Presentation is loading. Please wait.

Presentation is loading. Please wait.

A direct relation between confinement and chiral symmetry breaking in temporally odd-number lattice QCD Lattice 2013 July 29, 2013, Mainz Takahiro Doi.

Published byNeil Cecil Freeman Modified over 8 years ago

Similar presentations

Presentation on theme: "A direct relation between confinement and chiral symmetry breaking in temporally odd-number lattice QCD Lattice 2013 July 29, 2013, Mainz Takahiro Doi."— Presentation transcript:

1 A direct relation between confinement and chiral symmetry breaking in temporally odd-number lattice QCD Lattice 2013 July 29, 2013, Mainz Takahiro Doi (Kyoto University) in collaboration with Hideo Suganuma (Kyoto Univesity) Takumi Iritani (KEK) Abstract: We derive an identity connecting Polyakov loop and Dirac modes in temporally odd-number lattice, where the temporal length is odd in lattice unit. This identity describes the relation between confinement and chiral symmetry breaking. From this identity, we conclude that there is no one-to-one correspondence between confinement and chiral symmetry breaking in QCD. We have numerically confirmed this identity. Moreover, modifying Kogut-Susskind formalism for even lattice, we develop the method for spin-diagonalizing Dirac operator in the temporally odd-number lattice.

2 Contents Introduction Quark Confinement(Confinement) Chiral Symmetry Breaking(CSB) Previous Works QCD phase transition at finite temperature S. Gongyo, T. Iritani, H. Suganuma Our Work A Direct Relation between Polyakov loop and Dirac mode in Temporally Odd Number Lattice New Modified KS Formalism in Temporally Odd Number Lattice

3 Contents Introduction Quark Confinement(Confinement) Chiral Symmetry Breaking(CSB) Previous Works QCD phase transition at finite temperature S. Gongyo, T. Iritani, H. Suganuma Our Work A Direct Relation between Polyakov loop and Dirac mode in Temporally Odd Number Lattice New Modified KS Formalism in Temporally Odd Number Lattice

4 Introduction – Quark confinement Confinement : one cannot observe colored state (one quark, gluons, ・・・ ) one can observe only color-singlet states (mesons, baryons, ・・・ ) Polyakov loop : order parameter for quark deconfinement phase transition in quenched approximation. :Polyakov loop in continuum theory in lattice theory :free energy of the system with a single heavy quark 4(t) Finite temperature : periodic boundary condition for time direction

5 Introduction – Chiral Symmetry Breaking ・ Chiral condensate : order parameter for chiral phase transition ・ Banks-Casher relation ・ Chiral symmetry breaking : chiral symmetry is spontaneously broken CSB ・ u, d quarks get dynamical mass(constituent mass) ・ Pions appear as NG bosons for example :Dirac eigenvalue density

6 Contents Introduction Quark Confinement(Confinement) Chiral Symmetry Breaking(CSB) Previous Works QCD phase transition at finite temperature S. Gongyo, T. Iritani, H. Suganuma Our Work A Direct Relation between Polyakov loop and Dirac mode in Temporally Odd Number Lattice New Modified KS Formalism in Temporally Odd Number Lattice

7 QCD phase transition at finite temperature :Polyakovloop and it’s susceptibility :chiral condensate and it’s susceptibility High T Low T ・ two flavor QCD with light quarks ・ deconfinement transition chiral transition F. Karsch, Lect. Notes Phys. 583, 209 (2002)

8 :Polyakovloop and it’s susceptibility :chiral condensate and it’s susceptibility High T Low T ・ two flavor QCD with light quarks ・ These two phase transitions are strongly correlated(?) deconfinement transition chiral transition QCD phase transition at finite temperature We define critical temperature as the peak of susceptibility

9 Confinement and Chiral Symmetry Breaking S. Gongyo, T. Iritani, H. Suganuma, PRD86 (2012) 034510 Dirac eigenvalue equation: Dirac eigenmode: Dirac eigenvalue: Dirac eigenvalue density: removing the essence of CSB ※ This formalism is manifestly gauge invariant. Banks-Casher relation: removing low-lying Dirac modes(Dirac IR cut)

