Superluminal Neutrinos? Constraints and Constructions. John Ellis King s College London (& CERN)

Size: px
Start display at page:

Download "Superluminal Neutrinos? Constraints and Constructions. John Ellis King s College London (& CERN)"

Transcription

1 Versus and Superluminal Neutrinos? Constraints and Constructions John Ellis King s College London (& CERN)

2 Versus and Do neutrinos really travel faster than light? Do photons travel at the speed of light? Photon v c: 1997 Neutrino v c: 1999 Astrophysical constraints on photon v: 2005/7 SN and accelerator constraints on neutrino v: 2008 Interpretation of OPERA: 2011

3 History in the Making? 1862: Maxwell found that there should be electromagnetic waves travelling at approximately the (known) speed of light 1905: Einstein used universal speed of light as foundation of geometric description of physics 2011: OPERA finds 6-σ discrepancy between neutrino speed and that of light Life in the fast lane

4 MINOS Measurement of ν Speed Near & far detectors Uncertainties Published result almost 2 σ > 0

5

6 SN 1987a Constraints Revisited JE, Harries, Mersegaglia, Rubbia & Sakharov: arxiv:

7 Constraints from Supernova 1987a Data from 3 experiments Supernova simulation Arrived hours before γ s!!! δv < 10-9 JE, Harries, Mersegaglia, Rubbia & Sakharov: arxiv: Possible E dependence of δv constrained by bunching

8 Constraints from SN1987a Fit to possible E-dependent time-lag Linear: Quadratic: Subluminal and superluminal cases JE, Harries, Mersegaglia, Rubbia & Sakharov: arxiv:

9 OPERA could improve on MINOS JE, Harries, Mersegaglia, Rubbia & Sakharov: arxiv:

10 Structure of CNGS Beam Energy Spectrum Time structure JE, Harries, Mersegaglia, Rubbia & Sakharov: arxiv:

11 Possible Distortion of Spill 100 ns resolution, linear delay by 5 ns/gev, corresponding to M νqg1 = GeV JE, Harries, Mersegaglia, Rubbia & Sakharov: arxiv:

12 Arrival Times for Different Energies 1000-event slices Higher energies later JE, Harries, Mersegaglia, Rubbia & Sakharov: arxiv:

13 Fits to Simulated OPERA Data Linear case Quadratic case Sensitivity Sensitivity JE, Harries, Mersegaglia, Rubbia & Sakharov: arxiv:

14 Fitting Edges of Spill Factor ~ 5 less sensitivity to energy dependence JE, Harries, Mersegaglia, Rubbia & Sakharov: arxiv:

15 Using 5ns Bunch Structure 5 ns spacing, 1 ns bunches Fit to quadratic case Including rock events Sensitivity Sensitivity JE, Harries, Mersegaglia, Rubbia & Sakharov: arxiv:

16

17 The Main Result

18

19 Special and General Relativity Sagnac effect (rotation of Earth during travel): : δt = ns Tends to increase travel time Smaller than total error, taken into account Schwartzschild effects ~ Neutrinos follow geodesic, re-evaluate Euclidean distance Non-inertial effects, redshifts of clocks, dipole field, frame-dragging all negligible Kiritsis & Nitti: OPERA public note 136

20 Comparison of Neutrino Constraints Cacciapaglia, Deandrea & Panizzi: arxiv: Giudice, Sibiryakov & Strumia: arxiv: Alexandre, JE & Mavromatos: arxiv: SN1987a excludes δv ~ E or E 2

21 Power-Law Fit to Neutrino Data Need δv ~ E n with n > 2.5 Giudice, Sibiryakov & Strumia: arxiv:

22 Could Neutrinos be Tachyons? v would approach c from above as E increases No non-trivial finite-dimensional unitary representations of Lorentz group for m 2 < 0 i.e., no spin-1/2 spinors Should spin 0 be quantized as bosons? No (Feinberg) vs Yes (Sudarshan) Problem of causality! Reinterpret backward emission of E < 0 as forward emission of E > 0? Deform/break Lorentz symmetry?

23 Lifshitz-Type Field Theory Time and space dimensions scale differently (Interesting for quantum gravity, mass generation) Anisotropy parameter z Model for neutrino velocity: Action: Dispersion relation: Group velocity: v g = > c Superluminal propagation: δv ~ E 2 J. Alexandre: arxiv: Alexandre, JE & Mavromatos: arxiv:

24 Lorentz-Violating Gauge Theory Background vector or axial U(1) gauge field: Dispersion relation: Group velocity: Subluminal propagation (so far ) Alexandre, JE & Mavromatos: arxiv:

25 Background Gauge Field Allow background gauge field: Disersion relations: (ν anti-ν) Subluminal group v: Include anisotropic background: Group velocity may be super- or subluminal: Dependent on direction! Alexandre, JE & Mavromatos: arxiv:

26 Suggests Exotic Possibilities Neutrino speed antineutrino speed? Speed depends on direction? Possibility of diurnal variation as Earth rotates If no diurnal variation, V aligned with Earth s rotation axis In this case: Neutrino going North (MINOS) subluminal Null effect for neutrinos travelling East-West (T2K) Alexandre, JE & Mavromatos: arxiv:

27 Condensed-Matter Analogues? Systems known with relativistic fermionic excitations: p ~ E: Superfluids & superconductors Graphene Motivation for our early work Can study versions with superluminality e.g., PT-symmetry breaking in honeycomb photonic lattice Homework for particle physicists? Kupnin & Volovik: cond-mat/ JE, Mavromatos, Nanopoulos & Volkov: 1999 Szameit, Rechtsman, Bahat-Treidel & Segev: arxiv:

28 Čerenkov Radiation by Neutrinos Possible if speed > light dominant process e + e - Bremsstrahlung Energy loss rate: Difference between initial/final energies, terminal energy E T : Sensitive to δ = 2 δv and its E dependence Applied to IceCube data suggests Does not apply to models with distorted metrics, nonlinear deformations of Lorentz symmetry Cohen & Glashow: arxiv:

