R. D. McKeown. Jefferson Lab College of William and Mary

Similar documents
Neutrino Masses and Mixing

Neutrinos. Thanks to Ian Blockland and Randy Sobie for these slides. spin particle with no electric charge; weak isospin partners of charged leptons

Low Energy Precision Tests of Supersymmetry

The Standard Model of particle physics and beyond

Particle Physics. Michaelmas Term 2009 Prof Mark Thomson. Handout 11 : Neutrino Oscillations. Neutrino Experiments

P.M. King Ohio University for the MOLLER Collaboration

Is the Neutrino its Own Antiparticle?

TeV-scale type-i+ii seesaw mechanism and its collider signatures at the LHC

Symmetry Tests in Nuclear Physics

Status and prospects of neutrino oscillations

Reminder : scenarios of light new physics

Neutrino Physics: Lecture 1

Recent Discoveries in Neutrino Physics

Intense Slow Muon Physics

Lecture 18 - Beyond the Standard Model

Future Directions in Experimental Nuclear and Particle Physics

PLAN. Lecture I: Lecture II: Neutrino oscillations and the discovery of neutrino masses and mixings. Lecture III: The quest for leptonic CP violation


Matter over antimatter: The Sakharov conditions after 50 years

THE NEUTRINOS. Boris Kayser & Stephen Parke Fermi National Accelerator Laboratory

Neutrino Physics After the Revolution. Boris Kayser PASI 2006 October 26, 2006

Electric dipole moment: theory for experimentalists on the physics of atomic and nuclear EDMs

Weak Interactions. The Theory of GLASHOW, SALAM and WEINBERG

DARK MATTER. Martti Raidal NICPB & University of Helsinki Tvärminne summer school 1

Nuclear Physics Questions, Directions, Applications

Proton Decay and GUTs. Hitoshi Murayama (Berkeley) Durham July 20, 2005

Welcome to the PANIC Pedagogical Lectures! Jesse Thaler Big Questions in Particle Physics

Masaharu Aoki Osaka University

Chart of Elementary Particles

Elementary Particles, Flavour Physics and all that...

Proton Decays. -- motivation, status, and future prospect -- Univ. of Tokyo, Kamioka Observatory Masato Shiozawa

Is the Neutrino its Own Antiparticle?

FYS3510 Subatomic Physics. Exam 2016

To Be or Not To Be: Majorana Neutrinos, Grand Unification, and the Existence of the Universe

The God particle at last? Astronomy Ireland, Oct 8 th, 2012

EXPLORING PARTICLE-ANTIPARTICLE ASYMMETRY IN NEUTRINO OSCILLATION. Atsuko K. Ichikawa, Kyoto University

Neutrino Basics. m 2 [ev 2 ] tan 2 θ. Reference: The Standard Model and Beyond, CRC Press. Paul Langacker (IAS) LSND 90/99% SuperK 90/99% MINOS K2K

Relating the Baryon Asymmetry to WIMP Miracle Dark Matter

ATLAS. Questions and Answers

Neutrinos in Nuclear Physics

New Physics below the Fermi Scale. Mikhail Shaposhnikov

The Jlab 12 GeV Upgrade

Text. References and Figures from: - Basdevant et al., Fundamentals in Nuclear Physics - Henley et al., Subatomic Physics

NEUTRINOS II The Sequel

University College London. Frank Deppisch. University College London

Beyond Standard Model Effects in Flavour Physics: p.1

A first trip to the world of particle physics

NEUTRINO PROPERTIES PROBED BY LEPTON NUMBER VIOLATING PROCESSES AT LOW AND HIGH ENERGIES *

1 Historical Introduction

Neutrino Mass Seesaw, Baryogenesis and LHC

Neutrinos as Probes of new Physics

Neutron Lifetime & CKM Unitarity: The Standard Model & Beyond

Richard Jacobsson. 119 th IEFC, CERN, November 14,

Experimental consequences of (2 nd & 3 rd )-family lepton symmetry in neutrino physics

Analyzing CMS events

Neutrinos as a Unique Probe: cm

Precision Tests of the Standard Model. Yury Kolomensky UC Berkeley Physics in Collision Boston, June 29, 2004

Technicolor Dark Matter. Chris Kouvaris Université Libre de Bruxelles

F. Börkeroth, F. J. de Anda, I. de Medeiros Varzielas, S. F. King. arxiv:

Introduction to Particle Physics. HST July 2016 Luis Alvarez Gaume 1

Results from the Tevatron: Standard Model Measurements and Searches for the Higgs. Ashutosh Kotwal Duke University

Lecture 03. The Standard Model of Particle Physics. Part II The Higgs Boson Properties of the SM

Big Bang Nucleosynthesis

Overview of mass hierarchy, CP violation and leptogenesis.

FYS3510 Subatomic Physics. Exam 2016

What We Know, and What We Would Like To Find Out. Boris Kayser Minnesota October 23,

Introduction to Cosmology

XI. Beyond the Standard Model

Mass (Energy) in the Universe:

Hot Big Bang model: early Universe and history of matter

Testing leptogenesis at the LHC

Overview. The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions.

