ILC TDR v2: Physics, arXiv:1306.6352 ILC TDR Launch ILC TDR Launch Brock and Snowmass 2013 Snowmass 2013 H Yamamoto.

Slides:



Advertisements
Similar presentations
Kiwoon Choi PQ-invariant multi-singlet NMSSM
Advertisements

SUSY and other BSM physics with CMS
Outlook: Higgs, SUSY, flavor Ken-ichi Hikasa (Tohoku U.) Fourth Workshop, Origin of Mass and SUSY March 8, 2006, Epochal Tsukuba.
The minimal B-L model naturally realized at TeV scale Yuta Orikasa(SOKENDAI) Satoshi Iso(KEK,SOKENDAI) Nobuchika Okada(University of Alabama) Phys.Lett.B676(2009)81.
The classically conformal B-L extended standard model Yuta Orikasa Satoshi Iso(KEK,SOKENDAI) Nobuchika Okada(University of Alabama) Phys.Lett.B676(2009)81.
Compelling Questions of High Energy Physics? What does the future hold? Persis S. Drell Physics Department Cornell University.
Flavor Beyond the Standard Model Zurab Tavartkiladze, Gela Devidze Tbilisi State University Volkswagen meeting 14, 15 March 2013, Tbilisi.
Common Benchmarks for FCC Physics John Ellis King’s College London & FCC-ee/TLEP7 Workshop.
F. Richard Feb 2003 A Z’ within the ‘Little Higgs’ Scenario The LHC/LC Study group meeting CERN.
Comprehensive Analysis on the Light Higgs Scenario in the Framework of Non-Universal Higgs Mass Model M. Asano (Tohoku Univ.) M. Senami (Kyoto Univ.) H.
3.Phenomenology of Two Higgs Doublet Models. Charged Higgs Bosons.
Little Higgs Model Dark Matter and Its Implications at the LHC Chuan-Ren Chen (NTNU) KIAS-NCTS Joint Workshop High-1 2/9 – 2/15 In collaboration.
Little Higgs Dark Matter and Its Implications at the LHC Chuan-Ren Chen (NTNU) XS 2014, 5/6/2014 In collaboration with H-C Tsai, M-C Lee, [hep-ph]
Yingchuan Li Weak Mixing Angle and EIC INT Workshop on Pertubative and Non-Pertubative Aspects of QCD at Collider Energies Sep. 17th 2010.
Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u.
K. Kumar, W. Marciano, Y. Li Electroweak physics at EIC - Summary of week 7 INT Workshop on Pertubative and Non-Pertubative Aspects of QCD at Collider.
JoAnne Hewett, SLAC Scientific Opportunities at a Linear Collider: Making the Case.
.. Particle Physics at a Crossroads Meenakshi Narain Brown University.
Paris 22/4 UED Albert De Roeck (CERN) 1 Identifying Universal Extra Dimensions at CLIC  Minimal UED model  CLIC experimentation  UED signals & Measurements.
Mitsuru Kakizaki (University of Toyama)
1 New Frontiers in Particle Physics Jeff Forshaw University of Manchester.
LHC’s Second Run Hyunseok Lee 1. 2 ■ Discovery of the Higgs particle.
James Stirling IPPP, University of Durham with acknowledgements to R Barbieri, J Ellis, D Miller (ICHEP04), M Peskin (Victoria LCW), S. Dawson, R. Heuer.
SUSY Dark Matter Collider – direct – indirect search bridge. Sabine Kraml Laboratoire de Physique Subatomique et de Cosmologie Grenoble, France ● 43. Rencontres.
Physics Session Summary Nobuchika Okada Institute of Particle and Nuclear Studies, High Energy Accelerator Research Organization (KEK) TILC09, Tsukuba,
Tension Between A Fourth Generation And The LHC Higgs Searches Xiao-Gang He (SJTU&NTU) Xiao-Gang He and German Valencia, arXiv: Xiao-Gang He and.
SY Choi (Chonbuk, Korea) Highlighting “central HEP targets of ILC” based on Physics Chapter of RDR and many review talks/reports Leaving “cosmological.
FZÚ, J. Cvach, LCWS051 LCWS 05 1.LHC a ILC 2.Top 3.Higgs 4.Polarizace.
Supersymmetric Models with 125 GeV Higgs Masahiro Yamaguchi (Tohoku University) 17 th Lomonosov Conference on Elementary Particle Physics Moscow State.
DARK MATTER CANDIDATES Cody Carr, Minh Nguyen December 9 th, 2014.