29 Distortion of Energy Spectrum? Events seen up to very high energies >> <E ν > = 28.1 GeV No apparent distortion of kinematic observables (relevant to possibility of Čerenkov radiation)

30 Constraints from ICARUS No visible distortion of neutrino energy spectrum No excess of e + e - pairs Cohen & Glashow: arxiv: ICARUS Collaboration: arxiv:

31 Gravitational Čerenkov Radiation Possible if speed > gravity waves, assumed = c Gravitational Čerenkov radiation: with OPERA δv ~ , maximum propagation time: Excludes GZK neutrinos (E ν ~ GeV, t ~ 10 8 y) by many orders of magnitude IceCube sees no neutrinos with E ν > GeV: would have t max < 10-4 s Alexandre, JE & Mavromatos: arxiv:

32 Revisiting Lorentz Violation with SN ν s 2D SN simulations suggest ringing on millisec scale If seen can be used to bound Lorentz violation Detectable in IceCube? Analyze emissions using wavelets Smear with δv(e) Bound if pulses seen JE, Janka, Mavromatos, Sakharov & Sarkisyan: arxiv:

33 Revisiting Lorentz Violation with SN ν s Short time-scale power disappears for time delay τ > 0.04 (s/mev) Potential constraints in linear case in quadratic case For subluminal (superluminal) propagation Potential for strong bound on δv(e) JE, Janka, Mavromatos, Sakharov & Sarkisyan: arxiv:

34 Space-Time Foam?

35 Nature of Quantum Gravity Vacuum Expect quantum fluctuations in fabric of space-time In natural Planckian units: ΔE, Δx, Δt, Δχ ~ 1 Fluctuations in energy, space, time, topology of order unity Space-time foam J.A.Wheeler Induce Lorentz violation?

36 Probes of Lorentz Violation for Photons Time delay from distant object: Compare arrivals of photons of different energies from astrophysical source with small intrinsic δt Gamma-Ray Bursters, pulsars, active galaxies, Typical sensitivities: Amelino-Camelia, JE, Mavromatos, Nanopoulos + Sarkar: 1997

37 Robust Analysis of GRB Data Corrected treatment of redshift Improved lower limit: JE, Mavromatos, Nanopoulos, Sakharov + Sarkisyan: astro-ph/

38 Time Delay from Markarian 501? Arrival time delay of ~ 4 minutes reported for photons in highest-energy bin Sensitive to M QG1 ~ GeV MAGIC Collaboration: astro-ph/

39 Results for AGN Markarian 501 Significance of time delay < 95% Linear dispersion: (E/M QG1 ) One-σ range: M QG1 = (0.34 to 0.78) x GeV 95% CL lower limit: M QG1 > 0.26 x GeV Quadratic dispersion: (E/M QG2 ) 2 One-σ range: M QG2 = (0.47 to 1.1) x GeV 95% CL lower limit: M QG2 > 0.27 x GeV Cannot exclude initial time delay at source MAGIC Collaboration + JE, Mavromatos, Nanopoulos, Sakharov, Sarkisyan: arxiv:0708:2889 [astro-ph]

40 Analysis of AGN PKS Observation by HESS of multiple flaring of AGN at larger redshift with more statistics HESS Collaboration: arxiv:0706:0797 [astro-ph]

41 Analysis of AGN PKS Comparison between HESS data in different energy bins No significant differences in arrival times Lower limit on m QG > GeV HESS Collaboration: arxiv:1101:33650 [astro-ph]

42 Fermi Analysis of GRB Redshift z = ± γ energies up to 31 GeV No hint of energydependent time delay Lower limit on m QG depends sensitively on assumptions m QG > 1.2 to 102 m P Fermi Collaboration: arxiv: [astro-ph]

43 The Story so far No technical error found OPERA carried out test with separated bunches No theoretical error found Difficult to reconcile with other constraints (SN1987a, Cohen-Glashow radiation, ) No direct contradiction with other experiments Other experiments are preparing to check This is how science should be done (technical scrutiny, verification, tests, theory)

44

45 Comparison of Electron Constraints Much stronger than ν constraints

The Neutrino of the OPERA:

The Neutrino of the OPERA: The Neutrino of the OPERA: constraints on neutrino velocity. Giacomo Cacciapaglia KC London & IPN Lyon meeting @ King s College London 23 November 2011 Experimental situation OPERA announced a time of

More information

What We Really Know About Neutrino Speeds

What We Really Know About Neutrino Speeds What We Really Know About Neutrino Speeds Brett Altschul University of South Carolina March 22, 2013 In particle physics, the standard model has been incredibly successful. If the Higgs boson discovered

More information

Probes of Lorentz Invariance Violation (with gamma-rays) Ulisses Barres de Almeida CTA Science Meeting - Leicester

Probes of Lorentz Invariance Violation (with gamma-rays) Ulisses Barres de Almeida CTA Science Meeting - Leicester Probes of Lorentz Invariance Violation (with gamma-rays) Ulisses Barres de Almeida CTA Science Meeting - Leicester Talk Outline Lorentz Invariance Violation Time-of-Flight Experiments Search Methodologies:

More information

Probing Lorentz Invariance Violation

Probing Lorentz Invariance Violation University of Washington, Seattle, WA with high-energy astrophysical neutrinos based on PRD 87 116009 (2013) Department of Physics Arizona State University Enrico.Borriello@asu.edu June 8 th, 2015 In collaboration

More information

String Theory in the LHC Era

String Theory in the LHC Era String Theory in the LHC Era J Marsano (marsano@uchicago.edu) 1 String Theory in the LHC Era 1. Electromagnetism and Special Relativity 2. The Quantum World 3. Why do we need the Higgs? 4. The Standard

