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,

Slides:



Advertisements
Similar presentations
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.
Advertisements

NLC – The Next Linear Collider Project Colorado Univ. - Boulder Calorimetry Cornell-ALCPG Calorimetry Detector Study Plans at Colorado Uriel Nauenberg.
COSMIC RAY MUON DETECTION USING SCINTILLATION COUNTER AND WAVELENGTH SHIFTING FIBERS ARUNODAYA BHATTACHARYA VSRP-2009,TIFR,MUMBAI 6/7/09.
The Angra Neutrino Detector Detector, VETO and electronics conceptual design Laudo Barbosa (May 18th, 2006) Centro Brasileiro de Pesquisas Físicas (CBPF)
Status of the MICE SciFi Simulation Edward McKigney Imperial College London.
Off-axis Simulations Peter Litchfield, Minnesota  What has been simulated?  Will the experiment work?  Can we choose a technology based on simulations?
How to Build a Neutrino Oscillations Detector - Why MINOS is like it is! Alfons Weber March 2005.
Far Detector Data Quality Andy Blake Cambridge University.
An accelerator beam of muon neutrinos is manufactured at the Fermi Laboratory in Illinois, USA. The neutrino beam spectrum is sampled by two detectors:
Searching for Atmospheric Neutrino Oscillations at MINOS Andy Blake Cambridge University April 2004.
Directional Detectors and Digital Calorimeters Ed Norbeck and Yasar Onel University of Iowa For the 25 th Winter Workshop on Nuclear Dynamics Big Sky,
First Observations of Separated Atmospheric  and  Events in the MINOS Detector. A. S. T. Blake* (for the MINOS collaboration) *Cavendish Laboratory,
The MINOS Experiment Andy Blake Cambridge University.
Y. Karadzhov MICE Video Conference Thu April 9 Slide 1 Absolute Time Calibration Method General description of the TOF DAQ setup For the TOF Data Acquisition.
The Design of MINER  A Howard Budd University of Rochester August, 2004.
S K The Many Uses of Upward- going Muons in Super-K Muons traveling up into Super-K from high-energy  reactions in the rock below provide a high-energy.
NLC – The Next Linear Collider Project Colorado Univ. – Boulder, Jan., 2004 LCD-ALCPG Presentation at the ALCPG-SLAC Meeting Progress Report of Work at.
The Time-of-Flight system of the PAMELA experiment: in-flight performances. Rita Carbone INFN and University of Napoli RICAP ’07, Rome,
July 19, 2003 HEP03, Aachen P. Shanahan MINOS Collaboration 1 STATUS of the MINOS Experiment Argonne Athens Brookhaven Caltech Cambridge Campinas Dubna.
The Transverse detector is made of an array of 256 scintillating fibers coupled to Avalanche PhotoDiodes (APD). The small size of the fibers (5X5mm) results.
NuMI Schematic View of the MINOS Scintillator System 8 m Scintillator Module WLS Fibers Optical Connector Clear Fiber Ribbon Cable (2-6 m) Multiplex Box.
Leroy Nicolas, HESS Calibration results, 28 th ICRC Tsukuba Japan, August Calibration results of the first two H·E·S·S· telescopes Nicolas Leroy.
Report of the NTPC Test Experiment in 2007Sep and Others Yohei Nakatsugawa.
PERFORMANCE OF THE MACRO LIMITED STREAMER TUBES IN DRIFT MODE FOR MEASUREMENTS OF MUON ENERGY - Use of the MACRO limited streamer tubes in drift mode -Use.
VC Feb 2010Slide 1 EMR Construction Status o General Design o Electronics o Cosmics test Jean-Sebastien Graulich, Geneva.
Status of the NO ν A Near Detector Prototype Timothy Kutnink Iowa State University For the NOvA Collaboration.
Scintillation hodoscope with SiPM readout for the CLAS detector S. Stepanyan (JLAB) IEEE conference, Dresden, October 21, 2008.
The Design and Performance of the MINER A Detector Howard Budd, University of Rochester Technology and Instrumentation in Particle Physics 2011.
March 12, 2006R. Abrams LCWS06 Bangalore1 ILC Prototype Muon Scintillation Counter Tests Robert Abrams Indiana University.
Long Baseline Experiments at Fermilab Maury Goodman.