10 removing low-lying Dirac modes :Polyakov loop After removing the essence of CSB, the confinement property is kept one-to-one correspondence does not hold for confinement and chiral symmetry breaking in QCD. S. Gongyo, T. Iritani, H. Suganuma, PRD86 (2012) 034510 Confinement and Chiral Symmetry Breaking

11 Contents Introduction Quark Confinement(Confinement) Chiral Symmetry Breaking(CSB) Previous Works QCD phase transition at finite temperature S. Gongyo, T. Iritani, H. Suganuma Our Work A Direct Relation between Polyakov loop and Dirac mode in Temporally Odd Number Lattice New Modified KS Formalism in Temporally Odd Number Lattice

12 A Direct Relation between Polyakov loop and Dirac mode in Temporally Odd Number Lattice ・ Dirac zero modes are important for CSB (Banks-Casher relation) ・ Dirac zero modes have little contribution to Polyakov loop The relation between Confinement and CSB is not one-to-one correspondence in QCD. This conclusion agrees with the previous work by Gongyo, Iritani, Suganuma. ・・・ (A) H. Suganuma, T. Iritani, T. M. D. (Previous presentation) Dirac eigenmode : Link variable operator : Polyakov loop : notation: in temporally odd number lattice:

13 Numerical Confirmation of Analytical Relation (A) ・・・ (A) :are determined from : site : easily obtained notation and coordinate representation where explicit form of the Dirac eigenvalue equation *This formalism is gauge invariant. Numerical confirmation of this relation is important.

14 Kogut-Susskind (KS) Formalism In solving Dirac eigenvalue equation, to reduce the calculation without any approximation, We want to use KS formalism. where explicit form of the Dirac eigenvalue equation However, In temporally odd number lattice, KS formalism is not available directly. We developed new modified KS formalism applicable to temporally odd number lattice.

15 Kogut-Susskind (KS) Formalism Even Lattice J. B. Kogut and L. Susskind(1975) S. Gongyo, T. Iritani, H. Suganuma(2012) where KS Dirac operator : all gamma matrices are diagonalized staggered phase: (lattice size) : even ← “even lattice”

16 Kogut-Susskind (KS) Formalism Even Lattice J. B. Kogut and L. Susskind(1975) S. Gongyo, T. Iritani, H. Suganuma(2012) don't have spinor index where explicit form of the reduced Dirac eigenvalue equation ※ This method is available only in even lattice. This requirement is satisfied only in even lattice. : even periodic boundary condition for example

17 New Modified KS Formalism Temporally Odd Number Lattice where : even : odd ← “temporally odd-number lattice” We use Dirac representation( is diagonalized) : even staggered phase: case of even lattice

18 don't have spinor index where explicit form of the reduced Dirac eigenvalue equation This method is available in temporally odd number lattice. This requirement is satisfied in odd lattice. : even : odd periodic boundary condition *If Not using this method, results are same. New Modified KS Formalism Temporally Odd Number Lattice

19 Relation between Dirac eigenmode and KS Dirac eigenmode Dirac eigenmode KS Dirac eigenmode in odd lattice ・・・ (A) ・・・ (A)’ relation (A)’ is equivalent to (A)

20 Numerical Confirmation of Analytical Relation (A)’ ・・・ (A)’ (A) ⇔ (A)’ ・ quenched SU(3) lattice QCD ・ gauge coupling: ・ lattice size: ⇔ odd ・ periodic boundary condition lattice setup : right hand of (A)’ ・ plaquette action lattice spacing : odd For numerical confirmation of the relation (A)’, We calculated both sides of the relation (A)’, respectively. : left hand of (A)’ = Polyakov loop

21 ・・・ (A)’ (A) ⇔ (A)’ configration No. 1 lattice size : 2 3 ・・・ -0.8037 - i 8.256 -10.86 + i 11.53 -4.777 - i 7.051 -0.8037 - i 8.256-10.86 + i 11.53 -4.777 - i 7.051 Polyakov loop right hand of (A)’ Numerical Confirmation of Analytical Relation (A)’ (confined phase)

22 ・・・ (A)’ (A) ⇔ (A)’ configration No. 1 lattice size : 2 3 ・・・ -163.2 - i 2.156 -164.5 + i 9.025 -155.2 – i 3.704 -163.2 - i 2.157-164.5 + i 9.026 -155.2 - i 3.704 for other cases, results are same. Analytical relation (A)’ exactly holds. Polyakov loop right hand of (A)’ Numerical Confirmation of Analytical Relation (A)’ (deconfined phase)