More information

STREAM OF DARK MATTER AS A POSSIBLE CAUSE OF THE OPERA CLOCKS SYNCHRONIZATION SIGNALS DELAY

STREAM OF DARK MATTER AS A POSSIBLE CAUSE OF THE OPERA CLOCKS SYNCHRONIZATION SIGNALS DELAY STREAM OF DARK MATTER AS A POSSIBLE CAUSE OF THE OPERA CLOCKS SYNCHRONIZATION SIGNALS DELAY Jean Paul Mbelek 1 1. Sangha Center for Astronomy, Astrophysics and Cosmology, Sangha, Mali Correspondence to:

More information

Particle Physics Beyond Laboratory Energies

Particle Physics Beyond Laboratory Energies Particle Physics Beyond Laboratory Energies Francis Halzen Wisconsin IceCube Particle Astrophysics Center Nature s accelerators have delivered the highest energy protons, photons and neutrinos closing

More information

Vasiliki A. Mitsou. IFIC Valencia TAUP International Conference on Topics in Astroparticle and Underground Physics

Vasiliki A. Mitsou. IFIC Valencia TAUP International Conference on Topics in Astroparticle and Underground Physics Vasiliki A. Mitsou IFIC Valencia TAUP 2009 International Conference on Topics in Astroparticle and Underground Physics Rome, Italy, 1-5 July 2009 Dark energy models CDM Super-horizon CDM (SHCDM) [Kolb,

More information

arxiv: v1 [hep-ph] 17 Aug 2010

arxiv: v1 [hep-ph] 17 Aug 2010 1 arxiv:1008.2913v1 [hep-ph] 17 Aug 2010 CONSTRAINING LORENTZ INVARIANCE VIOLATION WITH FERMI V. VASILEIOU for the Fermi GBM and LAT Collaborations NASA Goddard Space Flight Center & University of Maryland,

More information

Relativity, Gravitation, and Cosmology

Relativity, Gravitation, and Cosmology Relativity, Gravitation, and Cosmology A basic introduction TA-PEI CHENG University of Missouri St. Louis OXFORD UNIVERSITY PRESS Contents Parti RELATIVITY Metric Description of Spacetime 1 Introduction

More information

Lorentz Invariance Violation: from theoretical and phenomenological perspectives

Lorentz Invariance Violation: from theoretical and phenomenological perspectives Lorentz Invariance Violation: from theoretical and phenomenological perspectives Bo-Qiang Ma ( 马伯强 ) Peking University ( 北京大学 ) Talk at Workshop on Lorentz and CPT Violation in Astrophysics and Cosmology

More information

First combined studies on Lorentz Invariance Violation from observations of astrophysical sources

First combined studies on Lorentz Invariance Violation from observations of astrophysical sources First combined studies on Lorentz Invariance Violation from observations of astrophysical sources Leyre Nogués, Tony T.Y. Lin, Cedric Perennes, Alasdair E. Gent, Julien Bolmont, Markus Gaug, Agnieszka

More information

Possible sources of very energetic neutrinos. Active Galactic Nuclei

Possible sources of very energetic neutrinos. Active Galactic Nuclei Possible sources of very energetic neutrinos Active Galactic Nuclei 1 What might we learn from astrophysical neutrinos? Neutrinos not attenuated/absorbed Information about central engines of astrophysical

More information

arxiv: v3 [hep-ph] 6 Sep 2016

arxiv: v3 [hep-ph] 6 Sep 2016 Light speed variation from gamma-ray bursts Haowei Xu a, Bo-Qiang Ma a,b,c,d, a School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 1871, China b Collaborative

More information

High Energy Emission. Brenda Dingus, LANL HAWC

High Energy Emission. Brenda Dingus, LANL HAWC High Energy Emission from GRBs Brenda Dingus, LANL HAWC What are GRBs? Cosmological distance Typical observed z>1 Energy released is up to few times the rest mass of Sun (if isotropic) in a few seconds

More information

SPECIAL RELATIVITY! (Einstein 1905)!

SPECIAL RELATIVITY! (Einstein 1905)! SPECIAL RELATIVITY! (Einstein 1905)! Motivations:! Explaining the results of the Michelson-Morley! experiment without invoking a force exerted! on bodies moving through the aether.! Make the equations

More information

Regularity of high energy photon events from gamma ray bursts 1

Regularity of high energy photon events from gamma ray bursts 1 Prepared for submission to JCAP Regularity of high energy photon events from gamma ray bursts 1 arxiv:181.884v2 [gr-qc] 6 Feb 218 Haowei Xu, a Bo-Qiang Ma 2a,b,c,d a chool of Physics and tate Key Laboratory

More information

square kilometer array: a powerful tool to test theories of gravity and cosmological models

square kilometer array: a powerful tool to test theories of gravity and cosmological models square kilometer array: a powerful tool to test theories of gravity and cosmological models mairi sakellariadou king s college london fundamental physics with the SKA flic-en-flac, mauritius, 30/4-5/5/

More information

Pair Production Constraints on Superluminal Neutrinos Revisited

Pair Production Constraints on Superluminal Neutrinos Revisited SLAC-PUB-14812 Pair Production Constraints on Superluminal Neutrinos Revisited Stanley J. Brodsky SLAC National Accelerator Laboratory, Stanford University, Stanford, California 94309 Susan Gardner Department

More information

Clock Adjustments for Neutrino Velocity Measurement. Tim Joslin

Clock Adjustments for Neutrino Velocity Measurement. Tim Joslin Clock Adjustments for Neutrino Velocity Measurement Tim Joslin Contents Abstract... 3 1 Introduction... 4 2 Einstein s Train Thought-Experiment... 4 2.1 The Relativity of Simultaneity... 4 2.2 Adjusting

More information

arxiv: v2 [hep-ph] 14 Mar 2012

arxiv: v2 [hep-ph] 14 Mar 2012 CERN-PH-TH/2011 234 Interpreting OPERA results on superluminal neutrino arxiv:1109.5682v2 [hep-ph] 14 Mar 2012 Gian F. Giudice a, Sergey Sibiryakov b, Alessandro Strumia c,d a CERN, Theory Division, CH

