Physics at the High Energy Frontier J. Hewett PANIC 2005.

Slides:



Advertisements
Similar presentations
Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
Advertisements

Fermilab E = Mc 2 Opening Windows on the World Young-Kee Kim Fermilab and the University of Chicago June 1, 2010.
STRING THEORY: CHALLENGES AND PROSPECTS John H. Schwarz October 2008.
Beyond the SM: SUSY and ToE A romantic dream for an unified description of the universe? Part III.
Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
The Importance of ILC Communications Barry Barish Communications Workshop VLCW06 17-July-06.
Future Directions in Experimental Nuclear and Particle Physics Barry Barish Bacher Symposium Caltech 5-Nov-05 Bacher at the Caltech Synchrotron Robert.
AAAS 2001 San Francisco1 Supersymmetry The Coming Revolutions in Particle Physics Hitoshi Murayama (UC Berkeley)
Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u.
Looking for SUSY Dark Matter with ATLAS The Story of a Lonely Lepton Nadia Davidson Supervisor: Elisabetta Barberio.
1 Discovering New Physics with the LHC Nadia Davidson Supervisor: Elisabetta Barberio EPP Nobel Prize for Physics in 2010:
Physics with ATLAS and CMS Are there new symmetries or extra-dimensions? What is dark matter? Where does mass come from? The two big multi-purpose experiments.
Physics with 500 GeV LC Hitoshi Murayama (UC Berkeley) LC Retreat Santa Cruz, June 27, 2002.
JoAnne Hewett, SLAC Scientific Opportunities at a Linear Collider: Making the Case.
Dean Karlen University of Victoria & TRIUMF APS NW Section Meeting 2005 Victoria, Canada.
2-Oct-06University of Bologna1 The Future of Particle Physics The Case for Building another Huge Particle Accelerator Barry Barish CALTECH 2-Oct-06.
Big Questions, L(H)C Answers Jonathan Feng UC Irvine LC/LHC Workshop, Fermilab 13 December 2002.
The International Linear Collider Barry Barish iThemba Cape Town 21-Oct-05.
Paris 22/4 UED Albert De Roeck (CERN) 1 Identifying Universal Extra Dimensions at CLIC  Minimal UED model  CLIC experimentation  UED signals & Measurements.
The International Linear Collider Barry Barish IUPAP General Assembly Cape Town 26-Oct-05.
Searches for New Physics Motivations Examples Searches so far Setting scene for LHC 1/12.
1 New Frontiers in Particle Physics Jeff Forshaw University of Manchester.
Higgs, Less Higgs, Higgsless or more Higgs? ITEP Winter School Otradoe, February 2012 John Ellis, King’s College London & CERN.
CERN, 21 February 2001 Egil Lillestøl, CERN & Univ. of Bergen Recorded at
My Chapter 30 Lecture.
Joseph Haley Joseph Haley Overview Review of the Standard Model and the Higgs boson Creating Higgs bosons The discovery of a “Higgs-like” particle.
The Dark Side of the Universe What is dark matter? Who cares?
Point 1 activities and perspectives Marzio Nessi ATLAS plenary 2 nd October 2004 Large Hadron Collider (LHC)
August 22, 2002UCI Quarknet The Higgs Particle Sarah D. Johnson University of La Verne August 22, 2002.
Lepton-Photon 2007 Summary and Outlook Young-Kee Kim The University of Chicago and Fermilab August 18, 2007 Daegu, Korea.
International Conference on Linear Colliders Paris, April 19-23, 2004 Theoretical Introduction John Ellis.
Quarks, Leptons, Bosons, the LHC and all that. Tony Liss OLLI Lecture September 23, 2008.
Physics Priorities S. Dawson July 11, 2007 Fermilab Steering Committee Meeting.
Masato Yamanaka (Saitama University) collaborators Shigeki Matsumoto Joe Sato Masato Senami arXiv: [hep-ph]Phys.Lett.B647: and Relic abundance.
Future Colliders: Opening Windows on the World Young-Kee Kim The University of Chicago ICFA Seminar September 28 - October 1, 2005 Kyungpook National University,
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 30: Particle Physics Fundamental.
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.
1 Supersymmetry Yasuhiro Okada (KEK) January 14, 2005, at KEK.
Low scale supergravity mediation in brane world scenario and hidden sector phenomenology Phys.Rev.D74:055005,2006 ( arXiv: hep-ph/ ) ACFA07 in Beijing:
Review of the Open Questions and the Potential for Discoveries ICFA Seminar Taegu, September 2005 John Ellis, TH Division, PH Department, CERN.
Compelling Scientific Questions The International Linear Collider will answer key questions about matter, energy, space and time We sample some of these.
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.
Phy107 Fall Final Exam Thursday, Dec. 21: 2:45 - 4:45 pm 113 Psychology Building Note sheet: one double-sided page Cumulative exam-covers all material,
22 December 2006Masters Defense Texas A&M University1 Adam Aurisano In Collaboration with Richard Arnowitt, Bhaskar Dutta, Teruki Kamon, Nikolay Kolev*,
Introduction to CERN Activities
The Higgs Boson Observation (probably) Not just another fundamental particle… July 27, 2012Purdue QuarkNet Summer Workshop1 Matthew Jones Purdue University.
Searching for New Matter with the D0 Experiment Todd Adams Department of Physics Florida State University September 19, 2004.
Sep/19/2008 Su Dong Stanford Student Orientation: Accelerator based Particle Physics1 Accelerator Based Particle Physics Su Dong Stanford Student Orientation.
Compelling Scientific Questions The International Linear Collider will answer key questions about matter, energy, space and time We now sample some of.
The Search For Supersymmetry Liam Malone and Matthew French.
The Standard Model of the elementary particles and their interactions
Main Issues in ADD phenomenology Find out of there are signals for Kaluza-Klein towers of gravitons ─ large-p T excess, missing energy, etc. Determine.
Particle Detectors January 18, 2011 Kevin Stenson.
STAU CLIC Ilkay Turk Cakir Turkish Atomic Energy Authority with co-authors O. Cakir, J. Ellis, Z. Kirca with the contributions from A. De Roeck,
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,
Collider Signals of Extra Dimension Scenarios
Global Analysis, Combination & Complementarity The vision: explore 10 TeV scale directly (100 TeV pp) + indirectly (e + e - )
Standard Model of Particle Physics
Physics Overview Yasuhiro Okada (KEK)
Elementary particles Spring 2005, Physics /24/2018 Lecture XXV.
Higgs and SUSY at future colliders
Search For New Physics Chary U of S.
Physics at a Linear Collider
Physics Overview Yasuhiro Okada (KEK)
Yasuhiro Okada (KEK) April 17, 2003, CAT, Indore, India
The Mysteries of Particle Physics and how we are trying to solve them
Physics Overview Yasuhiro Okada (KEK)
What do we hope to understand?
Can new Higgs boson be Dark Matter Candidate in the Economical Model
Presentation transcript:

Physics at the High Energy Frontier J. Hewett PANIC 2005

What is the world made of? What holds the world together? Where did we come from? Primitive Thinker Courtesy: Y.K. Kim

Evolved Thinker From “Quantum Universe” Courtesy: Y.K. Kim 1.Are there undiscovered principles of nature: New symmetries, new physical laws? 2. How can we solve the mystery of dark energy? 3. Are there extra dimensions of space? 4. Do all the forces become one? 5. Why are there so many kinds of particles? 6. What is dark matter? How can we make it in the laboratory? 7. What are neutrinos telling us? 8. How did the universe come to be? 9. What happened to the antimatter?

LHC: ILC: Collider Tools which Answer these Questions: proton e-e- e+e+ Broad energy reach Large event rate Knowledge of initial quantum state Well-defined initial energy and angular momentum (polarization) Clean environment Can vary CoM

The LHC is Becoming a Reality! The excitement is building - we are counting down the days….

Major Discoveries are Expected! - A. De Roeck, Snowmass 2005

Much Progress on the ILC in the Last Year: Superconducting rf Technology chosen Global Design Effort Launched! Barry Barrish is Director of the GDE + 3 Regional Directors + 45 Team Members and counting… Baseline Configuration being Defined now…

Barrish, Snowmass 05

Particles Tell Stories: Discovery of a new particle is the opening chapter of a story. These particles are merely the messengers which reveal a profound story about the nature of matter, energy, space, and time. Learning the full story involves: 1) Discovery of a new particle 2) Discovery of the theory behind the new particle It is up to us to find the new particles and to listen to their stories

Particles Tell Stories: Discovery of a new particle is the opening chapter of a story. These particles are merely the messengers which reveal a profound story about the nature of matter, energy, space, and time. Learning the full story involves: 1) Discovery of a new particle 2) Discovery of the theory behind the new particle Measurements at the ILC, together with results from the LHC, will identify the full nature of the physics at the TeV scale and reveal its full story It is up to us to find the new particles and to listen to their stories

HEPAP LHC/ILC Subpanel Report(s): 43 page semi-technical version, submitted to EPP2010 panel in late July /LHC-ILC-Subpanel-EPP2010.pdf 35 page non-technical version, in press. The report emphasizes: the synergy between the LHC and ILC differences in how measurements are made at ILC and LHC unique physics to ILC

The Authors:

The report centers on 3 physics themes : 1. Mysteries of the Terascale : Solving the mysteries of matter at the Terascale 2. Light on Dark Matter : Determining what Dark Matter particles can be produced in the laboratory and discovering their identity 3. Einstein’s Telescope : Connecting the laws of the large to the laws of the small Now for some highlights of physics unique to the ILC

Higgs at the Terascale An important Higgs production process is e + e -  Z + Higgs There are many possible final states, depending on how the Z and Higgs decay In e+e-  Z + Anything ‘Anything’ corresponds to a system recoiling against the Z The mass of this system is determined solely by kinematics and conservation of energy because we see everything else, we know what is escaping Recoil Technique : Peak in Recoil Mass corresponds to 120 GeV Higgs!