Lecture 23. November 16, Developing the SM s electroweak theory. Fermion mass generation using a Higgs weak doublet

Computational Applications in Nuclear Astrophysics using JAVA

The God particle at last? Science Week, Nov 15 th, 2012

Neutrinos. Riazuddin National Centre for Physics Quaid-i-Azam University Campus. Islamabad.

Beyond the Standard Model

Results from T2K. Alex Finch Lancaster University ND280 T2K

Flavour physics Lecture 1

e + e - (1) Silicon Vertex Detector

Discovery Physics at the Large Hadron Collider

Neutrinos and Cosmos. Hitoshi Murayama (Berkeley) Texas Conference at Stanford Dec 17, 2004

EDMs and flavor violation in SUSY models

Long & Very Long Baseline Neutrino Oscillation Studies at Intense Proton Sources. Jeff Nelson College of William & Mary

An Introduction to Particle Physics

A model of the basic interactions between elementary particles is defined by the following three ingredients:

Contents. Preface to the First Edition Preface to the Second Edition

Nuclear Physics Questions, Achievements, Goals

Laboratory for Nuclear Science

F. TASNÁDI LINKÖPING UNIVERSITY THEORETICAL PHYSICS NEUTRINO OSCILLATIONS & MASS

On Minimal Models with Light Sterile Neutrinos

MICROPHYSICS AND THE DARK UNIVERSE

Kiwoon Choi (KAIST) 3 rd GCOE Symposium Feb (Tohoku Univ.)

Lecture 8. CPT theorem and CP violation

Electroweak Physics: Lecture V

Parity Violating Electron Scattering at Jefferson Lab. Rakitha S. Beminiwattha Syracuse University

Status and Phenomenology of the Standard Model

Proton Decay Without GUT. Hitoshi Murayama (IAS) UCLA Dec 3, 2003

Experimental Particle Physics at SLAC. John Jaros Stanford Graduate Student Orientation September 17, 2015

FYS 3510 Subatomic physics with applications in astrophysics. Nuclear and Particle Physics: An Introduction

Transcription:

R. D. McKeown Jefferson Lab College of William and Mary Jlab User Meeting, June 2010 1

The Standard Model Renormalizable Gauge Theory Spontaneous Symmetry Breaking n 1 n 2 n 3 Massless g,g Higgs Particle Massive W,Z Fermion masses We have found W, Z, t,b,c,s,d,u,t,m,e,n 1,2,3 Jlab User Meeting, June 2010 2

Quest for the Higgs Particle LEPEWWG Jlab User Meeting, June 2010 3

Standard Model Extremely Successful many accurate predictions But some problems: Higgs not found tension among existing data Not self-consistent Higgs mass Origin of neutrino masses? What is the dark matter? Why not antimatter? Jlab User Meeting, June 2010 4

Unification Q= M/GeV Jlab User Meeting, June 2010 5

The Mass Puzzle Seesaw mechanism n L n R m D m D M n L n R m n m D 2 M m D Jlab User Meeting, June 2010 6 M

h Trouble for the Higgs f h (f = t,b,t,m, ) M h2 = (M h2 ) 0 + kg 2 L 2 /(16p 2 ) M h M GUT M Planck (and G F 0) New Physics at TeV scale stabilize M h Is it the dark matter? Jlab User Meeting, June 2010 7

Mass Scales Terascale ~ 1 TeV Unification ~ 10 13 TeV Planck ~ 10 15 TeV Symmetries Neutrinos LHC 1E-05 0.01 10 10000 10000000 1E+10 1E+13 1E+16 1E+19 M (TeV) Jlab User Meeting, June 2010 8

Flow Chart Higgs Mechanism Correct? Yes Terascale Physics No n, symmetries Yes No n, symmetries LHC Discoveries, n, symmetries Need n, symmetries independent of LHC results! Jlab User Meeting, June 2010 9

Low energy studies in the LHC era (and beyond!) Two frontiers in the search for new physics Collider experiments (pp, e + e -, etc) at higher energies (E >> M Z ) Indirect searches at lower energies (E < M Z ) but high precision Large Hadron Collider Ultra cold neutrons, High energy physics CERN Particle, nuclear & atomic physics Jlab User Meeting, June 2010 10

Matter Antimatter Asymmetry (The universe contains matter, not antimatter) Sakharov Criteria: Baryon number violation (or L B) (no evidence yet) CP violation (SM not enough) Non-equilibrium (universe expands, OK, need phase transition?) Experimental info: N-decay, EDM s, n mixing Jlab User Meeting, June 2010 11

Mass - origin of SM masses - mass/energy scales Matter asymmetry - CP violation - B,L violation Summary Attractive Framework: SUSY GUT contains all ingredients needed to address these issues: Light Higgs, CP, B, L, M GUT Is it correct?? Symmetries Neutrinos LHC 1E-05 0.01 10 10000 10000000 1E+10 1E+13 1E+16 1E+19 M (TeV) Jlab User Meeting, June 2010 12