More information

Fermi: Highlights of GeV Gamma-ray Astronomy

Fermi: Highlights of GeV Gamma-ray Astronomy Fermi: Highlights of GeV Gamma-ray Astronomy Dave Thompson NASA GSFC On behalf of the Fermi Gamma-ray Space Telescope Large Area Telescope Collaboration Neutrino Oscillation Workshop Otranto, Lecce, Italy

More information

Gamma-ray Astrophysics

Gamma-ray Astrophysics Gamma-ray Astrophysics AGN Pulsar SNR GRB Radio Galaxy The very high energy -ray sky NEPPSR 25 Aug. 2004 Many thanks to Rene Ong at UCLA Guy Blaylock U. of Massachusetts Why gamma rays? Extragalactic Background

More information

Experimental Tests and Alternative Theories of Gravity

Experimental Tests and Alternative Theories of Gravity Experimental Tests and Alternative Theories of Gravity Gonzalo J. Olmo Alba gonzalo.olmo@uv.es University of Valencia (Spain) & UW-Milwaukee Experimental Tests and Alternative Theories of Gravity p. 1/2

More information

Generalized Dirac Equations and Neutrinos

Generalized Dirac Equations and Neutrinos Generalized Dirac Equations and Neutrinos GEORGE MASON UNIVERSITY FAIRFAX VIRGINIA USA 06-DEC-2012 U. D. Jentschura Missouri University of Science and Technology Rolla, Missouri In exploring nature, a

More information

Emergent Dimensions. Bob Poltis. SUNY at Buffalo. Essential Cosmology for the Next Generation Cosmology on the Beach January 20, 2012 Cancún, Mexico

Emergent Dimensions. Bob Poltis. SUNY at Buffalo. Essential Cosmology for the Next Generation Cosmology on the Beach January 20, 2012 Cancún, Mexico Emergent Dimensions Bob Poltis SUNY at Buffalo Essential Cosmology for the Next Generation Cosmology on the Beach January 0, 01 Cancún, Mexico Extra Dimensions Add extra dimensions (make model more complicated:

More information

How well have we tested Einstein s Special Relativity?

How well have we tested Einstein s Special Relativity? How well have we tested Einstein s Special Relativity? There was a young lady named Bright, Whose speed was far faster than light; She started one day In a relative way, And returned on the previous night.

More information

New Tests of Lorentz Invariance Following from Observations of. the Highest Energy Cosmic Gamma Rays. Abstract

New Tests of Lorentz Invariance Following from Observations of. the Highest Energy Cosmic Gamma Rays. Abstract New Tests of Lorentz Invariance Following from Observations of the Highest Energy Cosmic Gamma Rays F.W. Stecker NASA Goddard Space Flight Center, Greenbelt, MD 20771 Sheldon L. Glashow Boston University,

More information

Aspects of Spontaneous Lorentz Violation

Aspects of Spontaneous Lorentz Violation Aspects of Spontaneous Lorentz Violation Robert Bluhm Colby College IUCSS School on CPT & Lorentz Violating SME, Indiana University, June 2012 Outline: I. Review & Motivations II. Spontaneous Lorentz Violation

More information

Physics of Short Gamma-Ray Bursts Explored by CTA and DECIGO/B-DECIGO

Physics of Short Gamma-Ray Bursts Explored by CTA and DECIGO/B-DECIGO Physics of Short Gamma-Ray Bursts Explored by CTA and DECIGO/B-DECIGO Hiroyasu Tajima Institute for Space Earth Environmental Research Nagoya University 17th DECIGO Workshop Nov 1, 18 Nagoya University

More information

The ATLAS Experiment and the CERN Large Hadron Collider

The ATLAS Experiment and the CERN Large Hadron Collider The ATLAS Experiment and the CERN Large Hadron Collider HEP101-2 January 28, 2013 Al Goshaw 1 HEP 101-2 plan Jan. 14: Introduction to CERN and ATLAS DONE Today: 1. Comments on grant opportunities 2. Overview

More information

2.5.1 Static tides Tidal dissipation Dynamical tides Bibliographical notes Exercises 118

2.5.1 Static tides Tidal dissipation Dynamical tides Bibliographical notes Exercises 118 ii Contents Preface xiii 1 Foundations of Newtonian gravity 1 1.1 Newtonian gravity 2 1.2 Equations of Newtonian gravity 3 1.3 Newtonian field equation 7 1.4 Equations of hydrodynamics 9 1.4.1 Motion of

More information

Applications of PT Symmetry and Pseudo-Hermiticity: From the Imaginary Cubic Perturbation to Elementary Particle Physics

Applications of PT Symmetry and Pseudo-Hermiticity: From the Imaginary Cubic Perturbation to Elementary Particle Physics Applications of PT Symmetry and Pseudo-Hermiticity: From the Imaginary Cubic Perturbation to Elementary Particle Physics PHHQP-12 Conference 2013 Koc University [Thanks to the Organizers for Recognizing

More information

Beyond the standard model? From last time. What does the SM say? Grand Unified Theories. Unifications: now and the future

Beyond the standard model? From last time. What does the SM say? Grand Unified Theories. Unifications: now and the future From last time Quantum field theory is a relativistic quantum theory of fields and interactions. Fermions make up matter, and bosons mediate the forces by particle exchange. Lots of particles, lots of

More information

Emmanuel Moulin! on behalf of the CTA Consortium!!! Rencontres de Moriond 2013! Very High Energy Phenomena in the Universe! March 9-16, La Thuile,

Emmanuel Moulin! on behalf of the CTA Consortium!!! Rencontres de Moriond 2013! Very High Energy Phenomena in the Universe! March 9-16, La Thuile, Emmanuel Moulin! on behalf of the CTA Consortium!!! Rencontres de Moriond 2013! Very High Energy Phenomena in the Universe! March 9-16, La Thuile, Italy Emmanuel Moulin CTA meeting, Zürich 2009 1 Core-energy

