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Hong-Jian He Tsinghua University 9th ACFA ILC Workshop Physics Session Summary Feb. 4-7, 2007, IHEP, Beijing
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Consensus: “Future” of ILC strongly depends on What New Phys LHC will discover. LHC 2007-
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Zhengguo Zhao, ( Anomalous Gauge Boson Coupling ) Zhengguo Zhao, ( Anomalous Gauge Boson Coupling ) Diboson Production and Triple Gauge Boson Couplings at TeV Hadron Collider Diboson Production and Triple Gauge Boson Couplings at TeV Hadron Collider Denis Perret-Gallix, ( Calculation Tool: Grace ) Denis Perret-Gallix, ( Calculation Tool: Grace ) Simulate with Grace Simulate with Grace Kingman Cheung, ( Higgs: Very Light A 0 ) Kingman Cheung, ( Higgs: Very Light A 0 ) Phenomenology of the Light Pseudoscalar Boson in NMSSM Phenomenology of the Light Pseudoscalar Boson in NMSSM Eri Asakawa, ( Exotic Higgs-Gauge-Coupling: H + W - Z 0 ) Eri Asakawa, ( Exotic Higgs-Gauge-Coupling: H + W - Z 0 ) Potential for Measuring the H + W - Z 0 vertex at colliders Potential for Measuring the H + W - Z 0 vertex at colliders Liang Han, ( NLO EW Corrections ) Liang Han, ( NLO EW Corrections ) Theoretical Calculation for ILC Precise Measurement Theoretical Calculation for ILC Precise Measurement Jin Min Yang, ( SUSY: Splitting Model ) Jin Min Yang, ( SUSY: Splitting Model ) Split Supersymmetry at ILC Split Supersymmetry at ILC Shou-hua Zhu, ( Exotic Higgs A 0 : 0.215GeV ) Shou-hua Zhu, ( Exotic Higgs A 0 : 0.215GeV ) Unique Higgs Boson Signature at Colliders Unique Higgs Boson Signature at Colliders Koichi Matsuda, ( Anomalous Higgs Yukawa: ee→ννtt, ee→htt ) Koichi Matsuda, ( Anomalous Higgs Yukawa: ee→ννtt, ee→htt ) New Physics Search by Helicity Decomposition of Heavy Fermion Pair-Production from W-boson Fusion at LHC/ILC New Physics Search by Helicity Decomposition of Heavy Fermion Pair-Production from W-boson Fusion at LHC/ILC Hideo Itoh, ( SUSY-breaking/brane world: TeV-scale X ) Hideo Itoh, ( SUSY-breaking/brane world: TeV-scale X ) Low scale supergravity mediation in brane world scenario Low scale supergravity mediation in brane world scenario and hidden sector Phenomenology and hidden sector Phenomenology W. Lohmann, ( Higgs: Detector Full simulation/Reconstruction ) W. Lohmann, ( Higgs: Detector Full simulation/Reconstruction ) Study of ee→Zh→llX using full detector simulation and exact reconstruction Study of ee→Zh→llX using full detector simulation and exact reconstruction
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Central Physics Issues for LHC & ILC Why TeV Scale ? What New Physics ? How to Compute/Observe: Signals vs Bkgnds ? How does ILC play Complementarity to LHC?
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New Physics at TeV Scale ?? Which is Guaranteed ?? Higgsless Higgs
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Hierarchy/Fine-Tuning Problem ? → Not strong enough ! → Not strong enough ! Unification ? → Many possible realizations ! → Many possible realizations ! Light Higgs ? → Not enforced by data ! → Not enforced by data ! Then, WHAT best justifies TeV Scale? … WHAT best justifies TeV Scale? … New Physics at TeV Scale ?
