spectral functions for holographic mesons

Spectral functionsfor holographic mesons

with Rowan Thomson, Andrei Starinets[arXiv:0706.0162]

and other stuffVwith Aninda Sinha [arXiv:0801.nnnn]

Motivation:

Exploring AdS/CFT as a tool to studythe strongly coupled quark-gluon plasma

See Steve Gubser’s talk!

Field theory story:N =2 SU(Nc) super-Yang-Mills with (Nf+1) hypermultiplets

Nf massive hyper’s “quarks”

2 complex scalars :2 Weyl fermions:

N =4 SYMcontent

fund. in U(Nc) & global U(Nf)

(Reader’s Digest version)

fundamental adjoint

adjoint fields: vector:1 hyper:

fundamental fields:

• work in limit of large Nc and large λ but Nf fixed

“quenched approximation”:

• low temperatures: free quarks

mesons ( bound states)f f

Finite Temperature:

• phase transition:

• high temperatures: NO quark or meson quasi-particles “quarks dissolved in strongly coupled plasma”

(strong coupling!!)

• note not a confining theory: free quarks

“mesons” ( bound states)f f

unusual dispersion relation:

Holographic Results

add Nf probe D7-branes

horizon

AdS5 boundary

pole

equator

S5

S3

D7

Free quarks appear with mass:

Karch & Katz (hep-th/0205236 )Adding flavour to AdS/CFT

Aharony, Fayyazuddin & Maldacena (hep-th/9806159 )

add Nf probe D7-branes

horizon

AdS5 boundary

pole

equator

S5

S3

D7

Karch & Katz (hep-th/0205236 )Adding flavour to AdS/CFT

Mesons ( bound states) dual to open string states supported by D7-brane

Aharony, Fayyazuddin & Maldacena (hep-th/9806159 )

Mesons:lowest lying open string states are excitations of themassless modes on D7-brane: vector, scalars (& spinors)

(free) spectrum:• expand worldvolume action to second order in fluctuations• solve linearized eq’s of motion by separation of variables

Veff

rDiscrete spectrum:

Kruczenski, Mateos, RCM & Winters [hep-th/0304032]

= radial AdS #= angular # on S3

Gauge theory thermodynamics = Black hole thermodynamics

Gauge/Gravity thermodynamics:Witten (hep-th/9803131); …..

• Replace SUSY D3-throat with throat of black D3-brane• Wick rotate and use euclidean path integral techniqes

• . . . . .

Extend these ideas to includecontributions of probe branes/fundamental matter

Gauge/Gravity thermodynamics with probe branes:put D7-probe in throat geometry of black D3-brane

SUSY embedding

Minkowski embedding

Black hole embedding

T=0: “brane flat”

Low T: tension supports brane; D7 remains outside BH horizon

raise T: horizon expands and increased gravity pulls brane towards BH horizon

High T: gravity overcomes tension; D7 falls through BH horizon

D7

D3

Phase transition†

(†This new phase transition is not a deconfinement transition.)

Mateos, RCM &Thomson [hep-th/0605046]; . . . . .Babington, Erdmenger, Evans, Guralnik & Kirsch [hep-th/0306018]

Brane entropy:

1st order phase transition

Transition temperature:

Mateos, RCM &Thomson [hep-th/0605046 & hep-th/0701132]

Mesons in Motion:

pseudoscalar

scalar

Mateos, RCM &Thomson [hep-th/0701132]Ejaz, Faulkner, Liu, Rajagopal & Wiedemann [arXiv:0712.0590]

Radial profile

k increasing

• holographic model shows bound states persist above Tc

and have interesting dispersion relation

• lattice QCD indicates heavy quark bound states persist above Tc

Asakawa & Hatsuda [hep-lat/0308034]

Datta, Karsch, Petreczky & Wetzorke [hep-lat/0312037]

Does “speed limit” apply to heavy quark states in QCD?

In experiments (eg, RHIC or LHC), these bound statesare created with finite (possibly large) momenta.

• holographic model shows bound states persist above Tc

and have interesting dispersion relation

• lattice QCD indicates heavy quark bound states persist above Tc

Asakawa & Hatsuda [hep-lat/0308034]

Datta, Karsch, Petreczky & Wetzorke [hep-lat/0312037]

Satz [hep-ph/0512217]

’s have finite width!

but in Mink. phase, holographic mesonsare absolutely stable (for large Nc)

can we do better in AdS/CFT?