More information

Retro-causal Holographic Dark Energy Coherent Vacuum Super-Solid Tetrad Emergent Gravity. Jack Sarfatti Cal Tech APS 10/30/10

Retro-causal Holographic Dark Energy Coherent Vacuum Super-Solid Tetrad Emergent Gravity. Jack Sarfatti   Cal Tech APS 10/30/10 Retro-causal Holographic Dark Energy Coherent Vacuum Super-Solid Tetrad Emergent Gravity Jack Sarfatti http://stardrive.org Cal Tech APS 10/30/10 Abstract A short review of experiments and theory suggesting

More information

Quantum Gravity and Entanglement

Quantum Gravity and Entanglement Quantum Gravity and Entanglement The magnetic induction creates a negative electric field, causing an electromagnetic inertia responsible for the relativistic mass change; it is the mysterious Higgs Field

More information

Particles and Deep Inelastic Scattering

Particles and Deep Inelastic Scattering Particles and Deep Inelastic Scattering Heidi Schellman University HUGS - JLab - June 2010 June 2010 HUGS 1 Course Outline 1. Really basic stuff 2. How we detect particles 3. Basics of 2 2 scattering 4.

More information

Violation of Lorentz Invariance in High-Energy γ Rays

Violation of Lorentz Invariance in High-Energy γ Rays Violation of Lorentz Invariance in High-Energy γ Rays M. E. Peskin July, 2005 There is a huge literature on Lorentz-Invarance violation. I am no expert on the subject, but hopefully I can give you some

More information

Faster-than-light-neutrinos

Faster-than-light-neutrinos Faster-than-light-neutrinos Karlstads universitet Fakulteten för teknik och naturvetenskap Avdelningen för fysik och elektroteknik 19/1 2012 Sofie Yngman Table of content Background 3 Neutrinos 3 Past

More information

Explorations of Planck-scale Noise in Noncommutative Holographic Spacetime 1

Explorations of Planck-scale Noise in Noncommutative Holographic Spacetime 1 Explorations of Planck-scale Noise in Noncommutative Holographic Spacetime 1 Ohkyung Kwon 1 C. J. Hogan, "Interferometers as Holograpic Clocks," arxiv:1002.4880 [gr-qc] Motivation Events in spacetime are

More information

The ATLAS Experiment and the CERN Large Hadron Collider

The ATLAS Experiment and the CERN Large Hadron Collider The ATLAS Experiment and the CERN Large Hadron Collider HEP101-2 April 5, 2010 A. T. Goshaw Duke University 1 HEP 101 Plan March 29: Introduction and basic HEP terminology March 30: Special LHC event:

More information

Introduction to Particle Physics

Introduction to Particle Physics Introduction to Particle Physics The Particle Zoo Symmetries The Standard Model Thomas Gajdosik Vilnius Universitetas Teorinės Fizikos Katedra Introduction to Particle Physics http://web.vu.lt/ff/t.gajdosik/wop/

More information

Special Relativity from Soft Gravitons

Special Relativity from Soft Gravitons Special Relativity from Soft Gravitons Mark Hertzberg, Tufts University CosPA, December 14, 2017 with McCullen Sandora, PRD 96 084048 (1704.05071) Can the laws of special relativity be violated in principle?

More information

Relativity and Black Holes

Relativity and Black Holes Relativity and Black Holes Post-MS Evolution of Very High Mass (>15 M Θ ) Stars similar to high mass except more rapid lives end in Type II supernova explosions main difference: mass of iron core at end

More information

Stephen Blaha, Ph.D. M PubHsMtw

Stephen Blaha, Ph.D. M PubHsMtw Quantum Big Bang Cosmology: Complex Space-time General Relativity, Quantum Coordinates,"Dodecahedral Universe, Inflation, and New Spin 0, 1 / 2,1 & 2 Tachyons & Imagyons Stephen Blaha, Ph.D. M PubHsMtw

More information

Illustration of the Emergence of Fundamental Forces

Illustration of the Emergence of Fundamental Forces Copyright 2017 by Sylwester Kornowski All rights reserved Illustration of the Emergence of Fundamental Forces Sylwester Kornowski Abstract: Here, within the Scale-Symmetric Theory (SST), we illustrate

More information

Class Notes Introduction to Modern Physics Physics 321 Plan II Under Construction

Class Notes Introduction to Modern Physics Physics 321 Plan II Under Construction Class Notes Introduction to Modern Physics Physics 321 Plan II Under Construction Austin M. Gleeson 1 Department of Physics University of Texas at Austin Austin, TX 78712 January 15, 2010 1 gleeson@physics.utexas.edu

More information

Adding Light to the Gravitational Waves on the Null Cone

Adding Light to the Gravitational Waves on the Null Cone Marshall University Marshall Digital Scholar Physics Faculty Research Physics Spring 4-2014 Adding Light to the Gravitational Waves on the Null Cone Maria Babiuc-Hamilton Marshall University, babiuc@marshall.edu

More information

Fourth International Workshop on Theoretical and Phenomenological Aspects of Underground Physics, Toledo (Spain) September

Fourth International Workshop on Theoretical and Phenomenological Aspects of Underground Physics, Toledo (Spain) September Fourth International Workshop on Theoretical and Phenomenological Aspects of Underground Physics, Toledo (Spain) September 17-21 1995 COSMOLOGICAL IMPLICATIONS OF A POSSIBLE CLASS OF PARTICLES ABLE TO

More information

16. Einstein and General Relativistic Spacetimes

16. Einstein and General Relativistic Spacetimes 16. Einstein and General Relativistic Spacetimes Problem: Special relativity does not account for the gravitational force. To include gravity... Geometricize it! Make it a feature of spacetime geometry.

