Gauge independence of Abelian confinement mechansim in SU2 gluodynamics T. Suzuki, Kanazawa Univ., Japan (In collab. with T.Sekido, K.Ishiguro, Y.Koma)

Slides:

Advertisements

Similar presentations

Closed k-strings in 2+1 dimensional SU(N c ) gauge theories Andreas Athenodorou St. John’s College University of Oxford GradCATS 2008 Mostly based on:

Advertisements

Two questions: (1) How to find the force, F on the electric charge, Q excreted by the field E and/or B? (2) How fields E and/or B can be created?

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

Duality and Confinement in the Dual Ginzburg-Landau Superconductor Physics Beyond Standard Model – 1st Meeting Rio-Saclay 2006 Leonardo de Sousa Grigorio.

Štefan Olejník Institute of Physics, Slovak Academy of Sciences, Bratislava, Slovakia Coulomb energy, remnant symmetry in Coulomb gauge, and phases of.

Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does.

Quark-quark interaction in baryons from Nambu-Bethe-Salpeter amplitudes on lattice Hideaki Iida (Kyoto Univ.) in collaboration with Yoichi Ikeda (Tokyo.

Lecture 17-The Magnetic Field Chapter 24 Friday, March 6.

1 Nuclear Binding and QCD ( with G. Chanfray) Magda Ericson, IPNL, Lyon SCADRON70 Lisbon February 2008.

From gluons to hybrids : Coulomb gauge perspective Adam Szczepaniak IU Gluons and glueballs in Coulomb gauge Gluelumps and Hybrids Spectrum of gluonic.

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

Heavy quark potential and running coupling in QCD W. Schleifenbaum Advisor: H. Reinhardt University of Tübingen EUROGRADworkshop Todtmoos 2007.

何汉新（ Han-Xin He ）中国原子能科学研究院 China Institute of Atomic Energy Quark Confinement Dynamics.

Lecture 3: The Standard Model

Color confinement mechanism and the type of the QCD vacuum Tsuneo Suzuki (Kanazawa Univ.) Collaborators: K.Ishiguro, Y.Mori, Y.Nakamura, T.Sekido （ M.Polikarpov,

JOINT INSTITUTE FOR POWER&NUCLEAR RESEARCH – SOSNY NATIONAL ACADEMY OF SCIENCES OF BELARUS 22010, Minsk, krasin str., 99 krasin str., 99 Tel.:

What we expect gauge/gravity duality in the near future: from the viewpoint of hydrodynamics and thermodynamics CQUeST and Hanyang Univ. Shin Nakamura.

Yang-Mills Theory in Coulomb Gauge H. Reinhardt Tübingen C. Feuchter & H. R. hep-th/ , PRD70 hep-th/ , PRD71 hep-th/ D. Epple, C. Feuchter,

1 Dynamical Holographic QCD Model Mei HUANG Institute of High Energy Physics, CAS Theoretical Physics Center for Science Facilities, CAS Seminar at USTC,

The relationship between a topological Yang-Mills field and a magnetic monopole RCNP, Osaka, 7 Dec Nobuyuki Fukui (Chiba University, Japan) Kei-Ichi.

Analytical derivation of gauge fields from link variables in SU(3) lattice QCD and its application in Maximally Abelian gauge S.Gongyo(Kyoto Univ.) T.Iritani,

XI ｔｈ International Conference on Quark Confinement and the Hadron Petersburg, Russia Philipp Gubler (RIKEN, Nishina Center) Collaborator:

Confinement mechanism and topological defects Review+ papers by A.V.Kovalenko, MIP, S.V. Syritsyn, V.I. Zakharov hep-lat/ , hep-lat/ , hep-lat/

Physics 106 Lesson #16 Capacitors Dr. Andrew Tomasch 2405 Randall Lab

Electric charge, electric field, static charge an charge by induction.

Entanglement Entropy in Holographic Superconductor Phase Transitions Rong-Gen Cai Institute of Theoretical Physics Chinese Academy of Sciences (April 17,

Static interquark potentials from lattice QCD Toru T. Takahashi (Gunma College of Technology)

Reinterpretation of Skyrme Theory Y. M. Cho Seoul National Univ.

Lattice results on QCD-strings N.D. Hari Dass Institute of Mathematical Sciences Chennai In collaboration with Dr Pushan Majumdar, U. Muenster.

Quick Practice In what direction is the magnetic force on the wire?

Discrete R-symmetry anomalies in heterotic orbifold models Hiroshi Ohki Takeshi Araki Kang-Sin Choi Tatsuo Kobayashi Jisuke Kubo (Kyoto univ.) (Kanazawa.

Hank Thacker University of Virginia References: J. Lenaghan, S. Ahmad, and HT Phys.Rev. D72: (2005) Y. Lian and HT, Phys. Rev. D75: (2007),

Peristaltic modes of single vortex in U(1) and SU(3) gauge theories Toru Kojo (Kyoto University) Kyosuke Tsumura (Fuji film corporation) Hideo Suganuma.

Heavy quark potential at non-zero temperature Péter Petreczky Hard Probes 2013, Stellenbosch, South Africa, November 4-8, 2013 Motivation : the study and.

WHOT-QCD Collaboration Yu Maezawa (RIKEN) in collaboration with S. Aoki, K. Kanaya, N. Ishii, N. Ukita, T. Umeda (Univ. of Tsukuba) T. Hatsuda (Univ. of.

VORTEX SOLUTIONS IN THE EXTENDED SKYRME FADDEEV MODEL In collaboration with Luiz Agostinho Ferreira, Pawel Klimas (IFSC/USP) Masahiro Hayasaka (TUS) Juha.