23 Contribution of Low-Lying Dirac Modes to Polyakov loop ・・・ (A)’ (A) ⇔ (A)’ ← without low-lying Dirac modes Now, We can remove low-lying Dirac modes from Polyakov loop, by removing low-lying Dirac modes from the summation over Dirac modes in right hand of (A)’ We can investigate the contribution of low-lying Dirac modes to Polyakov loop, in other words, contribution of the essence of CSB to confinement. the essence of CSB We numerically show that low-lying Dirac modes have little contribution to Polyakov loop.

24 ・・・ (A)’(A) ⇔ (A)’ configration No. 1 lattice size : 2 3 ・・・ -0.8037 - i 8.256 -10.86 + i 11.53 -4.777 - i 7.051 -0.8090 - i 8.251-10.84 + i 11.51-4.782 - i 7.040 Contribution of Low-Lying Dirac Modes to Polyakov loop Polyakov loop right hand of (A)’ without low-lying Dirac modes (confined phase)

25 configration No. 1 lattice size : 2 3 ・・・ -163.2 - i 2.156 -164.5 + i 9.025 -155.2 – i 3.704 -165.8 - i 2.197-167.3 + i 9.103-157.8 - i 3.723 for other cases, results are same. Polyakov loop right hand of (A)’ without low-lying Dirac modes ・・・ (A)’(A) ⇔ (A)’ Contribution of Low-Lying Dirac Modes to Polyakov loop Low-lying Dirac modes have little contribution to Polyakov loop (deconfined phase)

26 Conclusion and Future Work ・・・ (A) We have derived the analytical relation between Polyakov loop and Dirac eigenmodes in temporally odd-lattice lattice: Conclusion 1. We have found new Modified KS formalism available in temporally odd-number lattice as well as in even lattice: 2.2., Future Work ・ This relation in continuum limit ・ consider not only Polyakov loop but also other quantity about confinement, such as Wilson loop and monopole in Maximaly Abelian gauge. We have also numerically confirmed this relation in each gauge configuration in lattice QCD both in confined and deconfined phases. Thus, one-to-one correspondence does not hold between confinement and CSB in QCD.

Download ppt "A direct relation between confinement and chiral symmetry breaking in temporally odd-number lattice QCD Lattice 2013 July 29, 2013, Mainz Takahiro Doi."

Similar presentations

Lecture 1: basics of lattice QCD Peter Petreczky Lattice regularization and gauge symmetry : Wilson gauge action, fermion doubling Different fermion formulations.

Lecture 1: basics of lattice QCD Peter Petreczky Lattice regularization and gauge symmetry : Wilson gauge action, fermion doubling Different fermion formulations.
Large Nc Gauge Theories on the lattice Rajamani Narayanan Florida International University Rajamani Narayanan August 10, 2011.

Large Nc Gauge Theories on the lattice Rajamani Narayanan Florida International University Rajamani Narayanan August 10, 2011.
A). Introduction b). Quenched calculations c). Calculations with 2 light dynamical quarks d). (2+1) QCD LATTICE QCD SIMULATIONS, SOME RECENT RESULTS (END.

A). Introduction b). Quenched calculations c). Calculations with 2 light dynamical quarks d). (2+1) QCD LATTICE QCD SIMULATIONS, SOME RECENT RESULTS (END.
2+1 Flavor Polyakov-NJL Model at Finite Temperature and Nonzero Chemical Potential Wei-jie Fu, Zhao Zhang, Yu-xin Liu Peking University CCAST, March 23,

2+1 Flavor Polyakov-NJL Model at Finite Temperature and Nonzero Chemical Potential Wei-jie Fu, Zhao Zhang, Yu-xin Liu Peking University CCAST, March 23,
The QCD equation of state for two flavor QCD at non-zero chemical potential Shinji Ejiri (University of Tokyo) Collaborators: C. Allton, S. Hands (Swansea),

The QCD equation of state for two flavor QCD at non-zero chemical potential Shinji Ejiri (University of Tokyo) Collaborators: C. Allton, S. Hands (Swansea),
Scaling properties of the chiral phase transition in the low density region of two-flavor QCD with improved Wilson fermions WHOT-QCD Collaboration: S.