1 Summary talk for ILC Physics Yasuhiro Okada (KEK) November 12, 2004 ACFA LC7, Taipei.
ILC Physics a theorist’s perspective Koji TSUMURA (Kyoto from Dec 1 st ) Toku-sui annual workshop 2013 KEK, Dec , 2013.
1 Supersymmetry Yasuhiro Okada (KEK) January 14, 2005, at KEK.
INVASIONS IN PARTICLE PHYSICS Compton Lectures Autumn 2001 Lecture 8 Dec
Standard Model and Beyond Kiwoon Choi Physics at LHC and beyond Rencontres du Vietnam 2014 The IBS Center for Theoretical Physics of the Universe, South.
1 ILC の物理 岡田安弘 (KEK) ILC 測定器学術創成会議 2006年6月28日 KEK.
Lepton Physics One of the four pillars: Tera-Z, Oku-W, Mega-H, Mega-t John Ellis M = ± 0.8 GeV, ε =
Yingchuan Li Electroweak physics at EIC Brookhaven National Lab Feb. 3rd 2011, BNL.
Dark matter and hidden U(1) X (Work in progress, In collaboration with E.J. Chun & S. Scopel) Park, Jong-Chul (KIAS) August 10, 2010 Konkuk University.
Summary of Group C B. Barish, F. Boruzmati, A. Cohen, M. Endo, K. Fujii, M. Ibe, A. Ishikawa, S. Kanemura, E. Kato, R. Kitano, J. Lykken, M. Nojiri, T.
1 Higgs Physics Yasuhiro Okada (KEK) November 26, 2004, at KEK.
The Search For Supersymmetry Liam Malone and Matthew French.
Higgs boson pair production in new physics models at hadron, lepton, and photon colliders October Daisuke Harada (KEK) in collaboration.
The Standard Model of the elementary particles and their interactions
Charged Higgs boson at the LHC 이강영 ( 건국대학교 연세대학교
Jonathan Nistor Purdue University 1.  A symmetry relating elementary particles together in pairs whose respective spins differ by half a unit  superpartners.
Impact of quark flavour violation on the decay in the MSSM K. Hidaka Tokyo Gakugei University / RIKEN, Wako Collaboration with A. Bartl, H. Eberl, E. Ginina,
1 Overview of physics RDR and the next step Yasuhiro Okada (KEK/Sokendai) March 3, 2008 TILC08, Sendai, Japan.
03/31/2006S. M. Lietti - UED Search at SPRACE 1 Universal Extra Dimensions Search at SPRACE S. M. Lietti DOSAR Workshop at U.T. Arlington.
1 ILC Physics DCR Yasuhiro Okada (KEK) on behalf of the editors for DCR Physics Part, Abdelhak Djouadi, Joe Lykken, Klaus Moenig,Yasuhiro Okada, Mark Oreglia,
Future Colliders Gordon Watts University of Washington/Seattle APS NW Meeting May 12-14, 2016.
New Physics effect on Higgs boson pair production processes at LHC and ILC Daisuke Harada (KEK, Graduate University for Advanced Studies) in collaboration.
February 12, 2003ACFA LC Symposium 1 JLC Physics Yasuhiro Okada (KEK) ACFA LC Symposium February 12, 2003,Tsukuba, Japan.
Global Analysis, Combination & Complementarity The vision: explore 10 TeV scale directly (100 TeV pp) + indirectly (e + e - )
Hong-Jian He Tsinghua University Physics Case for Circular Colliders Physics Case for Circular Colliders International WS on FHECC, IHEP, Beijing, Dec.16-17,
Hong-Jian He Tsinghua University 9th ACFA ILC Workshop Physics Session Summary Feb. 4-7, 2007, IHEP, Beijing.
Energy Frontier: Higgs Boson Physics at Hadron Colliders Sally Dawson (BNL), Andrei Gritsan (Johns Hopkins), Rick Van Kooten (Indiana), Heather Logan (Carleton),
Determining the CP Properties of a Light Higgs Boson
Summary Session 3 Standard Model and Beyond
Dark Sectors for and anomalies
Physics Overview Yasuhiro Okada (KEK)
Ron Settles MPI-Munich
Higgs and SUSY at future colliders
ILC and future high energy physics
Physics at a Linear Collider
Physics Overview Yasuhiro Okada (KEK)
Yasuhiro Okada (KEK) April 17, 2003, CAT, Indore, India
Physics Overview Yasuhiro Okada (KEK)
SUSY SEARCHES WITH ATLAS
LHC: Seeking the Origin of Symmetry Breaking and Mass
Presentation transcript:

ILC TDR v2: Physics, arXiv: ILC TDR Launch ILC TDR Launch Brock and Snowmass 2013 Snowmass 2013 H LP 2013 H LP2013 Various Google Images … 10th LHC Physics Monthly KIAS on 13/Dec/2013 S.Y. Choi (Chonbuk, Korea) LHC ☞ ILC Physics : Why & How Introduction (ILC) Standard Physics (Higgs) New Physics (SUSY) How to go ahead

Introduction

Cosmic Uroboros Particle physics studies the fundamental nature of energy, matter, space and time, and applies the knowledge to understand the birth, evolution and fate of the Universe.

Neutrino Mass Theory of Flavor Higgs Boson Naturalness Matter Asymmetry Dark Matter Dark Energy Inflation … What we know is a droplet, while what we don’t know is an ocean Mysteries of the Universe (a partial list) [Fermi Today Nov/15, 2013] TeV-scale

Scenarios ⇔ Questions

I attach more value to finding a fact, even about the slightest thing, than to lengthy disputations about the Greatest Questions that fail to lead to any truth whatever. Galileo Galilei [Quigg]

Higgs-dependence Day

Perfect? Higgs Lamp Post M H = 125 GeV J P = 0 + v=246 GeV ↓ m[W, Z, f, H] [H Murayama] [Nobel prize website]

3 Major Frontiers Omni-directional Exploration

Precision experiments Discovery through inducing quantum loops Neutrino experiments Discovery by inducing quantum mixing Astrophysical experiments Discovery by capturing cosmic quanta Colliding beam experiments Discovery by producing on-shell states … Entangled Approaches

Energy Frontier Proposals [For details, Yamamoto’s talk]

LHC ☞ ILC real design [Yokoya’s talk] Most feasible and realistic

[Yokoya & ES Kim] [Yamamoto & IH Park] Two-minute Introduction Clean and Controllable

Physics at the ILC : determined by experimental data A Higgs particle Top quark Gauge bosons : W and Z … Clear physics case “Likely” (additional) physics case Anomalous (g-2) μ Dark matter … [SH Jung’s talk] Clarified more by next LHC experiments GigaZ

Standard Physics (Higgs) [For details, see Tanabe’s talk] Precision

The new world with a Higgs discovery Time to analyze!!! Urgent experimental checks for the SM Higgs boson or not elementary and single? Any deviation ⇒ BSM physics!

