Physics Overview Yasuhiro Okada KEK LCWS 06 ILC

Physics Overview Yasuhiro Okada (KEK) LCWS 06 & ILC GDE meeting, March 9, 2006 Indian Institute of Science, Bangalore, India 1

Fundamental questions in elementary particle physics What are the elementary constituents of matter? n What are forces acting between them? n How has the Universe begun and evolved? n 2

How have we come to the Standard Model ? gravity general relativity EM interaction Electroweak theory Higgs mechanism weak interaction Fermi theory strong interaction nuclear force 1900 pion quark QCD 2000 3

Why Te. V scale? n n n This is the scale of the weak interaction, in modern language, the Higgs vacuum expectation value (~246 Ge. V). We expect to fine a Higgs boson and “New Physics” associated to the electroweak symmetry breaking. The answer to the question “what is the physics behind the electroweak symmetry breaking? ” is a crucial branching point for the future of particle physics. Supersymmetry vs. Low cut-off theory (Little Higgs models, models with large extra-dimension, etc. ) 4

Why do we expect physics beyond the Standard Model? n n n We do not know how the Higgs field arises. There are evidences which require new particles and/or new interactions. Neutrino mass Dark matter Baryon-anti-baryon asymmetry of the Universe Expectation of Unification. GUT, Superstring 5

Why do we need both LHC & ILC? n n Two machines have different characters. Advantage of lepton colliders: e+ and e- are elementary particle (well-defined kinematics). Less background than LHC experiments. Beam polarization, energy scan. g - g, e- e- options, Z pole option. LHC ILC 6

Goals of ILC physics Higgs physics (Electroweak symmetry breaking and mass generation mechanism of quarks, leptons, and gauge bosons. ) n New physics signals Direct search for new particles and interactions. Indirect search for new physics effects through the SM particle processes. Capability of precise measurements of various quantities is a key. n 7

Higgs physics n n A Higgs boson will be discovered at LHC as long as its properties (production/decay) is similar to the SM Higgs boson. In order to study the Higgs mechanism at work, Higgs couplings to various particles have to be measured precisely. 8

Higgs boson search at LHC SM Higgs boson branching ratio Higgs boson discovery at LHC 5 MH(Ge. V) 9

Coupling measurements at ILC (Ecm>700 Ge. V) LHC: (10)% for ratios of coupling constants ILC: a few % determination Higgs self-coupling GLC Project m. H=120 Ge. V, Ecm=300 -500 Ge. V. L=500 fb-1 10

New physics effects in Higgs boson couplings n In many new physics models, the Higgs sector is extended and /or involves new interactions. The Higgs boson coupling can have sizable deviation from the SM prediction. The heavy Higgs boson mass in the MSSM B(h->WW)/B(h->tt) SUSY correction to Yukawa couplings B(h->bb)/B(h->tt) LC LHC LC ACFA report J. Guasch, W. Hollik, S. Penaranda 11

Radion-Higgs mixing in extra-dim model The triple Higgs coupling in 2 HDM in the electroweak baryogenesis scenario HEPAP report Little Higgs model with T parity S. Kanemura, Y. Okada, E. Senaha Deviation to 5 -10 % level can be distinguished at ILC C. -R. Chen, K. Tobe, C. -P. Yuan 12

Direct searches for New Physics n n Some type of new signals is expected around 1 Te. V range, if New Physics is related to a solution of the hierarchy problem. (SUSY, Large extra-dimension, etc ) The first signal of New Physics is likely to be obtained at LHC. (ex. squarks up to 2. 5 Te. V at LHC) ILC experiments are necessary to figure out what is New Physics, by measuring spin, quantum numbers, coupling constants of new particles, and finding lower mass particles which may escape detection at LHC. Beam polarization, energy scan, and well-defined initial kinematics play important roles in ILC studies. 13

SUSY studies at ILC SUSY is a symmetry between fermions and bosons. Spin determination is essential, ideal for ILC. SM particles Super partners quark Spin 1/2 lepton Spin 0 squark slepton gluon Spin 1 W, Z, g, H Spin 1 Spin 0 Spin 1/2 gluino Spin 1/2 neutralino, chargino neutralino mixing chargino mixing Mixing angle determination 14

SUSY relation SUSY predicts characteristic relations among superpartner’s interactions. Right-handed selectron production M. M. Nojiri, K. Fujii, and T. Tsukamoto 15

GUT relation Gaugino mass relation If we combine information from LHC and LC, we can test whether SUSY breaking masses satisfy GUT and/or Unification conditions Gauge coupling unification Scalar mass relation B. C. Allanach, et al in LHC/LC report 16

Dark matter and collider physics n n n Energy composition of the Universe Dark energy 73% Dark matter 23% Baryon 4% Dark matter candidate WIMP （weakly interacting massive particle) a stable, neutral particle WIMP candidates Neutralino (SUSY) KK-photon (UED) Heavy photon (Little Higgs with T parity)… 17

Dark matter profile in our galaxy Thermal history of the Universe Cosmological parameter determination WMAP, Planck, … Thermal relic abundance Direct and indirect (g, e+, anti-p, n ) searches for dark matter Detection rate Collider search for a dark matter candidate particle at LHC and ILC will play a particularly important role in distinguishing different models and determine properties of the dark matter candidate. See, E. A. Baltz, M. Battaglia, M. E. Peskin, and T. Wizansky, hep-ph/0602187 18

SUSY Dark matter at ILC SUSY mass and coupling measurements => Identification of dark matter ALCPG cosmology subgroup 19

Precision measurements of SM processes n n Improve precision of the fundamental parameters. Search for new physics in indirect ways. The threshold scan improves the top mass measurement and determines the top width. Top quark threshold scan Deviation of the top width in the Little Higgs model. C. F. Berger, M. Pelestein, F. Petriello GLC report 20

Z’ and e+e-->ff processes Z’ coupling determination at ILC Even if ILC at 500 Ge. V cannot produce a new Z’ particle kinematically, we can determine left-handed and right-handed couplings from ee-> ff processes. This will give important information to identify the correct theory. LHC=> mass ILC => coupling e f Z’ e f m z’ =2 Te. V, Ecm=500 Ge. V, L=1 ab-1 with and w/o beam polarization S. Godfrey, P. Kalyniak, A. Tomkins 21

Conclusions n n The LHC experiment is expected to open a new era of the high energy physics by finding a Higgs boson and other new particles. Establishing the mass generation mechanism is the urgent question. This will be achieved by precise determination of the Higgs couplings, and ILC will play essential roles. In order to explore New Physics, Higgs coupling measurements, direct study of new particles and new phenomena, and indirect searches through SM processes are all important at ILC. Te. V physics explored at LHC and ILC will lead to new understanding of unification and cosmology. 22