A Direct Search for Magnetic Monopoles at H1 HEP03, Aachen, 17-23/7/03 David Milstead The University of Liverpool.

Slides:



Advertisements
Similar presentations
5th May 2010Fergus Wilson, RAL1 Experimental Particle Physics PHYS6011 Looking for Higgs and SUSY at the LHC or...what can you get for $10,000,000,000.
Advertisements

5th May 2011Fergus Wilson, RAL1 Experimental Particle Physics PHYS6011 Looking for Higgs and SUSY at the LHC or...what can you get for $10,000,000,000.
A Realization of Effective SUSY Zhen-hua Zhao ITP,CAS Liu & Zhao arXiv:
20.6 Force between Two Parallel Wires The magnetic field produced at the position of wire 2 due to the current in wire 1 is: The force this field exerts.
The largest contribution to the mass of the atom is: 1.Higgs field providing fundamental particle mass by interacting with quarks 2.Einstein’s E = mc 2.
Searching for Magnetic Monopoles
BSM searches at HERA John Martin University of Toronto / ZEUS for H1 and ZEUS.
Flavor Beyond the Standard Model Zurab Tavartkiladze, Gela Devidze Tbilisi State University Volkswagen meeting 14, 15 March 2013, Tbilisi.
APPEAL July '14Tony Weidberg, Oxford University1 Introduction To Particle Physics Why do we need accelerators and detectors? Particle Detectors with examples.
Physics with Single, Multi- & Di-Photons at LEP HEP2003, Aachen, July HEP2003, Aachen, July Marat Gataullin (Caltech/L3) on behalf of LEP Collaborations.
MAGNETIC MONOPOLES Andrey Shmakov Physics 129 Fall 2010 UC Berkeley.
Yingchuan Li Weak Mixing Angle and EIC INT Workshop on Pertubative and Non-Pertubative Aspects of QCD at Collider Energies Sep. 17th 2010.
Susy05, Durham 21 st July1 Split SUSY at Colliders Peter Richardson Durham University Work done in collaboration with W. Kilian, T. Plehn and E. Schmidt,
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.
The Large Hadron Collider -Exploring a New Energy Frontier
The Fundamental Theorem of Calculus
Constrained MSSM Unification of the gauge couplings Radiative EW Symmetry Breaking Heavy quark and lepton masses Rare decays (b -> sγ, b->μμ) Anomalous.
The CMS Muon Detector Thomas Hebbeker Aachen July 2001 Searching for New Physics with High Energy Muons.
P Spring 2002 L9Richard Kass Four Quarks Once the charm quark was discovered SU(3) was extended to SU(4) !
Search for Anomalous tWb Couplings at D0, L. Li (Shanghai Jiao Tong University) SUSY 2012, August 16, Liang Li Shanghai Jiao Tong University Search.
A review on magnetic monopoles What is a RPP review good for ? Why are monopoles important ? What is already in the RPP ? Why is a monopole review desirable.
ROY, D. (2011). Why Large Hadron Collider?. Pramana: Journal Of Physics, 76(5), doi: /s
Tests of the Standard Model and constraints on new physics from Fermion-pair production at LEP2 Georgios Anagnostou INP Demokritos Athens/Birmingham University.
Charged Higgs Results from Tevatron Sudeshna Banerjee Tata Institute of Fundamental Research Mumbai, India For CDF and DØ Collaborations Fermilab, Chicago.
Flavor Beyond Standard Model G.G. Devidze High Energy Physics Institute of Tbilisi State University 1.Introduction 2.Flavor beyond the standard model 3.Heavy.
Calibration of the ZEUS calorimeter for electrons Alex Tapper Imperial College, London for the ZEUS Collaboration Workshop on Energy Calibration of the.
Motivation Polarized 3 He gas target Solenoid design and test 3 He feasibility test Summary and outlook Johannes Gutenberg-Universit ä t Mainz Institut.
Copyright © 2009 Pearson Education, Inc. Applications: Motors, Loudspeakers, Galvanometers.
Work partially supported by under Contract 32/2011.
Introduction to CERN David Barney, CERN Introduction to CERN Activities Intro to particle physics Accelerators – the LHC Detectors - CMS.
1 Search for Magnetic Monopoles at the Relativistic Heavy Ion Collider (RHIC) Praveen Chaudhari *, Vasily Dzhordzhadze, Veljko Radeka, Margareta Rehak,
Neutralino Dark Matter in Light Higgs Boson Scenario (LHS) The scenario is consistent with  particle physics experiments Particle mass b → sγ Bs →μ +
What is the Higgs??? Prof Nick Evans University of Southampton.
INVASIONS IN PARTICLE PHYSICS Compton Lectures Autumn 2001 Lecture 8 Dec
LOGO B. I. Stepanov Institute of Physics National Academy of Sciences of Belarus.
Search for a Z′ boson in the dimuon channel in p-p collisions at √s = 7TeV with CMS experiment at the Large Hadron Collider Search for a Z′ boson in the.
C. K. MackayEPS 2003 Electroweak Physics and the Top Quark Mass at the LHC Kate Mackay University of Bristol On behalf of the Atlas & CMS Collaborations.
ATLAS experiment at the CERN Large Hadron Collider Peter Watkins, Head of Particle Physics Group, University of Birmingham, UK
8 th Topical Seminar on “Innovative Particle and Radiation Detectors” Siena Oct CALIBRATION AND SEARCH FOR EXOTIC PARTICLES WITH CR39 AND MAKROFOL.
Latest Physics Results from ALEPH Paolo Azzurri CERN - July 15, 2003.
Calorimeters Chapter 21 Chapter 2 Interactions of Charged Particles - With Focus on Electrons and Positrons -
1 The Origin of Mass: - Inertial Mass - München 2009 by Albrecht Giese, Hamburg The Origin of Mass 1.
Multiple Parton Interaction Studies at DØ Multiple Parton Interaction Studies at DØ Don Lincoln Fermilab on behalf of the DØ Collaboration Don Lincoln.
Neutral Current Deep Inelastic Scattering in ZEUS The HERA collider NC Deep Inelastic Scattering at HERA The ZEUS detector Neutral current cross section.
Measuring the charged pion polarizability in the  →    −  reaction David Lawrence, JLab Rory Miskimen, UMass, Amherst Elton Smith, JLab.
Introduction to CERN Activities
1 EPS2003, Aachen Nikos Varelas ELECTROWEAK & HIGGS PHYSICS AT DØ Nikos Varelas University of Illinois at Chicago for the DØ Collaboration
Electroweak Symmetry Breaking without Higgs Bosons in ATLAS Ryuichi Takashima Kyoto University of Education For the ATLAS Collaboration.
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.
Introduction to Particle Physics I Sinéad Farrington 18 th February 2015.
The Higgs Boson Beate Heinemann, University of Liverpool  The Standard Model and Beyond  Tevatron and LHC  Tevatron Results on Higgs Searches  Future.
1 FK7003 Lecture 17 – Interactions in Matter ● Electromagnetic interactions in material ● Hadronic interactions in material ● Electromagnetic and hadronic.
High energy photon LHC Krzysztof Piotrzkowski Université Catholique de Louvain LHC as a high energy  and  p collider Tagging photoproduction.
Beate Heinemann University of Liverpool For the CDF collaboration EPS 2003, Aachen, Physics Beyond the Standard Model with Photonic Final.
Backup slides Z 0 Z 0 production Once  s > 2M Z ~ GeV ÞPair production of Z 0 Z 0 via t-channel electron exchange. e+e+ e-e- e Z0Z0 Z0Z0 Other.
Higgs in the Large Hadron Collider Joe Mitchell Advisor: Dr. Chung Kao.
Derek F. Jackson Kimball. Collaboration Dmitry Budker, Arne Wickenbrock, John Blanchard, Samer Afach, Nathan Leefer, Lykourgas Bougas, Dionysis Antypas.
DIS 2003, May 22-27, St PetersburgAndrew Mehta Electroweak Physics and Searches1 Electroweak Physics + Searches Andrew Mehta DIS 2003, St. Petersburg,
Sfermion Flavor and Proton Decay in Minimal SU(5) GUT with High-scale SUSY Natsumi Nagata 26 June, 2014 PASCOS 2014 Warsaw, Poland Based on N. Nagata and.
Search for Heavy Stable Search for Heavy Stable Particles in CMS Particles in CMS Albert De Roeck CERN, Geneva, Switzerland Antwerp University Belgium.
Lecture 18 - Detectors Detector systems
ATLAS measurement of light-by-light scattering provides
Monopoles The Mystery.
Physics Overview Yasuhiro Okada (KEK)
Searching for Magnetic Monopoles
Minoru Nagai (ICRR, Univ. of Tokyo)
Physics Overview Yasuhiro Okada (KEK)
Physics Overview Yasuhiro Okada (KEK)
SUSY SEARCHES WITH ATLAS
Presentation transcript:

A Direct Search for Magnetic Monopoles at H1 HEP03, Aachen, 17-23/7/03 David Milstead The University of Liverpool

Monopoles in Particle Physics ‘t hooft/Polyakov – Monopole from breaking of simple symmetry group into U(1) SUSY GUTs: GeV Little Higgs: 1-5 TeV ? Electric charge quantisation Dirac - e=nh/g   Gauge group symmetry breaking

First search in ep at =300 GeV Sensitive to 150 GeV mass QED coupling for Dirac Monopole g D  g =g D 2 /4  34  em =1/137 Monopoles at HERA p s Processes predicted but not rate 10 3 greater ionisation energy loss rate than mip m m e e’ gg  em gg

Monopoles of strength > 0.75 g D stopped Bind to Al nucleus dipole moment and only released by melting (Milton et al.) Take 60cm section of 2mm thick H1 beam-pipe around interaction zone. Used : lumi=60pb -1 Cut into 14 strips and pass through superconducting loops and measure current. Monopoles in the H1 beam pipe

Southampton SQUID DC SQUID (2G mod. 581) at Southampton Oceanography Centre, UK. Sample sizes up to 1m long and 5cm radius. Measures changes in magnetic field T.

90g D 10g D 1.2g D Induced current x x position /cm Calibration Signature of monopole is persistent current Use solenoids with varying currents to mimick step solenoidsc loop i B

Signal survival Monopole signal survives after strip traversal strip Solenoid ( = 1 g d ) i

Beam pipe measurements Induced current from strips No candidates found Dirac Monopole Strip number Current

Monopole Acceptance Rising acceptance with high charge and low mass Use  mm (comphep) model

Cross-section upper limits First upper limits in ep collisions

Upper limit for Dirac Monopole Production Different experimental techniques Competitive ep limit

Upper limit for 3g d monopoles Only limits from ep and pp

First search in electron-proton scattering at =300 GeV at the H1 experiment Search for monopoles stopped in the beam pipe. Monopole masses up to 150 GeV and charges 1 < g D < 6 excluded. Magnetic monopoles play fundamental role in modern physics theories. Summary and Outlook s