Compelling Questions of High Energy Physics? What does the future hold? Persis S. Drell Physics Department Cornell University.

Slides:



Advertisements
Similar presentations
LRP2010 WG5 Fundamental Interactions Nathal Severijns ( K.U.Leuven) for WG5 Scoping workshop Frankfurt, October th 2009.
Advertisements

Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
Kiwoon Choi PQ-invariant multi-singlet NMSSM
Can we experimentally test seesaw and leptogenesis? Hitoshi Murayama (IPMU Tokyo & Berkeley) Melbourne Neutrino WS, Jun 4, 2008 With Matt Buckley.
Outlook: Higgs, SUSY, flavor Ken-ichi Hikasa (Tohoku U.) Fourth Workshop, Origin of Mass and SUSY March 8, 2006, Epochal Tsukuba.
Chiral freedom and the scale of weak interactions.
The classically conformal B-L extended standard model Yuta Orikasa Satoshi Iso(KEK,SOKENDAI) Nobuchika Okada(University of Alabama) Phys.Lett.B676(2009)81.
Higgs Boson Mass In Gauge-Mediated Supersymmetry Breaking Abdelhamid Albaid In collaboration with Prof. K. S. Babu Spring 2012 Physics Seminar Wichita.
Discrete Space-Time Symmetries Xiao-Gang He USTC, Nanakai, and NTU 1. Discrete Space-Time Symmetries 2. The Down Fall of Parity P Symmetry 3. The Down.
1 FK7003 Lecture 8 ● CP -violation ● T -violation ● CPT invariance.
WHAT’S IN AN ATOM?. MATTER Atom ~ mNucleus ~ mQuarks
1 NEUTRINO SEESAW AND CP VIOLATION FROM DYNAMICAL ELECTROWEAK SYMMETRY BREAKING 1.Introduction 2.UV Complete Model(s) 3.Seesaw 4.CP Violation R.Shrock.
The Asymmetry between Matter and Antimatter Besma M’charek FEW, Vrije Universiteit Amsterdam.
Neutrino Physics - Lecture 1 Steve Elliott LANL Staff Member UNM Adjunct Professor ,
Chiral freedom and the scale of weak interactions.
P461 - particles VII1 Glashow-Weinberg-Salam Model EM and weak forces mix…or just EW force. Before mixing Bosons are massless: Group Boson Coupling Quantum.
Richard Howl The Minimal Exceptional Supersymmetric Standard Model University of Southampton UK BSM 2007.
The Top Quark and Precision Measurements S. Dawson BNL April, 2005 M.-C. Chen, S. Dawson, and T. Krupovnikas, in preparation M.-C. Chen and S. Dawson,
Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u.
4 th Generation Leptons in Minimal Walking Technicolor Theory Matti Heikinheimo University of Jyväskylä.
1 Discovering New Physics with the LHC Nadia Davidson Supervisor: Elisabetta Barberio EPP Nobel Prize for Physics in 2010:
Smashing the Standard Model: Physics at the CERN LHC
Chiral freedom and the scale of weak interactions.
Schlüsselexperimente der Elementarteilchenphysik:.
Chiral freedom and the scale of weak interactions.
.. Particle Physics at a Crossroads Meenakshi Narain Brown University.
Aug 29-31, 2005M. Jezabek1 Generation of Quark and Lepton Masses in the Standard Model International WE Heraeus Summer School on Flavour Physics and CP.
Particle Physics From Strings To Stars. Introduction  What is Particle Physics?  Large Hadron Collider (LHC)  Current Experiments – ALICE – ATLAS –
A New Theory of Neutrino Oscillations Netta Engelhardt
1 New Frontiers in Particle Physics Jeff Forshaw University of Manchester.
 Collaboration with Prof. Sin Kyu Kang and Prof. We-Fu Chang arXiv: [hep-ph] submitted to JHEP.
Particle Physics at the Energy Frontier Tevatron → LHC & The Very Early Universe Tony LissAir Force Institute of TechnologyApril 10, 2008.
Fermion Masses and Unification Steve King University of Southampton.
Minimal SO(10)×A4 SUSY GUT ABDELHAMID ALBAID In Collaboration with K. S. BABU Oklahoma State University.
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.
LHC and Search for Higgs Boson Farhang Amiri Physics Department Weber State University Farhang Amiri Physics Department Weber State University.
Wednesday, Apr. 23, 2003PHYS 5326, Spring 2003 Jae Yu 1 PHYS 5326 – Lecture #24 Wednesday, Apr. 23, 2003 Dr. Jae Yu Issues with SM picture Introduction.
Physics Priorities S. Dawson July 11, 2007 Fermilab Steering Committee Meeting.
1 Supersymmetry Yasuhiro Okada (KEK) January 14, 2005, at KEK.
INVASIONS IN PARTICLE PHYSICS Compton Lectures Autumn 2001 Lecture 8 Dec
WHAT BREAKS ELECTROWEAK SYMMETRY ?. We shall find the answer in experiments at the LHC? Most likely it will tells us a lot about the physics beyond the.
Introduction to Particle Physics How to compute the Universe?
1 Highlights from Belle Jolanta Brodzicka (NO1, Department of Leptonic Interactions) SAB 2009.
Universality of weak interactions?
QFD, Weak Interactions Some Weak Interaction basics
Introduction to CERN Activities
Neutrino mass and DM direct detection Daijiro Suematsu (Kanazawa Univ.) Erice Sept., 2013 Based on the collaboration with S.Kashiwase PRD86 (2012)
Impact of Neutrino Oscillation Measurements on Theory Hitoshi Murayama NuFact 03 June 10, 2003.
The Higgs Boson Observation (probably) Not just another fundamental particle… July 27, 2012Purdue QuarkNet Summer Workshop1 Matthew Jones Purdue University.
Yingchuan Li Electroweak physics at EIC Brookhaven National Lab Feb. 3rd 2011, BNL.
Searching for New Matter with the D0 Experiment Todd Adams Department of Physics Florida State University September 19, 2004.
H. Quarks – “the building blocks of the Universe” The number of quarks increased with discoveries of new particles and have reached 6 For unknown reasons.
Sally Dawson, BNL Standard Model and Higgs Physics FNAL LHC School, 2006 Introduction to the Standard Model  Review of the SU(2) x U(1) Electroweak theory.
The Standard Model of the elementary particles and their interactions
The Importance of the TeV Scale Sally Dawson Lecture 3 FNAL LHC Workshop, 2006.
Physics 222 UCSD/225b UCSB Lecture 12 Chapter 15: The Standard Model of EWK Interactions A large part of today’s lecture is review of what we have already.
THE CONNECTION BETWEEN NEUTRINO EXPERIMENTS AND LEPTOGENESIS Alicia Broncano Berrocal MPI.
1-2 Mass Degeneration in the Leptonic Sector Hiroyuki ISHIDA (Tohoku University) Collaboration with : Takeshi ARAKI (MISC) Ref ; T. Araki and H.I. arXiv.
Pontecorvo’s idea An introductory course on neutrino physics (IV)
Classically conformal B-L extended Standard Model
Compelling Questions of High Energy Physics?
Elementary particles Spring 2005, Physics /24/2018 Lecture XXV.
Beyond the standard model
Beyond the Higgs wan ahmad tajuddin wan abdullah
Flavour and Non-universal Gauge Interaction
Methods of Experimental Particle Physics
Neutrino Oscillations
Introduction to Particle Physics
LHC: Seeking the Origin of Symmetry Breaking and Mass
Presentation transcript:

Compelling Questions of High Energy Physics? What does the future hold? Persis S. Drell Physics Department Cornell University

Physics: “The knife that cuts into the grain of nature” -Jacob Bronowski “The rules of the game are what we mean by fundamental physics…” - Richard Feynman

Fundamental Questions of Particle Physics What are the fundamental constituents of matter? How many are there? Can we understand why they have the masses that they do? What are the fundamental forces? Can we understand why some are weak and some are strong? Can they be unified? What is the structure of spacetime? How did the Universe evolve in the first seconds after the big bang?

??

Building Blocks Forces and Force Carriers

The decay of the muon via the weak interactions   e e   W-W-

Ingredients of the Standard Model Local Gauge Invariance –Symmetries Generate Interactions Spontaneous Symmetry Breaking –Gives mass to force carriers –Predicts a Higgs Non-Abelian –The force carriers can have charge Add in the matter fields of the quarks and leptons, lots of extra parameters, bake at 350 for 30 minutes –Correctly predict the results of every high energy physics experiment for the last 30 years.

Top Features of the Standard Model Every experiment for last 30 years has either agreed with the model or the experiment is wrong. Unification of 3 of 4 forces Explains HEP to the TeV scale ( m) Predicted the existence and mass of the Z boson Makes flavor mixing in the quark sector understandable to a 1st year physics grad –CKM Leaves us with lots of unanswered questions! Weak EM Strong Gravity V ud V us V ub V cd V c s V cb V td V ts V tb d s b d s b = strong weak

Quark Flavor Mixing Eigenstates of the strong interactions (states of quark flavor u,d,s,c,b,t) are not eigenstates of the weak interactions –Flavor a symmetry of the SI –Flavor not a symmetry of the WI Weak Interaction diagonal on a different basis WI basis and SI basis related by rotation matrix (CKM) Phenomenology of flavor mixing V ud V us V ub V cd V c s V cb V td V ts V tb d s b d s b = strong weak

Worst “bugs” in the Standard Model Too many free parameters Different bases for strong and weak interactions Where do the masses come from? Parity violation of the weak interactions added by hand Fundamental Scalar (spin 0) Higgs Fine tuning problems Only works to 1TeV Doesn’t include gravity Leaves us with lots of unanswered questions

Compelling Questions for the Next Decade -Going beyond the SM- What is the right description of gravity? Can all the forces be unified? What is the origin of mass? What is the new physics beyond the SM? Can we understand flavor mixing and where does CP violation come from? Can we explain the Universe?

Current Probes of SM -The high energy frontier- LEP: M H > 100GeV – Possible signal at M H = 114GeV ?? FNAL: May discover Higgs if light enough LHC: Will discover the Higgs!

-High Density Frontier- (Nucleon+Nucleon) BNL

-High Precision Frontier- Rare K and B decays Masses and mixing of –Flavor oscillations

-Precision Frontier- Neutrino Oscillations Lepton Flavor Mixing –No neutrino mass => no lepton flavor mixing –Finite neutrino mass => expect lepton flavor mixing just like we have quark flavor mixing Simplest solution: leptons mix just like quarks Problem with simplest solution: very unnatural. –Once allow neutrino to have mass: Dirac mass like quarks Majorana mass (unique to particles without electric charge) Rule of QFT: be as generic as possible = e   e   Lepton Mixing Matrix weak mass

-Precision Frontier- CP Violation What happened to the anti-matter? –Studies of CP Violation in K and B decays –Studies of rare processes that are highly suppressed in the SM so new physics has a chance to compete favorably. Big Bang Matter=Antimatter Now Matter only

Warning: focus on the problem at hand, but still be a student of problems in other fields Be Broad

Be Critical Warning: Always temper your criticism with judgement

Three of these plots show statistical fluctuations. One shows a real signal. Can you pick out the real signal?

Be Bold ‘Truth emerges more readily from error than from confusion’ - Francis Bacon

Be Optimistic!