MEM Analysis of Glueball Correlators at T>0 speaker Noriyoshi ISHII (RIKEN, Japan) in collaboration with Hideo SUGANUMA (TITECH, Japan) START.

PARALLEL PLATES. From previous work, the electric field strength can be found from the electric force on a test charge.

20 Magnetic Field & Forces. Magnetism S N S N Extended…

1 CONFINING INTERQUARK POTENTIALS FROM NON ABELIAN GAUGE THEORIES COUPLED TO DILATON Mohamed CHABAB LPHEA, FSSM Cadi- Ayyad University Marrakech, Morocco.

Gribov copy problem in lattice gauge theory simulation Bornyakov Vitaly IHEP & ITEP ICHEP

Lattice 2006 Tucson, AZT.Umeda (BNL)1 QCD thermodynamics with N f =2+1 near the continuum limit at realistic quark masses Takashi Umeda (BNL) for the RBC.

1 By: Ryan Shanahan How magnetic fields are Made?.

Inter-Quark Potentials in Baryons and Multi-Quark Systems in QCD H. Suganuma, A. Yamamoto, H. Iida, N. Sakumichi (Kyoto Univ.) with T.T.Takahashi (Kyoto.

1 Heavy quark potential in full QCD lattice simulations at finite temperature Yuu Maezawa (The Univ. of Tokyo) Tsukuba-Tokyo collaboration Univ. of Tsukuba.

K.M.Shahabasyan, M. K. Shahabasyan,D.M.Sedrakyan

Localization of the scalar and fermionic eigenmodes and confinement J. Greensite, F.V. Gubarev, A.V.Kovalenko, S.M. Morozov, S. Olejnik, MIP, S.V. Syritsyn,

Electric Field Lines Contents: Basic Concept Field Lines and point charges Field Lines and conductors.

The magnetic force on the moving charges pushes the wire to the right.

Hadron 2007 Frascati, October 12 th, 2007 P.Faccioli, M.Cristoforetti, M.C.Traini Trento University & I.N.F.N. J. W. Negele M.I.T. P.Faccioli, M.Cristoforetti,

関戸暢石黒克也、森祥寛、中村宜文、鈴木恒雄 Kanazawa-univ & RIKEN 共同研究者 Kanazawa-univ & RIKEN Gauge invariance of the dual Meissner effect in pure SU(2) QCD.

Gauge independence of Abelian dual Meissner effect in pure SU(2) QCD Katsuya Ishiguro Y.Mori, T.Sekido, T.Suzuki Kanazawa-univ & RIKEN Joint Meeting of.

P-Term Cosmology A.C. Davis (with C. Burrage) ,

Magnetism. Magnets  Poles of a magnet are the ends where objects are most strongly attracted Two poles, called north and south  Like poles repel each.

Inter-quark potential from NBS wavefunction on lattice H.Iida (Kyoto Univ.), Y.Ikeda (Tokyo Inst. of Tech) 新学術領域「素核宇宙融合」 x 「新ハドロン」クロスオーバー研究会 July,

Chapter 21 Magnetic Induction and Chapter 22.9: Transformers.

Producing Magnets with Moving CHarge Magnets have two ends – poles – called north and south. Like poles repel; unlike poles attract.

Confinement and Bags Governed by SSB of Scale Invariance (E. G. Int. J

Study of the structure of the QCD vacuum

Nc=2 lattice gauge theories with

P. Gubler, T.T. Takahashi and M. Oka, Phys. Rev. D 94, (2016).

Monopoles The Mystery.

Electric Charge and Static Electricity

Dark Photon Search At A Circular Collider

QCD thermodynamics on QCDOC Machine

Neutron EDM with external electric field

Masakazu Sano Hokkaido University

in collaboration with G. Ishiki, S. Shimasaki

Fig. 4 Characterizing phase transitions of matter coupled to a ℤ2 gauge field in a two-leg ladder. Characterizing phase transitions of matter coupled to.

Presentation transcript:

Gauge independence of Abelian confinement mechansim in SU2 gluodynamics T. Suzuki, Kanazawa Univ., Japan (In collab. with T.Sekido, K.Ishiguro, Y.Koma) Lattice /7/2007

Surprizing results: 1. Extraction of the confining component in gauge fields is possible without cooling or any gauge fixing. Gauge independence 2. Abelian and monopole dominances are almost perfect. 3. Squeezing of electric fields occurs due to solenoidal monopole currents. The Abelian dual Meissner effect is working. The vacuum is near the border between type 1 and 2 superconductor. 4. Confinement of non-Abelian color charge is explained in the framework of the Abelian dual Meissner effect.

1. Extraction of confining component Non-perturbative confining component

2-1. Abelian dominance

Abelian static potential Error bars are very small.

Force from Abelian static potential Consistent with theoretical works ( ’ 99 Ogilvie, Faber et al. )

2-2 Monopole dominance

Noise reduction method using random gauge transformations

Abelian, monopole and photon static potentials

Forces

String tensions Monopole dominance as well as Abelian dominance are seen very beautifully. Both are much better than in MA gauge.

3. Squeezing of electric field flux Connected correlations between NA Wilson loop and Abelian operators

Dual Meissner effect Monopoles are responsible for the dual Meissner effect.

Vacuum type Errors are still too large. We need more statistics on larger lattice.

4. Color confinement from Abelian picture

Surprizing results: 1. Extraction of the confining component in gauge fields is possible without cooling or any gauge fixing. Gauge independence 2. Abelian and monopole dominances are almost perfect. 3. Squeezing of electric fields occurs due to solenoidal monopole currents. The Abelian dual Meissner effect is working. The vacuum is near the border between type 1 and 2 superconductor. 4. Confinement of non-Abelian color charge is explained in the framework of the Abelian dual Meissner effect.