Outline of a precision Higgs program Experimental and theoretical requirements Projections of Higgs coupling accuracy Measurement potential at future colliders Projection of Higgs property studies Mass, spin-parity, CP mixture, etc Extended Higgs boson sectors Phenomenology and prospects for discovery Higgs Themes [P Ko’s talk]

Models with new TeV-scale particles give corrections to Higgs couplings of a few % An experimental program to determine these couplings is achievable LHC is the facility to study Higgs in the next decade Interesting precision begins with 300/fb running Success requires considerable theoretical effort Lepton colliders are required in order to measure sub-% precision in couplings in a model-independent fashion With access to invisible and exotic decay modes Higgs Couplings

Model-independent x-section and coupling measurement A dream case

New particles are around 1 TeV Coupling measurements [For details, see Tanabe’s talk]

Clear and big improvement from ILC measurements?! [Peskin]

Any deviation from the straight line ⇒ BSM physics Putting everything together SM Higgs Mechanism: Mass ∝ Coupling [ILC TDR 2013]

Precision neutral-current measurements predicted M W/Z UA1/UA2 discovered W/Z bosons LEP nailed the SM gauge sector Precision W/Z measurements predicted M H LHC discovered a Higgs particle ILC nails the Higgs sector Precision H measurements predict ? ?? ??? Repeated History of Collider Experiments? [H Murayama]

New Physics (SUSY) [For details, see Tanabe’s talk] Complementary

The questions of fine tuning is still open Dark matter (particle) is not included Neutrino masses are not included (g-2) μ with ~4σ discrepancy Gravity is not included … TeV-scale particle candidates Weakly coupled: SUSY, DM, Long-lived Strongly coupled/composite: RS, KK and Z’, long-lived … Evolution towards robust search strategies SM is NOT the ultimate theory

Natural hierarchy, unification, DM, (g-2) μ, more Higgs bosons, etc SUSY as a Show Case Still the best BSM scenario?!

Case 1: DM – Is it a particle? “Particle concept” has been working so far! [Ellis, 2013]

DM : Lightest neutralino DM could be reconstructed to match astrophysical data!? [ILC TDR 2013]

Case 2: Anomalous (g-2) μ [Benayoun, David, DelBuono, Jegerlehner, 2012] More than 4 σ deviation ⇒ real? SM physics?!

SUSY easily explains the deviation Experimental data indicate not too heavy smuons /sneutrinos not too heavy charginos/neutralinos Precision SUSY spectroscopy at ILC if kinematically accessible

[ILC TDR 2013] (sub)per-cent precision possible at ILC Precision ILC analyses

Case 3: Light Higgs below 125 GeV The discovered 125 GeV Higgs might not be the lightest Higgs in the spectrum! Several light Higgs bosons ⇒ Rich Higgs phenomenology Constraints Direct searches for the lightest Higgs Direct searches for other heavier neutral Higgses Direct searches for the charged Higgses Flavor constraints (e.g. Bs to muon pairs)

LHC ILC Could be a unique opportunity for the ILC!

Crucial to take into account all decay channels Huge reduction of excluded parameter space LCWS 13]

[Heinemeyer]

Case 4: LHC finds only a SM-like Higgs and nothing else ILC + GigaZ Precise Higgs measurement (ILC) Precision observable measurements (GigaZ) Precise top measurement (ILC+GigaZ) Any significant deviations from the SM predictions could be observed at ILC

How to go ahead

A Meaningful Majority Opinion Discovery of a Higgs particle together with W/Z, top, DM, (g-2) μ, … comprises a perfect physics case for the ILC Staged Approaches ILC as a Higgs and top factory Start at lower energies to produce ~0.1 million Higgs bosons Go to higher energies for top physics Go to higher energies for Higgs + top and Higgs self-couplings Go to higher energies for TeV scale exploration or Other options : GigaZ, photon colliders etc

The Higgs discovery marks the dawn of a new era! ILC, fueled by a global program on many fronts, can get us to a new paradigm of fundamental physics!! ILC on the Launch Pad [Lykken]

Back-up Slides

2013 Nobel Prize in Physics

Higgs Self-Coupling

Clear and strong improvement from ILC measurements?? [SFitter 2013]

Higgs Mass and Width

Perfect agreement with the Standard Model

Energy7-14 TeV0.25 – 1 TeV Useful energypartlyall Beamproton (complex)electron (point) Signalhighlow noisevery highlow analysisspecificalmost all eventsnot allall statusrealR&D LHC ⇔ ILC