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Shinji Takeda Kanazawa U. in collaboration with Masashi Hayakawa, Shunpei Uno (Nagoya U.) Ken-Ichi Ishikawa, Yusuke Osaki (Hiroshima U.) Norikazu Yamada (KEK) Running coupling constant of ten-flavor QCD with the Schroedinger functional method arXiv: (will appear in PRD) Symposium on Lattice gauge theory at U. of Wuppertal 2/5/2011

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Contents I. Introduction Physics background Walking Technicolor Conformal window II. Lattice calculation of running coupling III. Summary

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I.Introduction

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Successes of Lattice QCD ‣ Hadron masses and their interactions ‣ ‣ The SM parameters ‣ Weak matrix elements ‣... Scholz lattice 2009 Lattice calculations truly reliable. Apply to Something different

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LHC era Use Lattice to explore LHC physics ‣ Higgs mechanism ‣ Physics above the EW scale ‣ Among many New Physics candidates, Technicolor is attractive and best suited for Lattice Simulation

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➜ New strong interaction SU(N TC ): technicolor ➜ At Λ TC ∼v weak, technifermion condensate 〈T R T L 〉 ➜ Gives dynamical SU(2) L xU(1) Y breaking ➜ New strong interaction SU(N TC ): technicolor ➜ At Λ TC ∼v weak, technifermion condensate 〈T R T L 〉 ➜ Gives dynamical SU(2) L xU(1) Y breaking Technicolor (TC) Technicolor (TC) [Weinberg(‘79), Susskind(‘79)] Alternative for Higgs sector of SM model No fine tuning ➜ 〈TT〉breaks chiral symmetry SU(2) L ×SU(2) R ➜ Produce technipion π TC (NG bosons) ➜ π TC become longitudinal components of W and Z ➜ M W = M z cosθ W = ½gF π (F π = v weak =246 GeV) ➜ 〈TT〉breaks chiral symmetry SU(2) L ×SU(2) R ➜ Produce technipion π TC (NG bosons) ➜ π TC become longitudinal components of W and Z ➜ M W = M z cosθ W = ½gF π (F π = v weak =246 GeV)

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Extended TC Eichten(‘80) Susskind(‘79) How do SM fermion get mass? ⇒ Extended TC ➜ New gauge theory SU(N ETC ), N ETC >N TC T ETC =(T TC,f SM ) ➜ Assuming SSB: SU(N ETC ) ➔ SU(N TC )xSM at Λ ETC >>Λ TC ➜ New gauge theory SU(N ETC ), N ETC >N TC T ETC =(T TC,f SM ) ➜ Assuming SSB: SU(N ETC ) ➔ SU(N TC )xSM at Λ ETC >>Λ TC : fermion mass : FCNC G ff TT

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Walking TC Holdom(‘81) Yamawaki et al. (‘86) Solving tension of SM fermion mass VS. FCNC μ M ETC g 2 (μ) g 2 SχSB M TC g 2 initial Classic TC or QCD-like theory Walking TC If γ=O(1): Large enhancement

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Find the location of N f c in various GT. Conformal Window SχSB & Confining Conformal Asymptotic non-free NfNf ⇦ QCD N f af NfcNfc 0 Speculation on “Phase diagram” of GT ⇦ WTC?

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Prediction phase (2013?-) Perform large-scale lattice simulation of candidate theories to find the precise values for f π, m ρ, (m σ ), Σ, S-parameter,... Searching phase (-2012?) Strategy on the lattice Now is in Searching phase. Prediction phase on the Next-Generation supercomputer? Calculate hadron spectrum to see scaling behavior Calculate running coupling and anomalous dimension directly on the lattice.

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So far, the following SU(Nc) gauge theories have been intensively studied Candidates for WTC NcNcNcNc NfNfNfNfRep. Running g 2 spectroscopy Large N f QCD 36~16fund. 8 < N c f <12 N c f >12 N c f <12 Large N f two-color QCD 26, 8fund. N c f <6 - Sextet QCD 32sextet conformal conformal confinment Two-color adjoint QCD 22adjoint conformal Currently, many contradictions and little consensus

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II.Lattice calculation of running coupling

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Machines used - (SR11K, BG/L) - GPGPU & CPU - INSAM GPU - GPGPU, GCOE cluster - B-factory computer system

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Schrödinger functional scheme Luescher, Weisz, Wolff, (’91) LuescherWeiszWolff SF coupling Standard background field Θ=0 PCAC mass=0 O(a) un-improved Wilson fermion Plaquette gauge action time (Dirichlet) space L (periodic up to exp(iθ) ） 0 L

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Anomalous dimension in SF scheme to 2-loop With g FP 2 for 3-loop β-function in SF scheme, Perturbation theory Perturbation is not reliable =>Use Lattice method! Perturbative IRFP(g FP 2 ) for SU(3) gauge theory

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8 & 12 flavor QCD Appelquist, Fleming, Neil, (‘08) N f = 8 N f = 12 g 2 IRFP ~ 5 consistent with PT prediction Conclusion: N f =12 is too large while N f =8 is too small. (12-flavor QCD is still under debate.)

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Raw data of each L/a is close to each other. ⇒ slow running 10 flavor QCD (This work)

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Step scaling function u=g 2 (L) g2g2 g02g02 L/a s×L/a Σ(u,s,a/L) Taking the continuum limit σ(u,s) = lim Σ(u,s,a/L), u=g SF 2 is not easy since O(a) improvement is not implemented Reducing discretization errors as much as possible before taking the limit is crucial. a/L→0

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“ 2-loop improvement ” PACS-CS Collaboration (‘09) ‣ Use weak coupling region to estimate the two-loop improvement coefficients. ‣ “2-loop” Improved step scaling function ： Deviation at 2- loop:

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Extrapolation to the continuum limit shows sign-flip before g SF 2 reaches about 10. Y. Shamir, B. Svetitsky and T. DeGrand, (‘08) Discrete beta function negativeconsistent with zeropositive

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Result suggests the existence of IRFP at g FP 2 = 3.3 ~ Where is IRFP?

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‣ σ P = Z P (s L) / Z P (L) ‣ Non-zero BG field ‣ For 3.3 < g 2 FP < 9.35, 0.28 < γ FP < 1.0 ! ‣ Precise value of g 2 FP is important Anomalous dimension Preliminary

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III.Summary

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Summary Lattice technique can be used to search for realistic WTC models and to see whether the long-standing (~30 yrs) problems in TC are really resolved by WTC. As a first step, we started with the study of running coupling of 10-flavor QCD to identify conformal window in SU(3) GT. The result shows an evidence of IRFP in 3.3 < g 2 FP < 9.4. ⇒ 8< N f c < < γ m < 1.0 is obtained from preliminary analysis. Pinning down γ m requires precise value of the IRFP. Next important task is to calculate S-parameter.

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