ILC Simulation for e + e -  Z + Higgs with Z  2 b-quarks and Higgs  invisible N. Graf

Provides accurate, direct, and Model Independent measurements of the Higgs couplings Recoil technique gives precise determination of Higgs properties Independent of its decay mode The strength of the Higgs couplings to fermions and bosons is given by the mass of the particle Within the Standard Model this is a direct proportionality This is a crucial test of whether a particle’s mass is generated by the Higgs boson! Higgs f f - ~ m f

Size of measurement errors ILC will have unique ability to make model independent tests of Higgs couplings at the percent level of accuracy. m h = 120 GeV

Possible deviations in models with Extra Dimensions This is the right sensitivity to discover extra dimensions, new sources of CP violation, or other novel phenomena Mass (GeV) m h = 120 GeV Coupling strength to Higgs boson Higgs is Different! First fundamental scalar to be discovered: could be related to many things, even dark energy

ILC Studies superpartners individually via e + e -  SS Determines Quantum numbers (spin!) Supersymmetric relation of couplings  = e  ~ ~ = 2e - Proof that it IS Supersymmetry! Supersymmetry at the Terascale M 1 (GeV) Ratio of Coupling Stregths Selectron pair production 2% accuracy in determination of Supersymmetric coupling strength

Precise Mass Measurements of Superpartners Example: e  e +  Fixed center of mass energy gives flat energy distribution in the laboratory for final state e - Endpoints can be used to determine superpartner masses to part-per-mil accuracy ~~ e A realistic simulation: Determines Superpartner masses of the electron and photon to 0.05%!

A complicated Table with lots of details that illustrates how ILC results improve upon Superpartner mass measurements at the LHC Shows accuracy of mass determinations at LHC and ILC alone and combined

Accurate superpartner mass determinations necessary for unification tests Evolution of superpartner masses to high scale: Force unificationMatter Unification Einstein’s Telescope to Unification

Kaluza-Klein modes in a detector Number of Events in e + e -   +  - For a conventional braneworld model with a single curved extra dimension of size ~ cm For this same model embedded in a string theory Standard Model Z- boson 1 st KK mode 2 nd KK mode 3 rd KK mode Extra Dimensions at the Terascale

Detailed measurements of the properties of KK modes can determine: That we really have discovered additional spatial dimensions Size of the extra dimensions Number of extra dimensions Shape of the extra dimensions Which particles feel the extra dimensions If the branes in the Braneworld have fixed tension Underlying geometry of the extra dimensional space

Example: Production of Graviton Kaluza-Klein modes in flat extra dimensions, probes gravity at distances of ~ cm Production rate for e + e -   + Graviton with 7 Extra Dimensions Size of Measurement error Measurement possible due to well-defined initial state & energy plus clean environment

Where particles live in extra dimensions Polarized Bhabha Scattering Determines location of left- and right- handed electron in extra dimension of size 4 TeV -1 Location of e L in an extra dimension Location of e R in an extra dimension

Telescope to Very High Energy Scales ‘X’ Many tools to detect existence of heavy object ‘X’: Deviations in production rates Deviations in production properties such as distribution of angle from beam-line Deviations in distributions of angular momentum For all types of final state fermions! ILC can probe presence of Heavy Objects with Mass > Center of Mass Energy in e + e  ff  Indirect search for New Physics -

Various Unification Models For ILC Sensitivity : Solid = 5  = standard discovery criteria Dashed = 2  95% (=2  ) direct discovery at LHC Example: New Heavy Z-like Boson from Unification Theories Collider Sensitivity Mass of Z-like Boson (TeV) ILC can probe masses many times the machine energy!

95% contours for Z’ couplings to leptons at ILC LHC determines mass ILC determines interactions Number of Events in pp   +  - Mass of muon pair (TeV)Axial Coupling Vector Coupling Kaluza- Klein Z’ SO(10): origin of mass E 6 : unified Higgs Drell-Yan distribution at LHC

Light on Dark Matter Dark Matter comprises 23% of the universe No reason to think Dark Matter should be simpler than the visible universe  likely to have many different components Dream: Identify one or components and study it in the laboratory

A component of Dark Matter could be the Lightest Neutralino of Supersymmetry - stable and neutral with mass ~ 0.1 – 1 TeV In this case, electroweak strength annihilation gives relic density of m 2 Ω CDM h 2 ~ (1 TeV) 2 One Possibility: Dark Matter in Supersymmetry

Comparative precision of ILC measurements (within SUSY) ILC and Astro measurements ILC and direct detection

The more discoveries that are made at the LHC, the greater the discovery potential at the ILC

When the LHC makes its discoveries, let’s be ready to start construction on the ILC!