Scaling properties of the chiral phase transition in the low density region of two-flavor QCD with improved Wilson fermions WHOT-QCD Collaboration: S.
Lattice QCD (INTRODUCTION) DUBNA WINTER SCHOOL 1-2 FEBRUARY 2005.

Lattice QCD (INTRODUCTION) DUBNA WINTER SCHOOL 1-2 FEBRUARY 2005.
Topological current effect on hQCD at finite density and magnetic field Pablo A. Morales Work in collaboration with Kenji Fukushima Based on Phys. Rev.

Topological current effect on hQCD at finite density and magnetic field Pablo A. Morales Work in collaboration with Kenji Fukushima Based on Phys. Rev.
Axial symmetry at finite temperature Guido Cossu High Energy Accelerator Research Organization – KEK Lattice Field Theory on multi-PFLOPS computers German-Japanese.

Axial symmetry at finite temperature Guido Cossu High Energy Accelerator Research Organization – KEK Lattice Field Theory on multi-PFLOPS computers German-Japanese.
XQCD 2007T.Umeda (Tsukuba)1 Study of constant mode in charmonium correlators in hot QCD Takashi Umeda This talk is based on the Phys. Rev. D75 094502 (2007)

XQCD 2007T.Umeda (Tsukuba)1 Study of constant mode in charmonium correlators in hot QCD Takashi Umeda This talk is based on the Phys. Rev. D (2007)
1 A Model Study on Meson Spectrum and Chiral Symmetry Transition Da

1 A Model Study on Meson Spectrum and Chiral Symmetry Transition Da
1 Chiral Symmetry Breaking and Restoration in QCD Da Huang Institute of Theoretical Physics, Chinese Academy of

1 Chiral Symmetry Breaking and Restoration in QCD Da Huang Institute of Theoretical Physics, Chinese Academy of
O(N) linear and nonlinear sigma-model at nonzeroT within the auxiliary field method CJT study of the O(N) linear and nonlinear sigma-model at nonzeroT.

O(N) linear and nonlinear sigma-model at nonzeroT within the auxiliary field method CJT study of the O(N) linear and nonlinear sigma-model at nonzeroT.
QCD – from the vacuum to high temperature an analytical approach.

QCD – from the vacuum to high temperature an analytical approach.
Thermal 2007T.Umeda (Tsukuba)1 Constant mode in charmonium correlation functions Takashi Umeda This is based on the Phys. Rev. D75 094502 (2007) Thermal.

Thermal 2007T.Umeda (Tsukuba)1 Constant mode in charmonium correlation functions Takashi Umeda This is based on the Phys. Rev. D (2007) Thermal.
N F = 3 Critical Point from Canonical Ensemble χ QCD Collaboration: A. Li, A. Alexandru, KFL, and X.F. Meng Finite Density Algorithm with Canonical Approach.

N F = 3 Critical Point from Canonical Ensemble χ QCD Collaboration: A. Li, A. Alexandru, KFL, and X.F. Meng Finite Density Algorithm with Canonical Approach.
QCD – from the vacuum to high temperature an analytical approach an analytical approach.

QCD – from the vacuum to high temperature an analytical approach an analytical approach.
QCD – from the vacuum to high temperature an analytical approach an analytical approach.

QCD – from the vacuum to high temperature an analytical approach an analytical approach.
The XXV International Symposium on Lattice Field Theory 29 July - 5 August 2007, Regensburg, Deutschland K. Miura, N. Kawamoto and A. Ohnishi Hokkaido.

The XXV International Symposium on Lattice Field Theory 29 July - 5 August 2007, Regensburg, Deutschland K. Miura, N. Kawamoto and A. Ohnishi Hokkaido.
Fluctuations and Correlations of Conserved Charges in QCD at Finite Temperature with Effective Models Wei-jie Fu, ITP, CAS Collaborated with Prof. Yu-xin.

Fluctuations and Correlations of Conserved Charges in QCD at Finite Temperature with Effective Models Wei-jie Fu, ITP, CAS Collaborated with Prof. Yu-xin.

Similar presentations

Ads by Google