New Frontiers of Lattice Field Theories GGI Firenze 17 September - - PowerPoint PPT Presentation

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New Frontiers of Lattice Field Theories GGI Firenze 17 September - - PowerPoint PPT Presentation

QCD with many flavors at zero and non-zero temperature Maria Paola Lombardo Albert Deuzeman, MPL , Kohtaroh Miura , Tiago Nunes da Silva, Elisabetta Pallante New Frontiers of Lattice Field Theories GGI Firenze 17 September 2012 QCD with many


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QCD with many flavors at zero and non-zero temperature

New Frontiers of Lattice Field Theories

GGI Firenze 17 September 2012

Maria Paola Lombardo

Albert Deuzeman, MPL , Kohtaroh Miura , Tiago Nunes da Silva, Elisabetta Pallante

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Hadronic Ph Phase

Quasi Conformal/ Walking dynamics Conformal Window of QCD

Nfc

NAF NAF

Nf

QCD with many flavors : Sketchy view of the phase diagram

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(ideal) Outline

  • Nf=0
  • Nf=1
  • Nf=2
  • Nf=3
  • Nf=4
  • Nf=5
  • Nf=6
  • Nf=7
  • Nf=8
  • Nf=9
  • Nf=10
  • Nf=11
  • Nf=12
  • Nf=13
  • Nf=14
  • Nf=15
  • Nf=16
  • Summary
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Outline

  • Nf=0
  • Nf=2
  • Nf=3
  • Nf=4
  • Nf=5
  • Nf=6
  • Nf=7
  • Nf=8
  • Nf=9
  • Nf=10
  • Nf=11
  • Nf=12
  • Nf=13
  • Nf=14
  • Nf=15
  • Nf=16

Introduction

Near Conformal: Continuum and Lattice Conformal

Summary Nfc ≈ 12

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Near Conformal: Continuum and Lattice

This talk’s main theme: precursors effects of conformality when approaching Nfc from the QCD side

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QCD-like : running coupling

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Running vs Walking :

Both compatible with IR slavery and UV freedom

Walking :

Separation of Scales:

Interesting for Phenomenology

Running : L sets the scale

acr

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  • For Nf > 8 the perturbative b

function of QCD develops a second 0 : the Banks-Zacs IRFP .

  • Then the coupling runs to IRFP
  • Chiral Symmetry Breaking requires a>acr:
  • 1) IRFP < acr 

CONFORMAL WINDOW

2) IRFP > acr 

IRFP disappears

QCD-like, but:

NEAR-CONFORMALITY, WALKING

The discovery of the conformal window of QCD

Miransky-Yamawaki, 1997; Appelquist et al. 1997

Conformal transition Relevant for Technicolor a*

acr acr

CONFORMAL WINDOW NEAR-CONFORMALITY, WALKING

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Running established up to 5 Flavors

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Can we establish walking as well?

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Can we establish walking as well? (if yes, it has to be for Nf > 5)

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Near-Conformal behaviour On the QCD-side can be seen in:

Different scales LUV and LIR Critical behaviour Nf Nfc

m

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  • J. Braun , H. Gies 06 08 09

Thermal transition and near-conformal dynamics

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Towards Conformality: Continuum (from the lattice)

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From the Lattice..

Nt x a Ns x a

Must be approx. constant for several Nt

(Old fashioned asymptotic scaling)

..to the continuum

Via old fashioned asymptotic scaling

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Nf = 6 Chiral crossover of order parameter

Nt

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Nf=6 , Polyakov loop

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Nf=6 : Chiral crossover of the chiral cumulant Rp

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Summary of results for bc (updated at xQCD2012)

Must be Nt independent

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Nt-(quasi) independence of Tc/LLat for Nf = 6

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Tc/L as a function of Nf

Tc/L

Nf

Scale separation

Conventional running

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Fixing an UV scale

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Tc/MUV

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Trading LLAT for LIR stable

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Shuryak and Sulejmanpasic , 2012 Shuryak and Liao, 2012

Alternative analysis

Our results Strongest coupled QGP?

Nf

Line Of IRFP

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Hadronic Phase

Strongly Coupled QGP

Quasi Conformal QGP

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(Quasi)Conformality and High T QCD

  • S. Borsaniy et al.2011
  • M. Panero 2010

h/S < (3 –5) / 4 p

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Conformality and near-Conformality at zero and finite T: coupling ‘walks’ in the plasma!

  • J. Braun, H. Gies , 06

Conformal Window

Kaczmarez-Zantov 2005

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Towards Conformality- Lattice

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evidence of)

And in progress

PHASES OF QCD ON THE LATTICE : Temperature = 0

Miransky, Yamawaki

?

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evidence of)

And in progress

PHASES OF QCD ON THE LATTICE : Finite Nt

?

Nf=0 Yang- Mills finite T deconf Finite T chiral transition finite Nf

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Phases of QCD below Nf_c

PHASES OF QCD ON THE LATTICE : Finite Nt Numerical results

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Critical number of flavor from thermal lines

Nfc = 10(2) (preliminary)

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Inside the Conformal window

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The nucleon mass and the ‘Edinburgh Plot’ in the conformal window

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Mass ratio : qualitative features discriminating broken and symmetric phases

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The transition of 4dQED on a Lattice Kocic, Kogut, MPL, 1992

Symmetric Broken

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Nf = 12

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Nf=12: mass ratio

Our results

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Chiral Partners, and anomalous dimension

Caveat... Can we compute anomalous dimenions away from IRFP ???

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Critical scaling of the chiral transition Critical scaling of IRFP

Two Tasks: 1) Chiral Symmetry vs Chiral Symmetry Breaking 2) If we measure an anomalous dimension, is this associated to Chiral or Conformal Symmetries?

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Summary

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Near-conformal dynamics (continuum): Tc/L suggests scale separation for Nf > 6 Pre-conformal (critical) behaviour

  • bserved for Nf > 6, with Nf critical = 11 (3)

Shuryak’s (equivalent) view : coupling at (Tc, Nfc) = coupling at IRFP Near-conformal dynamics (lattice) : Thermal pseudocritical lines meet at (g*, Nf critical), with Nf critical = 10(2) (preliminary)

All estimates confirm that twelve flavors is close to the conformal transitions – Nf=12 difficult to study directly (as we know!) Interesting interplay with finite temperature QCD with implications for the physics of the strongly interactive quark gluon plasma