More information

PRINCIPLES OF PHYSICS. \Hp. Ni Jun TSINGHUA. Physics. From Quantum Field Theory. to Classical Mechanics. World Scientific. Vol.2. Report and Review in

PRINCIPLES OF PHYSICS. \Hp. Ni Jun TSINGHUA. Physics. From Quantum Field Theory. to Classical Mechanics. World Scientific. Vol.2. Report and Review in LONDON BEIJING HONG TSINGHUA Report and Review in Physics Vol2 PRINCIPLES OF PHYSICS From Quantum Field Theory to Classical Mechanics Ni Jun Tsinghua University, China NEW JERSEY \Hp SINGAPORE World Scientific

More information

Those invisible neutrinos

Those invisible neutrinos Those invisible neutrinos and their astroparticle physics Amol Dighe Department of Theoretical Physics Tata Institute of Fundamental Research, Mumbai Bhoutics, IITM, March 31st, 2017 Those invisible neutrinos...

More information

PoS(ICRC2017)556. Effects of Lorentz invariance violation on cosmic ray photon emission and gamma ray decay processes

PoS(ICRC2017)556. Effects of Lorentz invariance violation on cosmic ray photon emission and gamma ray decay processes Effects of Lorentz invariance violation on cosmic ray photon emission and gamma ray decay processes a,b and A. Pérez-Lorenzana b a Instituto de Física de São Carlos, Universidade de São Paulo, Av. Trabalhador

More information

David Mattingly University of California-Davis

David Mattingly University of California-Davis David Mattingly University of California-Davis Quantum gravity in the Americas III Penn State August 26 th, 2006 What is QG phenomenology? The search for effects at low energies(

More information

Jarek Nowak University of Minnesota. High Energy seminar, University of Virginia

Jarek Nowak University of Minnesota. High Energy seminar, University of Virginia Jarek Nowak University of Minnesota High Energy seminar, University of Virginia Properties of massive neutrinos in the Standard Model. Electromagnetic properties of neutrinos. Neutrino magnetic moment.

More information

Hadronic Search for SUSY with MT2 variable

Hadronic Search for SUSY with MT2 variable Hadronic Search for SUSY with MT2 variable Esmaeel Eskandari on behalf of the CMS Collaboration School of Particles & Accelerators, Institute for Research in Fundamental Sciences (IPM) The 2nd IPM Meeting

More information

NEUTRINOS. Concha Gonzalez-Garcia. San Feliu, June (Stony Brook-USA and IFIC-Valencia)

NEUTRINOS. Concha Gonzalez-Garcia. San Feliu, June (Stony Brook-USA and IFIC-Valencia) NEUTRINOS (Stony Brook-USA and IFIC-Valencia San Feliu, June 2004 Plan of Lectures I. Standard Neutrino Properties and Mass Terms (Beyond Standard II. Neutrino Oscillations III. The Data and Its Interpretation

More information

Special Relativity. Principles of Special Relativity: 1. The laws of physics are the same for all inertial observers.

Special Relativity. Principles of Special Relativity: 1. The laws of physics are the same for all inertial observers. Black Holes Special Relativity Principles of Special Relativity: 1. The laws of physics are the same for all inertial observers. 2. The speed of light is the same for all inertial observers regardless

More information

The cosmological constant puzzle

The cosmological constant puzzle The cosmological constant puzzle Steven Bass Cosmological constant puzzle: Accelerating Universe: believed to be driven by energy of nothing (vacuum) Vacuum energy density (cosmological constant or dark

More information

dt = p m, (2.1.1) dt = p

dt = p m, (2.1.1) dt = p Chapter 2 Special relativity 2.1 Galilean relativity We start our discussion of symmetries by considering an important example of an invariance, i.e. an invariance of the equations of motion under a change

More information

M. Lattanzi. 12 th Marcel Grossmann Meeting Paris, 17 July 2009

M. Lattanzi. 12 th Marcel Grossmann Meeting Paris, 17 July 2009 M. Lattanzi ICRA and Dip. di Fisica - Università di Roma La Sapienza In collaboration with L. Pieri (IAP, Paris) and J. Silk (Oxford) Based on ML, Silk, PRD 79, 083523 (2009) and Pieri, ML, Silk, MNRAS

More information

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

Lecture 03. The Standard Model of Particle Physics. Part II The Higgs Boson Properties of the SM Lecture 03 The Standard Model of Particle Physics Part II The Higgs Boson Properties of the SM The Standard Model So far we talked about all the particles except the Higgs If we know what the particles

More information

Neutrino Oscillations and the Matter Effect

Neutrino Oscillations and the Matter Effect Master of Science Examination Neutrino Oscillations and the Matter Effect RAJARSHI DAS Committee Walter Toki, Robert Wilson, Carmen Menoni Overview Introduction to Neutrinos Two Generation Mixing and Oscillation

More information

On the Extended Lorentz Transformation Model and Its Application to Superluminal Neutrinos

On the Extended Lorentz Transformation Model and Its Application to Superluminal Neutrinos Journal of Modern Physics, 01, 3, 101-106 http://dx.doi.org/10.36/jmp.01.3913 Published Online September 01 (http://www.scirp.org/journal/jmp) On the Extended Lorentz Transformation Model and Its Application

More information

Fundamental Particles

Fundamental Particles Fundamental Particles Standard Model of Particle Physics There are three different kinds of particles. Leptons - there are charged leptons (e -, μ -, τ - ) and uncharged leptons (νe, νμ, ντ) and their

More information

Spectra of Cosmic Rays

Spectra of Cosmic Rays Spectra of Cosmic Rays Flux of relativistic charged particles [nearly exactly isotropic] Particle density Power-Law Energy spectra Exponent (p, Nuclei) : Why power laws? (constraint on the dynamics of

More information

Outline. Charged Leptonic Weak Interaction. Charged Weak Interactions of Quarks. Neutral Weak Interaction. Electroweak Unification