Spectral functions: diagnostic for “meson dissociation”

• simple poles in retarded correlator:

yield peaks:

“quasi-particle” if

• characteristic high “frequency” tail:

discrete spectrum;low temperature Mink. phase

continuous spectrum;high temperature BH phase

mesons stable (at large Nc) no quasi-particles

hi-freq tail

Spectral functions: diagnostic for “meson dissociation”

• approaching phase transition, structure builds quasinormal frequencies approach real axis

Thermal spectral function:

subract off asymptotic tail: phase transition

see also: Hoyos, Landsteiner & Montero [hep-th/0612169]

RCM, Rowan Thomson & Andrei Starinets [arXiv:0706.0162]

Kobayashi, Mateos, Matsuura, RCM & Thomson [hep-th/0611099]Mateos, Matsuura, RCM & Thomson [arXiv:0709.1225]; . . . . .

Need an extra dial: “Quark” density

D7-brane gauge field:

asymptotically (ρ→∞):

Kobayashi, Mateos, Matsuura, RCM & Thomson [hep-th/0611099]Mateos, Matsuura, RCM & Thomson [arXiv:0709.1225]; . . . . .

Need an extra dial: “Quark” density

electric field lines can’t end in empty space; nq produces neck

D7-brane gauge field:

asymptotically (ρ→∞):

BH embedding with tunable horizon

See also: Erdmenger, Kaminski & Rust [arXiv:0710.033]

Increasing nq, increases width of meson statesSpectral functions:

nq = 0 = 0.001 = 0.05 = 0.25

at rest: q=0

See also: Erdmenger, Kaminski & Rust [arXiv:0710.033]

Increasing nq, increases width of meson statesSpectral functions:

nq = 0 = 0.001 = 0.05 = 0.25

at rest: q=0

Spectral functions:

introduce nonvanishing momentum

(nq = 0.25)

Spectral functions:follow positions of peaks

real part of quasiparticle frequency, Ω(q)

(nq = 0.25)

Spectral functions:follow positions of peaks

real part of quasiparticle frequency, Ω(q)

(nq = 0.25)

vmax = 0.9975(calculated for nq=0)

Quasiparticles obey same speed limit!

follow widths of peaksimaginary part of quasiparticle frequency, Γ(q)

Γ(q) divergesat finite qmax

examine Schrodinger potential for quasinormal modes

Quasiparticles limited to maximum momentum qmax

Conclusions/Outlook:

• first order phase transition appears as universal feature of holographic theories with fundamental matter (Tf > Tc)

• how robust is this transition? should survive finite 1/Nc, 1/λ, Nf/Nc corrections interesting question for lattice investigations

• D3/D7 system: interesting framework to study quark/meson contributions to strongly-coupled nonAbelian plasma

• “speed limit” universal for quasiparticles in plasma

• quasiparticle widths increase dramatically with momentum find in present holographic model universal behaviour? real world effect? (INVESTIGATING)

[extra slides]

Meson spectrum:

Minkowski:discrete stable states

black hole:continuous gapless excitations

• feature of QCD ??

• in a confining theory, will have two phase transitions for sufficiently heavy quarks

• simple physical picture: Matsui & Satz

(Hong, Yoon & Strassler)structure functions reveal:

(Rey, Theisen & Yee)Wilson lines reveal:

mesons dissociate:

• one of most striking features of transition is “meson melting”:

even with mq=0, hypermultiplets introduce non-vanishing -function; however, running of `t Hooft coupling vanisheswith large-Nc limit

More legal details:

with large but finite Nc to avoid Landau pole need to introduce additional matter content at some large UV scale

Probe approximation: Nf /Nc → 0recall above construction does not take into account the“gravitational” back-reaction of the D7-branes!

→ at finite Nf /Nc back-reaction would cause singularity; introduce orientifold at large radius

(see, however: Burrington et al; Kirsch & Vaman; Casero, Nunez & Paredes, . . . . )

entropy density:

Reminder about large N counting:

counts # of d.o.f.

entropy density:

counts # of d.o.f.

in our limit, thermodynamics dominated by adjoint fields;we are calculating small corrections due to fundamental matter

these dominate over quantum effects, eg, Hawking radiation,

phase transition

physical properties of thermalsystem are multi-valued

minimizing free energy(euclidean brane action)

fixes physical configuration

criticalembedding

Minkowskiembeddings

BH embeddingsSee also:Babington et al (hep-th/0306018) Kirsch (hep-th/0406274)

Brane entropy:

1st order phase transition

Transition temperature:

H

Gauge theory entropy:

λ

enhanced over naïvelarge-N counting

phase transition“small glitch in extensive quantities”