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Fine-Tuning Problem ? Fine-Tuning Problem ? ● Radiative Corrections to Higgs Mass: ● Degree of Fine-Tuning (DFT): DFT = 200 2 /[|-2000 2 +520 2 +460 2 |*(Λ/10TeV) 2 ]
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Fine-Tuning is a Technical Problem ! Fine-Tuning is a Technical Problem ! Not strong enough for LHC/ILC! Λ=11TeV 3.5TeV 2.5TeV
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SM Higgs Potential runs into more serious Vacuum Energy Problem even at Tree-Level: ( eg, S.Weinberg,1989 ) = V min – λv 4 /4 = V min - O(100GeV) 4 == (10 - 4 eV) 4 → 60 Orders of Magnitude Fine-tuning ! → So, Why do we care 1% Tuning at 1-Loop ?!
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Unification without SUSY? Unification without SUSY? → YES. → Many possible realizations !!! Trinification with just 6 Higgs doublets (Willenbrock et al, 2003) 5d TeV GUT with just 3 real scalars of SU(2)-adjoint (Dienes etal, 1998) And more: Efficacious Unification with 2 scalar octocts, 1 triplet scalar, 1 triplet majorana fermiom, which also predicts dark matter, as good as Splitting SUSY (E. Ma, 05), ……… Trinification 5d TeV GUT
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A Misconception: Light Higgs from Data ? 114.4 < M H < 260GeV (95%CL) → Could be True Only If No New Physics & Higgs was Exactly SM-like!
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Heavy Higgs vs Precision Data: No Problem ! Heavy Higgs vs Precision Data: No Problem ! R. S. Chivvukula, Snowmass-2001H. J. He, Snowmass-2001 Top Seesaw Model
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SUSY with Heavy Higgs: OK… Called “λSUSY” See Y. Nomura’s talk, hep-ph/0607332 ● λSH 1 H 2 remains perturbative up to about 10TeV ● M h is heavy, up to 300GeV ● Higgs/Higgsino: 200-700GeV
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Lesson for LHC & ILC: Lesson for LHC & ILC: Keep Your Mind Fully Open !!! Keep Your Mind Fully Open !!!
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The Real Problem with Particle Masses is Unitarity Violation Unitarity Violation in the High Energy Scattering !!!!!
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Unitarity of W L W L → W L W L : Electroweak Symmetry Breaking Scale Unitarity of W L W L → W L W L : Electroweak Symmetry Breaking Scale → Stronger & More Robust than Fine-tuning bound !
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Scales of Fermion Mass Generation
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→ Future: After LHC/ILC !
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K. Cheung’s talk: NMSSM How to Observe ? Large tanβ & v s J.M. Yang’s talk: Splitting SUSY S.H. Zhu’s Talk ee→Zh →Z+4μ
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Probing Higgsless Parameters: E vs Polarization Han, He, Yuan
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Higgsless Model: New W’ at ILC
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Conclusions Conclusions Why TeV Scale: Unitarity of W L W L → W L W L ILC must be upgradeable to 1TeV ! ILC must be upgradeable to 1TeV ! What New Physics: Many Kinds – Keep your Mind Open !!! Light Higgs or Heavy Higgs or Higgsless; Light Higgs or Heavy Higgs or Higgsless; SUSY or Splitting SUSY or SUSY-Less; SUSY or Splitting SUSY or SUSY-Less; 4-Dimension or Extra-d or Deconstruction… 4-Dimension or Extra-d or Deconstruction… How to Compute/Observe at ILC: Signals vs Bkgnds New Channels, Beam polarizations, New Channels, Beam polarizations, e-e- Mode, Photon-collider, …… e-e- Mode, Photon-collider, …… ILC plays Complementarity: Precision Test, Loop Effects, …… Precision Test, Loop Effects, ……
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Back Up Slides Back Up Slides
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VLHC: http://vlhc.org (50-200TeV)http://vlhc.org
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New Phys
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LHCILC
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Importance of Photon Collider & Polarization (Charged Higgs Boson Production)
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Different SUSY Breakings and Particle Spectrum: Need Precision Tests at ILC !
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