The MINOS Experiment Andy Blake Cambridge University.

Slides:



Advertisements
Similar presentations
New Frontiers in Physics Richard Lasky – Summer 2010.
Advertisements

Trigger issues for KM3NeT the large scale underwater neutrino telescope the project objectives design aspects from the KM3NeT TDR trigger issues outlook.
MINOS sensitivity to dm2 and sin2 as a function of pots. MINOS sensitivity to theta13 as a function of pots Precision Neutrino Oscillation Physics with.
Neutrino emission =0.27 MeV E=0.39,0.86 MeV =6.74 MeV ppI loss: ~2% ppII loss: 4% note: /Q= 0.27/26.73 = 1% ppIII loss: 28% Total loss: 2.3%
1 Deep Sea Neutrino Telescope Detection Principle.
Search for spontaneous muon emission from lead nuclei with OPERA bricks M. Giorgini, V. Popa Bologna Group OPERA Collaboration Meeting, LNGS, 19-22/05/2003.
How to Build a Neutrino Oscillations Detector - Why MINOS is like it is! Alfons Weber March 2005.
An accelerator beam of muon neutrinos is manufactured at the Fermi Laboratory in Illinois, USA. The neutrino beam spectrum is sampled by two detectors:
Neutrino Physics Pedro Ochoa May 15th 2006.
Searching for Atmospheric Neutrino Oscillations at MINOS Andy Blake Cambridge University April 2004.
First Observations of Separated Atmospheric  and  Events in the MINOS Detector. A. S. T. Blake* (for the MINOS collaboration) *Cavendish Laboratory,
Neutrinos: Detecting the Invisible!
Atmospheric Neutrino Anomaly
The neutrons detection involves the use of gadolinium which has the largest thermal neutron capture cross section ever observed. The neutron capture on.
NuMI MINOS The MINOS Far Detector Cosmic Rays and their neutrinos are being collected now. How does this work, and of what use is this data? Alec Habig,
P461 - particles VIII1 Neutrino Physics Three “active” neutrino flavors (from Z width measurements). Mass limit from beta decay Probably have non-zero.
10/24/2005Zelimir Djurcic-PANIC05-Santa Fe Zelimir Djurcic Physics Department Columbia University Backgrounds in Backgrounds in neutrino appearance signal.
New results from K2K Makoto Yoshida (IPNS, KEK) for the K2K collaboration NuFACT02, July 4, 2002 London, UK.
July 19, 2003 HEP03, Aachen P. Shanahan MINOS Collaboration 1 STATUS of the MINOS Experiment Argonne Athens Brookhaven Caltech Cambridge Campinas Dubna.
A long baseline neutrino oscillation search - MINOS Reinhard Schwienhorst School of Physics and Astronomy University of Minnesota.
Atmospheric Neutrino Oscillations in Soudan 2
NEW RESULTS FROM MINOS Patricia Vahle, for the MINOS collaboration College of William and Mary.
Making a neutrino beam The neutrinos detected in the MINOS experiment are produced in the Neutrinos at the Main Injector (NuMI) beam line at Fermi National.
My Chapter 30 Lecture.
NuMI NuMI Overview NBI 2002 S. Childress (FNAL) 14 March ‘02 NuMI / MINOS Overview.
Chapters 9, 11, 12 Concepts covered that will also be candidates for exam questions.
The Elementary Particles. e−e− e−e− γγ u u γ d d The Basic Interactions of Particles g u, d W+W+ u d Z0Z0 ν ν Z0Z0 e−e− e−e− Z0Z0 e−e− νeνe W+W+ Electromagnetic.
Particle Production in the MICE Beam Line Particle Accelerator Conference, May 2009, Vancouver, Canada Particle Production in the MICE Beam Line Jean-Sebastien.
Latest Results from The MINOS Experiment
2 Atmospheric Neutrinos Atmospheric neutrino detector at Kolar Gold Field –1965.
Monday, Feb. 24, 2003PHYS 5326, Spring 2003 Jae Yu 1 PHYS 5326 – Lecture #11 Monday, Feb. 24, 2003 Dr. Jae Yu 1.Brief Review of sin 2  W measurement 2.Neutrino.
Long Baseline Experiments at Fermilab Maury Goodman.
Wednesday, Feb. 14, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #6 Wednesday, Feb. 14, 2007 Dr. Jae Yu 1.Neutrino Oscillation Formalism 2.Neutrino.
Neutrino Oscillations in vacuum Student Seminar on Subatomic Physics Fundamentals of Neutrino Physics Dennis Visser
Muon Identification in the MINOS Calibration Detector Anna Holin 05 December 2005 University College London.