Recent Neutrino History Persistent observations of deficit of solar neutrinos 1998 observation of oscillations of atmospheric neutrinos by Super-K 2002 SNO results imply matter-dependent oscillations of solar neutrinos KamLAND observes oscillations of reactor (man-made) anti-neutrinos Jlab User Meeting, June 2010 13

Neutrinos Oscillate! First laboratory evidence for physics beyond the standard model!! Jlab User Meeting, June 2010 14

Neutrinos: The Best is Yet to Come? Absolute mass scale q 13 the last mixing angle Mass hierarchy CP violation Antineutrino=neutrino (Majorana)? Jlab User Meeting, June 2010 15

Neutrino Mass Scale sensitivity: m n < 0.2eV (90%CL) ~ 75 m long with 40 s.c. solenoids Jlab User Meeting, June 2010 16

bb Decay Jlab User Meeting, June 2010 17

Neutrinoless bb Decay Whatever processes cause 0nbb, its observation would imply the existence of a Majorana mass term and thus would represent New Physics: Schechter and Valle,82 (n) R e e 0nbb n L W u d d u W By adding only Standard model interactions we obtain ( n) R (n) L Majorana mass term Observing the 0nbb decay implies that n are massive Majorana particles. Jlab User Meeting, June 2010 18

bb Decay Experiments 10 ton 10 mev CUORE EXO Majorana GERDA Jlab User Meeting, June 2010 19

Maki Nakagawa Sakata Matrix Gateway to CP Violation! CP violation Jlab User Meeting, June 2010 20

n e Survival Probability Dominant q 12 Oscillation Subdominant q 13 Oscillation Clean measurements of q, Dm 2 No CP violation, negligible matter effects Jlab User Meeting, June 2010 21

Daya Bay Reactor Neutrino Experiment 4 reactor cores, 11.6 GW 2 more cores in 2011, 5.8 GW Mountains provide overburden to shield cosmic-ray backgrounds Baseline ~2km Multiple detectors measure ratio of far/near sites Jlab User Meeting, June 2010 22

Experiment Construction Assembly Building Jlab User Meeting, June 2010 23

q 13 the last mixing angle Spring 2011: Near site turn-on Spring 2012: Far site turn-on Jlab User Meeting, June 2010 24

n e Appearance DUSEL Mass hierarchy (+/-) FNAL CP violation matter Jlab User Meeting, June 2010 25

Mass Hierarchy and CP Violation Jlab User Meeting, June 2010 http://nwg.phy.bnl.gov/~diwan/nwg/fnal-bnl/ 26

Supernova Large Underground Detector Long Baseline Neutrino Oscillations Nucleon decay (B violation, Mass scale< M GUT?) Supernova neutrino detection (q 13, r-process?) Jlab User Meeting, June 2010 27

CKM Unitarity Jlab User Meeting, June 2010 28

Lifetime and Correlations combine in a (presently) confused picture for the physics of g A or unitarity X X J. Nico, 2007 A = 0.1196(5) [PERKEO II 2007] Jlab User Meeting, June 2010 29

Neutron Decay Measurements Correlation measurements Lifetime measurements Jlab User Meeting, June 2010 30

Electric Dipole Moment (EDM) Existence of EDM implies violation of Time Reversal Invariance + - J t t J J + - d T violation CP violation SUSY, Terascale Matter Antimatter asymmetry d - J Jlab User Meeting, June 2010 31

nedm Limits e-cm nedm search Complementary Electron Atoms Nuclei, Deuteron (ring) LHC Jlab User Meeting, June 2010 32

New nedm Experiment Superfluid He UCN converter with high E-field 3 He co-magnetometer Jlab User Meeting, June 2010 33

Parity-violating electron scattering SLAC Moller? JLab Future Scale-dependence of Weak Mixing Jlab User Meeting, June 2010 34

Jlab User Meeting, June 2010 35

meter s first toroid hybrid toroid meters PV Moller Scattering: Custom Toroidal Spectrometer 5kw LH Target SOLID (PVDIS): High Luminosity on LD2 and LH2 Better than 1% errors for small bins Large Q 2 coverage x-range 0.25-0.75 W 2 > 4 GeV 2 36 Jlab User Meeting, June 2010

Kurylov, et al. Jlab User Meeting, June 2010 37

Muon g-2 e Momentum Spin 3.4 s 3.4 s SUSY? Jlab User Meeting, June 2010 38

m m e Conversion ( A, Z) e ( A, Z) Courtesy: A. de Gouvea??? MEGA Sindrum II Jlab User Meeting, June 2010 39 39

Neutrinos have provided dramatic discoveries, with more to come! Fundamental symmetries complement LHC - additional information - can often extend reach beyond LHC Both relevant to other questions -origin of matter -SM masses -nucleosynthesis Many new high-sensitivity experiments Jlab User Meeting, June 2010 40

Many Thanks M. Ramsey-Musolf K. Kumar S. Page H. Robertson B. Filippone P. Vogel A. de Gouvea D. Hertzog R. Holt many others Jlab User Meeting, June 2010 41