Turning on a small temperature T allows us to identify the state in the CFT.
CFT T
Boost
Taking a strip in boosted frame of width gives rise to the log enhanced entanglement
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CFT Description
Boosted slice
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We can go back down to 4 dim. on a small spatial circle along z direction of radius r.
How does entanglement behave?
Three scales: Analysis not complete. Work in progress.
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Conclusions
• Gravity theories quite easily give rise to compressible phases with unbroken U(1) symmetry.
• Some of these are interesting possibilities for non-Fermi liquids.
• Some simple string embeddings have been found. These might help lead to further progress.
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