Monday, Feb. 19, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #7 Monday, Feb. 19, 2007 Dr. Jae Yu 1.Neutrino Oscillation Experiments 2.Long.
Latest Results from the MINOS Experiment Justin Evans, University College London for the MINOS Collaboration NOW th September 2008.
Application of neutrino spectrometry
MINERvA Main INjector ExpeRiment for -A is the symbol for the neutrino. The beam that is sent to MINERvA is made out of neutrinos. In chemistry, an A stands.
Detector Monte-Carlo ● Goal: Develop software tools to: – Model detector performance – Study background issues – Calculate event rates – Determine feasibility.
Mass Hierarchy Study with MINOS Far Detector Atmospheric Neutrinos Xinjie Qiu 1, Andy Blake 2, Luke A. Corwin 3, Alec Habig 4, Stuart Mufso 3, Stan Wojcicki.
OPERA Neutrino Experiment Tija Sīle presentation is based on: Doktorantūras skolas “Atomāro un nepārtrauktās vides fizikālo.
PHY418 Particle Astrophysics
Calibration of the MINOS Detectors Using Stopping Muons Jeff Hartnell University of Oxford & Rutherford Appleton Laboratory IoP Particle Physics 2004 Tuesday.
Michel Gonin – Ecole Polytechnique – France : SUPER NOVA SN1987A Super-Kamiokande Introduction neutrino oscillations mixing matrices Introduction.
E. W. Grashorn and A. Habig, UMD, for the MINOS Collaboration The Detectors of The Main Injector Neutrino Oscillation Search (MINOS) Experiment The MINOS.
Harvard Neutrino Group DoE Review August 21, 2006.
March 3, 2009Tom Gaisser1 Neutrino oscillations Review of particle physics, neutrino interactions and neutrino oscillations.
Accelerator-based Long-Baseline Neutrino Oscillation Experiments Kam-Biu Luk University of California, Berkeley and Lawrence Berkeley National Laboratory.
Low Z Detector Simulations
Atmospheric Neutrinos Phenomenology and Detection p 00 ++  e+e+ e-e- ++  Michelangelo D’Agostino Physics C228 October 18, 2004.
Measurement of the neutrino velocity with the MINOS detectors and NuMI neutrino beam GdR Saclay – 11/04/08 Magali Besnier hep-ex – v3.
Search for active neutrino disappearance using neutral-current interactions in the MINOS long-baseline experiment 2008/07/31 Tomonori Kusano Tohoku University.
1 Experimental Particle Physics PHYS6011 Fergus Wilson, RAL 1.Introduction & Accelerators 2.Particle Interactions and Detectors (2) 3.Collider Experiments.
Monday, Mar. 3, 2003PHYS 5326, Spring 2003 Jae Yu 1 PHYS 5326 – Lecture #12 Monday, Mar. 3, 2003 Dr. Jae Yu 1.Neutrino Oscillation Measurements 1.Atmospheric.
NUMI NUMI/MINOS Status J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting.
Neutrino. Game Board FERMILABHAPPENINGSFIRSTSNEUTRINOSDETECTION.
The Latest MINOS Results Xinjie Qiu Stanford University (for the MINOS Collaboration) International Symposium on Neutrino Physics and Beyond Sept
 Alpha and gamma have very specific energies  Beta have a continuous distribution of energy  Must be some other particle taking away some of the.
E. W. Grashorn, for the MINOS Collaboration Observation of Shadowing in the Underground Muon Flux in MINOS This poster was supported directly by the U.S.
Ff Neutrino Time of Flight measurements (with MINOS) Phil Adamson 12 th September 2012.
New Results from MINOS Matthew Strait University of Minnesota for the MINOS collaboration Phenomenology 2010 Symposium 11 May 2010.
Neutral Current Interactions in MINOS Alexandre Sousa, University of Oxford for the MINOS Collaboration Neutrino Events in MINOS Neutrino interactions.
Neutrino factory near detector simulation
J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting
Chris Smith California Institute of Technology EPS Conference 2003
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 6th May 2009 Fergus Wilson, RAL.
6. Preliminary Results from MINOS
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 28th April 2008 Fergus Wilson. RAL.
Experimental Particle Physics PHYS6011 Joel Goldstein, RAL
Presentation transcript:

The MINOS Experiment Andy Blake Cambridge University

Neutrinos are the most abundant particles in the universe … … but the most difficult to detect ! Three flavours – electron, muon, tau Weakly interacting (absorbed by ~10 light years Pb) Extremely small mass (< kg)

Neutrino Oscillations Quantum mechanical phenomenon – the weak eigenstates can be a mixture of the free eigenstates If neutrinos really mix and have mass, flavour oscillations occur during flight. The oscillation probability is given by: (L = distance travelled, E = energy,  M 2 = mass difference squared)

One example - Atmospheric Neutrinos Produced from interactions of cosmic rays with the atmosphere. Expect ~ isotropic  and e  and e measured by Japanese Super-Kamiokande experiment (50kT water cerenkov detector) Found deficit in upward-going  but upward-going  travel longer distance to detector so  -  oscillations may be taking place.

M ain I njector N eutrino O scillation S earch Soudan Underground Laboratory Fermi National Accelerator Laboratory Produce  beam at Fermilab (nr. Chicago). Measure beam in two detectors: (1) 1 km away (1kT near detector at Fermilab, IL) (2) 730km away (5kT far detector at Soudan, MN) Compare measurements and look for oscillations. Beam scheduled to switch on early 2005.

Wilson Hall for Scale Target Hall Near Detector Hall Absorber Hall Proton carrier Decay volume Muon Monitors How do you make a neutrino beam … ? Fire ~ protons per second at ~ 50g graphite target. Select pions from the resultant spray of secondary particles. Focus pions into tight beam. Let pions decay inside 600m evacuated pipe to produce muons and neutrinos. At end of pipe, absorb muons in rock, leaving just neutrinos! Just have to aim beam pipe at your detectors!

How do you detect a neutrino beam … ? 5.4 kT calorimeter (8m x 8m x 30m). 485 inch-thick planes of steel. ~ 1T magnetic field. 93,000 strips of plastic scintillator. Muon neutrinos interact inside detector to produce muons, which leave trails of ionization and induce photon emissions in scintillator. Photons detected by 1450 PMTs. Signal amplified and digitized by sensitive electronics. Signature of neutrino interaction: (1) muon track with contained vertex (2) timing + direction consistent with neutrino beam from Fermilab Expect to detect ~10 3 of ~10 13 neutrinos that pass through far detector each year. The Soudan Detector

How do you measure neutrino oscillations … ? Measure  energy spectrum at near and far detector. Use near spectrum to predict far spectrum for no oscillations. Look for oscillation dip in ratio of far spectrum to far prediction.

Cambridge Involvement in MINOS Far detector neutrino event Monte Carlo neutrino event my first atmospheric neutrino ! Currently 3 staff + 2 graduate students + 1 postdoc. Significant software commitments (1) DAQ control software (2) Monte Carlo simulation (3) Data reconstruction + analysis Analysis of atmospheric neutrinos. Analysis of beam neutrinos. Oscillation analysis

New Physics … ? The eleventh commandment - “thou shalt not violate CPT in your theories”. CPT symmetry requires that and have identical properties. Separate measurements of  and  oscillations possible at MINOS. _ _ An alternative view … Alternative mass hierarchy for neutrinos and anti-neutrinos …

Summary Over the last 5 years, our understanding of neutrino physics has increased hugely. Over the next 5 years, a new generation of neutrino experiments will make precise measurements. MINOS will be a major part of this experimental effort. Cambridge will continue to make significant contributions.