Outline. Charged Leptonic Weak Interaction. Charged Weak Interactions of Quarks. Neutral Weak Interaction. Electroweak Unification Weak Interactions Outline Charged Leptonic Weak Interaction Decay of the Muon Decay of the Neutron Decay of the Pion Charged Weak Interactions of Quarks Cabibbo-GIM Mechanism Cabibbo-Kobayashi-Maskawa

More information

Nuclear and Particle Physics

Nuclear and Particle Physics Nuclear and Particle Physics W. S. С Williams Department of Physics, University of Oxford and St Edmund Hall, Oxford CLARENDON PRESS OXFORD 1991 Contents 1 Introduction 1.1 Historical perspective 1 1.2

More information

Neutrinos and DM (Galactic)

Neutrinos and DM (Galactic) Neutrinos and DM (Galactic) ArXiv:0905.4764 ArXiv:0907.238 ArXiv: 0911.5188 ArXiv:0912.0512 Matt Buckley, Katherine Freese, Dan Hooper, Sourav K. Mandal, Hitoshi Murayama, and Pearl Sandick Basic Result

More information

The Scale-Symmetric Theory as the Origin of the Standard Model

The Scale-Symmetric Theory as the Origin of the Standard Model Copyright 2017 by Sylwester Kornowski All rights reserved The Scale-Symmetric Theory as the Origin of the Standard Model Sylwester Kornowski Abstract: Here we showed that the Scale-Symmetric Theory (SST)

More information

The T2K experiment Results and Perspectives. PPC2017 Corpus Christi Mai 2017 Michel Gonin On behalf of the T2K collaboration

The T2K experiment Results and Perspectives. PPC2017 Corpus Christi Mai 2017 Michel Gonin On behalf of the T2K collaboration The T2K experiment Results and Perspectives PPC2017 Corpus Christi Mai 2017 Michel Gonin On behalf of the T2K collaboration 1 Overview Neutrino oscillations The T2K off-axis experiment Oscillation results

More information

The Correct Interpretation of the Kaluza-Klein Theory

The Correct Interpretation of the Kaluza-Klein Theory Copyright 2014 by Sylwester Kornowski All rights reserved The Correct Interpretation of the Kaluza-Klein Theory Sylwester Kornowski Abstract: Here, within the Scale-Symmetric Everlasting Theory (S-SET),

More information

Elementary Particles, Flavour Physics and all that...

Elementary Particles, Flavour Physics and all that... Elementary Particles, Flavour Physics and all that... 1 Flavour Physics The term Flavour physics was coined in 1971 by Murray Gell-Mann and his student at the time, Harald Fritzsch, at a Baskin-Robbins

More information

Chris Verhaaren Joint Theory Seminar 31 October With Zackaria Chacko, Rashmish Mishra, and Simon Riquelme

Chris Verhaaren Joint Theory Seminar 31 October With Zackaria Chacko, Rashmish Mishra, and Simon Riquelme Chris Verhaaren Joint Theory Seminar 31 October 2016 With Zackaria Chacko, Rashmish Mishra, and Simon Riquelme It s Halloween A time for exhibiting what some find frightening And seeing that it s not so

More information

A first trip to the world of particle physics

A first trip to the world of particle physics A first trip to the world of particle physics Itinerary Massimo Passera Padova - 13/03/2013 1 Massimo Passera Padova - 13/03/2013 2 The 4 fundamental interactions! Electromagnetic! Weak! Strong! Gravitational

More information

Appendix A2. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France.

Appendix A2. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France. Appendix A. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France. Prepared by: Arash Akbari-Sharbaf Why Build Accelerators? Probe deeper From

More information

Gravitational Waves and High Energy Neutrino coincidences : The gwhen Project

Gravitational Waves and High Energy Neutrino coincidences : The gwhen Project Gravitational Waves and High Energy Neutrino coincidences : The gwhen Project Thierry Pradier for the gwhen Group IPHC (IN2P3) & University of Strasbourg Antares : B. Baret, B. Bouhou, A. Kouchner, L.

More information

Cosmic Rays: A Way to Introduce Modern Physics Concepts. Steve Schnetzer

Cosmic Rays: A Way to Introduce Modern Physics Concepts. Steve Schnetzer Cosmic Rays: A Way to Introduce Modern Physics Concepts Steve Schnetzer Rutgers CR Workshop May 19, 2007 Concepts Astrophysics Particle Physics Radiation Relativity (time dilation) Solar Physics Particle

More information

A. Chen (INAF-IASF Milano) On behalf of the Fermi collaboration

A. Chen (INAF-IASF Milano) On behalf of the Fermi collaboration A. Chen (INAF-IASF Milano) On behalf of the Fermi collaboration Astro-Siesta, May 13 th 2010 Why is it important? Contains information about the evolution of matter in the universe: star formation history,

More information

Astrophysical Radiation Processes

Astrophysical Radiation Processes PHY3145 Topics in Theoretical Physics Astrophysical Radiation Processes 3: Relativistic effects I Dr. J. Hatchell, Physics 407, J.Hatchell@exeter.ac.uk Course structure 1. Radiation basics. Radiative transfer.

More information

Neutrino Oscillations and Astroparticle Physics (5) John Carr Centre de Physique des Particules de Marseille (IN2P3/CNRS) Pisa, 10 May 2002

Neutrino Oscillations and Astroparticle Physics (5) John Carr Centre de Physique des Particules de Marseille (IN2P3/CNRS) Pisa, 10 May 2002 Neutrino Oscillations and Astroparticle Physics (5) John Carr Centre de Physique des Particules de Marseille (IN2P3/CNRS) Pisa, 10 May 2002 n High Energy Astronomy Multi-Messanger Astronomy Cosmic Rays

More information

Quantum Physics and Beyond

Quantum Physics and Beyond Physics 120 John Harris 1 Physics 120 Announcements / Issues Quiz next week at beginning of class Covers everything up through last week s class (see next 2 slides), through Reading assignments including

More information

Radiation processes and mechanisms in astrophysics I. R Subrahmanyan Notes on ATA lectures at UWA, Perth 18 May 2009