21-Aug-06DoE Site Review / Harvard(1) Front End Electronics for the NOvA Neutrino Detector John Oliver Long baseline neutrino experiment Fermilab (Chicago)
Start Counter Collaboration Meeting September 2004 W. Boeglin FIU.
Muon Identification in the MINOS Calibration Detector Anna Holin 05 December 2005 University College London.
NESTOR SIMULATION TOOLS AND METHODS Antonis Leisos Hellenic Open University Vlvnt Workhop.
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.
The Status of MINOS Mike Kordosky University College London for the collaboration.
SL1Calo Input Signal-Handling Requirements Joint Calorimeter – L1 Trigger Workshop November 2008 Norman Gee.
08-June-2006 / Mayda M. VelascoCALOR Chicago1 Initial Calibration for the CMS Hadronic Calorimeter Barrel Mayda M. Velasco Northwestern University.
CEA DSM Irfu Reconstruction and analysis of ANTARES 5 line data Niccolò Cottini on behalf of the ANTARES Collaboration XX th Rencontres de Blois 21 / 05.
Detector Monte-Carlo ● Goal: Develop software tools to: – Model detector performance – Study background issues – Calculate event rates – Determine feasibility.
The Electromagnetic Calorimeter – 2005 Operation J. Sowinski for the Collaboration and the Builders Indiana Univ. Michigan State Univ. ANL MIT BNL Penn.
LM Feb SSD status and Plans for Year 5 Lilian Martin - SUBATECH STAR Collaboration Meeting BNL - February 2005.
Calibration of the MINOS Detectors Using Stopping Muons Jeff Hartnell University of Oxford & Rutherford Appleton Laboratory IoP Particle Physics 2004 Tuesday.
5-9 June 2006Erika Garutti - CALOR CALICE scintillator HCAL commissioning experience and test beam program Erika Garutti On behalf of the CALICE.
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.
MINER A Main INjector ExpeRiment for v-A Active segmented scintillator detector: 5.87 tons Nuclear targets of C, Fe and Pb, Water, Helium.
The Detector Performance Study for the Barrel Section of the ATLAS Semiconductor Tracker (SCT) with Cosmic Rays Yoshikazu Nagai (Univ. of Tsukuba) For.
PMT measurements in Antares Oleg Kalekin on behalf of Antares collaboration VLVnT 2011 Erlangen
LHCf Detectors Sampling Calorimeter W 44 r.l, 1.6λ I Scintilator x 16 Layers Position Detector Scifi x 4 (Arm#1) Scilicon Tracker x 4(Arm#2) Detector size.
Search for active neutrino disappearance using neutral-current interactions in the MINOS long-baseline experiment 2008/07/31 Tomonori Kusano Tohoku University.
NUMI NUMI/MINOS Status J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting.
MINER A at the Triple Point: Three Phases at once Deborah Harris AEM August 31, 2009.
A Brand new neutrino detector 「 SciBar 」 (2) Y. Takubo (Osaka) - Readout Electronics - Introduction Readout electronics Cosmic ray trigger modules Conclusion.
Status of the NOνA Experiment Satish Desai - University of Minnesota For the NOνA Collaboration APS Meeting - April 2013 Denver, Colorado.
The Latest MINOS Results Xinjie Qiu Stanford University (for the MINOS Collaboration) International Symposium on Neutrino Physics and Beyond Sept
The NO A Near Detector: An overview Jose A. Sepulveda-Quiroz For the NO A Collaboration Iowa State University and Argonne National Laboratory APS April.
Monitoring and Commissioning the NOνA Far Detector M. Baird 1, J. Bian 2, J. Coelho 4, G. Davies 3, M. Messier 1, M. Muether 5, J. Musser 1 and D. Rocco.
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.
 13 Readout Electronics A First Look 28-Jan-2004.
Results with the RPC system of OPERA and perspectives
Experimental Method: 2 independent detectors on both sides of IP
J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting
A First Look J. Pilcher 12-Mar-2004
Chris Smith California Institute of Technology EPS Conference 2003
Far Detector Performance and Calibration
BESIII EMC electronics
Experimental Method: 2 independent detectors on both sides of IP
Presentation transcript:

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, Univ. of Minnesota Duluth, for the MINOS collaboration

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 2 The MINOS Experiment Main Injector Neutrino Oscillation Search –Will utilize NuMI beam from Fermilab Front-to-back  oscillation study –Produce well-studied  beam –Measure  spectrum just after production with “Near Detector” –Measure again 735 km later with “Far Detector” Beam goes from Fermilab to the Soudan Mine Underground Lab 735 km

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 3 The Far Detector Steel/Scintillator sampling calorimeter –5.4 kt, 8m diameter, 31m long –486 layers, each made of: 1” steel 1 cm plastic scintillator –Magnetized to ~1.5 T Design goals – e /  /  discrimination –Good energy resolution For both  and showers –Good timing, both hit-to-hit and absolute For particle direction and synching with Fermilab beam ½ of the Far Detector To FermilabTo Fermilab 15m 8m

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 4 Far Detector Progress Construction began August 2001 Now up to about plane #225 –Almost halfway done! –First half complete in July when it will be magnetized Taking Cosmic Ray data as it is built –Each plane independently instrumented Plane #200, May 3, 2002

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 5 Particle Detection 4.1 cm x 8m scint strips bundled into “modules” –Light channeled out via 2- ended fiber Each plane’s strips are 90 o from the last –“U” and “V” views 17 GeV MC  shown below from side, in U,V From FNAL

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 6 Multiplexing Light detected by 16 pixel PMTs 8 fibers per pixel, ganged together with: –Maximal physical strip separation –Minimal in-PMT cross- talk M16 PMT 16 mm Fiber Layout One of 3 Ham. M16 PMTs in this “Mux Box”

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 7 Front End Electronics Fibers from each strip end are multiplexed onto PMT pixels Signals amplified, shaped, and tracked+held by “VA” chips –Calibration charge can also be injected in the same place as PMT charge for functionality check and calibration of full electronics path Timing information sent upstream from this “Front End” rack

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 8 Data Gathering VME “Master” crate –VA Readout Controllers “VARC”s Charge from PMTs digitized by 14-bit ADCs Time stamped to 1.6ns by internal clock –2/6 or 2/36 pre-trigger applied –Hits given absolute GPS time Data read out over PVIC bus to computer room –4/5 plane software trigger applied, hits time ordered –Data formatted in ROOT 1 of 16 VME crates Digitizes 72 mux boxes Each w/3 16-pixel PMTs

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 9 De-multiplexing Scintillator strip ends are multiplexed 8-1 per electronics channel How to figure out which strip a particle really went through? Matching hits on both ends of a strip helps in the simplest track case For multiple hits on a plane and showers: –All the different possible “hypotheses” of which strip was really hit tested against the possible real physics –Best fitting hypotheses saved Reconstructing close multiple muons very difficult!

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 10 A Cosmic Ray De-multiplexed Success rate for Cosmic Rays: –94% of hits correctly associated with their strips –97% of CR events successfully sorted out CR  before De-multiplexing CR  after De-multiplexing

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 11 Light Injection Calibration using controlled light: –LEDs illuminate 8-10 calibration fiber ends each –Fibers carry light from LED to shine on ends of scint strip fibers Varying light levels used to map out detector and phototube response Regular pulsing at a constant light level during normal operations –Tracks changing detector response –Flags problems with optical path Light from calibration fibers illuminating ends of fibers from the scintillator where they are bundled

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 12 Cosmic Rays CR-  light output with expectations ~10 pe at mid-strip (sum of both ends) As planes are added to the detector, they contribute to the data acquisition Currently taking Cosmic Ray data –CR rate: 1000  /strip/month, 2% stop in detector Excellent “beam” for detector commissioning –Real particle data provide end- to-end test of all hardware, software systems Good calibration source –Geometry, gain, timing, reconstruction software

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 13 CR Calibrations Physical plane locations are surveyed as the planes are raised –CR  draw nice straight lines –Residuals to the  fits are not bad with nominal plane geometry, excellent with survey-corrected data Timing calibrations –CR  are nice straight lines moving at  =1 –Use this physics to find and fit absolute timing offsets Need t0 fit plot Timing offsets (ns) vs. channel. Different delays in different electronics paths are clearly seen, as is the few (2.6) nanosecond resolution

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 14 Initial Searches Atmospheric are present in the data –Contained vertex search being refined –Up-going  search underway as part of CR timing calibrations Reconstruct timing of  tracks –Down-going CR’s have  =1 –Up-going -induced  have  =-1 An up-  !

NuMI MINOS Neutrino 2002, May 25-30, 2002, Munich Alec Habig Page 15 Summary First ! An up-going  seen on the evening of March 22, 2002 – MINOS works! The MINOS Far Detector construction is nearing the ½ way point Data being taken as the detector grows is used to validate and calibrate both hardware and software Will be ready for beam –Plus atmospheric work can be done with magnetic field! / separation The presenter gratefully acknowledges support for this poster from the National Science Foundation via its RUI grant #