Radiation processes and mechanisms in astrophysics I. R Subrahmanyan Notes on ATA lectures at UWA, Perth 18 May 2009 Radiation processes and mechanisms in astrophysics I R Subrahmanyan Notes on ATA lectures at UWA, Perth 18 May 009 Light of the night sky We learn of the universe around us from EM radiation, neutrinos,

More information

Searches for Local Lorentz Violation

Searches for Local Lorentz Violation Searches for Local Lorentz Violation Jay D. Tasson St. Olaf College outline background motivation SME gravity theory pure-gravity sector matter-gravity couplings experiments & observations motivation E

More information

On the Neutrino Opera in the CNGS Beam

On the Neutrino Opera in the CNGS Beam October, 2011 PROGRESS IN PHYSICS Volume 4 On the Neutrino Opera in the CNGS Beam Armando V.D.B. Assis Departamento de Física, Universidade Federal de Santa Catarina UFSC, Trindade 88040 900, Florianópolis,

More information

Introduction to Neutrino Physics. TRAN Minh Tâm

Introduction to Neutrino Physics. TRAN Minh Tâm Introduction to Neutrino Physics TRAN Minh Tâm LPHE/IPEP/SB/EPFL This first lecture is a phenomenological introduction to the following lessons which will go into details of the most recent experimental

More information

High-Energy Emission from GRBs: First Year Highlights from the Fermi Gamma-ray Space Telescope

High-Energy Emission from GRBs: First Year Highlights from the Fermi Gamma-ray Space Telescope High-Energy Emission from GRBs: First Year Highlights from the Fermi Gamma-ray Space Telescope Jonathan Granot University of Hertfordshire (Royal Society Wolfson Research Merit Award Holder) on behalf

More information

Final Exam: Sat. Dec. 18, 2:45-4:45 pm, 1300 Sterling Exam is cumulative, covering all material. From last time

Final Exam: Sat. Dec. 18, 2:45-4:45 pm, 1300 Sterling Exam is cumulative, covering all material. From last time Final Exam: Sat. Dec. 18, 2:45-4:45 pm, 1300 Sterling Exam is cumulative, covering all material From last time Quantum field theory is a relativistic quantum theory of fields and interactions. Fermions

More information

Today in Astronomy 102: relativity, continued

Today in Astronomy 102: relativity, continued Today in Astronomy 10: relativity, continued Einstein s procedures and results on the special theory of relativity. Formulas and numerical examples of the effects of length contraction, time dilation,

More information

GW from GRBs Gravitational Radiation from Gamma-Ray Bursts

GW from GRBs Gravitational Radiation from Gamma-Ray Bursts GW from GRBs Gravitational Radiation from Gamma-Ray Bursts Tsvi Piran Racah Inst. of Jerusalem, Israel Dafne Guetta,, Ehud Nakar, Reem Sari Once or twice a day we see a burst of low energy gamma-rays from

More information

HAWC: A Next Generation All-Sky VHE Gamma-Ray Telescope

HAWC: A Next Generation All-Sky VHE Gamma-Ray Telescope HAWC: A Next Generation All-Sky VHE Gamma-Ray Telescope VHE Astrophysics Energy range 10 GeV 10 TeV Non thermal processes in the universe Highly variable sources Particle acceleration Physics of extreme

More information

The future of neutrino physics (at accelerators)

The future of neutrino physics (at accelerators) Mauro Mezzetto, Istituto Nazionale Fisica Nucleare, Padova The future of neutrino physics (at accelerators) Present Status Concepts, strategies, challenges The two players: Dune and Hyper-Kamiokande Conclusions

More information

electrodynamics and Lorentz violation

electrodynamics and Lorentz violation Vacuum Cherenkov radiation in Lorentz violating quantum electrodynamics and experimental limits on the scale of Lorentz violation Damiano Anselmi (IHEP/CAS, Beijing, & Pisa University) Lorentz symmetry

More information

Quantum Physics and General Relativity

Quantum Physics and General Relativity Quantum Physics and General Relativity The self maintained electric potential of the accelerating charges equivalent with the General Relativity space-time curvature, and since it is true on the quantum

More information

An Astrophysical Plasma Wakefield Accelerator. Alfven Wave Induced Plasma Wakefield Acceleration

An Astrophysical Plasma Wakefield Accelerator. Alfven Wave Induced Plasma Wakefield Acceleration An Astrophysical Plasma Wakefield Accelerator Alfven Wave Induced Plasma Wakefield Acceleration Laboratory Astrophysics at SLAC Study in a Laboratory setting: Fundamental physics Astrophysical Dynamics

More information

Search for high energy neutrino astrophysical sources with the ANTARES Cherenkov telescope

Search for high energy neutrino astrophysical sources with the ANTARES Cherenkov telescope Dottorato di Ricerca in Fisica - XXVIII ciclo Search for high energy neutrino astrophysical sources with the ANTARES Cherenkov telescope Chiara Perrina Supervisor: Prof. Antonio Capone 25 th February 2014

More information

Exam Results. Force between charges. Electric field lines. Other particles and fields

Exam Results. Force between charges. Electric field lines. Other particles and fields Exam: Exam scores posted on Learn@UW No homework due next week Exam Results F D C BC B AB A Phy107 Fall 2006 1 Particles and fields We have talked about several particles Electron,, proton, neutron, quark

More information

Searching for the Axion

Searching for the Axion Searching for the Axion Leslie J Rosenberg Lawrence Livermore National Laboratory August 2, 2004 Outline What is the axion? Axion properties. The window of allowed axion masses and couplings. Selected

More information

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

Contents. Preface to the First Edition Preface to the Second Edition Contents Preface to the First Edition Preface to the Second Edition Notes xiii xv xvii 1 Basic Concepts 1 1.1 History 1 1.1.1 The Origins of Nuclear Physics 1 1.1.2 The Emergence of Particle Physics: the

More information