July 28, 2004Tim Bolton NUFACT 2004-- OSAKA 1 Reactor  13 in the USA Will discuss  Physics case for a “medium” sin 2 2  13 ≤0.01 reactor experiment.

Slides:



Advertisements
Similar presentations
Results from Daya Bay Xin Qian On behalf of Daya Bay Collaboration Xin Qian, BNL1.
Advertisements

Controlling Systematics in a Future Reactor  13 Experiment Jonathan Link Columbia University Workshop on Future Low-Energy Neutrino Experiments April.
Heeger theta13, May A Neutrino Project at Diablo Canyon.
Stokstad, Heeger NSD, May 1, 2003 Reactor Neutrino Measurement of  13 Measuring the Last Undetermined Neutrino Mixing Angle  13 Searching for Subdominant.
6/6/2003Jonathan Link, Columbia U. NuFact03 Future Measurement of sin 2 2  13 at Nuclear Reactors Jonathan Link Columbia University June 6, 2003 ′03.
Summary of Nufact-03 Alain Blondel NuFact 03 5th International Workshop on Neutrino Factories & Superbeams Columbia University, New York 5-11 June 2003.
15 March 2004Cal Poly Meeting Status of Midwest  13 Effort Status of Braidwood site General strategy and layout of experiment Civil construction estimate.
Cosmic Induced Backgrounds D. Reyna Argonne National Lab.
Daya Bay Neutrino Experiment
21 March 2004 Overview of Braidwood Reactor Experiment Introduction to Braidwood site General strategy and layout of experiment Underground construction.
Braidwood Status Report Jonathan Link Columbia University APS Study, Reactor Working Group February 7&8, 2004.
Reactor Working Group Report
Summary of Nufact-03 Alain Blondel NuFact 03 5th International Workshop on Neutrino Factories & Superbeams Columbia University, New York 5-11 June 2003.
12 December 2003APS Neutrino StudyE. Blucher APS Neutrino Study: Reactor Working Group What can we learn from reactor experiments? Future reactor experiments.
Measuring  13 with Reactors Stuart Freedman University of California at Berkeley SLAC Seminar September 29, 2003.
1 The Daya Bay Reactor Electron Anti-neutrino Oscillation Experiment Jianglai Liu (for the Daya Bay Collaboration) California Institute of Technology APS.
Fermilab Neutrino Beamline to DUSEL Mike Martens Fermilab PAC November 3, 2009.
Jun Cao Institute of High Energy Physics, Beijing Daya Bay Neutrino Experiment 3rd International Conference on Flavor Physics, Oct. 3-8, 2005 National.
Daya Bay Reactor Neutrino Experiment Jun Cao On behalf of the Daya Bay Collaboration Institute of High Energy Physics XIII International.
Caren Hagner CSTS Saclay Present And Near Future of θ 13 & CPV in Neutrino Experiments Caren Hagner Universität Hamburg Neutrino Mixing and.
Eun-Ju Jeon Sejong Univ. Sept. 09, 2010 Status of RENO Experiment Neutrino Oscillation Workshop (NOW 2010) September 4-11, 2010, Otranto, Lecce, Italy.
Measuring sin 2 2  13 at the Daya Bay Reactor Neutrino Experiment Christopher Mauger (for the Daya Bay Collaboration) W. K. Kellogg Radiation Laboratory.
The Earth Matter Effect in the T2KK Experiment Ken-ichi Senda Grad. Univ. for Adv. Studies.
Physics with a very long neutrino factory baseline IDS Meeting CERN March 30, 2007 Walter Winter Universität Würzburg.
1 17 November 2005BNL HEP Seminar The Braidwood Neutrino Experiment Outstanding questions in neutrino oscillation physics: importance of  13 Experimental.
Long Baseline Experiments at Fermilab Maury Goodman.
A detector design for the Daya Bay reactor neutrino experiment Yifang Wang Institute of High Energy Physics, Beijing Jan. 18, 2004.
Using Reactor Anti-Neutrinos to Measure sin 2 2θ 13 Jonathan Link Columbia University Fermilab Long Range Planning Committee, Neutrino Session November.
1 Antineutrino Detector of Dayabay Reactor Neutrino Experiment Yuekun Heng, IHEP, Beijing On Behalf of the DayaBay Collaboration.
Karsten M. Heeger US Reactor  13 Meeting, March 15, 2004 Comparison of Reactor Sites and  13 Experiments Karsten Heeger LBNL.
Fermilab Neutrino Program Jim Strait Neutrino Discussion at CERN 26 November 2013.
νeνe νeνe νeνe νeνe νeνe νeνe Distance (L/E) Probability ν e 1.0 ~1800 meters 3 MeV) Reactor Oscillation Experiment Basics Unoscillated flux observed.
Karsten Heeger, Univ. of WisconsinDNP2006, Nashville, October 28, 2006 A High-Precision Measurement of sin 2 2  13 with the Daya Bay Reactor Antineutrino.
The NOvA Experiment Ji Liu On behalf of the NOvA collaboration College of William and Mary APS April Meeting April 1, 2012.
Measuring sin 2 2  13 with the Daya Bay nuclear power reactors Yifang Wang Institute of High Energy Physics.
Kr2Det: TWO - DETECTOR REACTOR NEUTRINO OSCILLATION EXPERIMENT AT KRASNOYARSK UNDERGROUND SITE L. Mikaelyan for KURCHATOV INSTITUTE NEUTRINO GROUP.
FJPPL Suekane1 Nu_2-WP2: R&D of detectors for future high statistics, high precision experiment (R&D for reactor anti-neutrino experiments) F.Suekane,
L. Oberauer, Paris, June 2004   Measurements at Reactors Neutrino 2004 CdF, Paris, June chasing the missing mixing angle.
Baseline Optimization Studies D. Reyna Argonne National Lab.
Karsten Heeger, LBNL TAUP03, September 7, 2003 Reactor Neutrino Measurement of  13 Karsten M. Heeger Lawrence Berkeley National Laboratory.
Results for the Neutrino Mixing Angle  13 from RENO International School of Nuclear Physics, 35 th Course Neutrino Physics: Present and Future, Erice/Sicily,
Degeneracy and strategies of LBL Osamu Yasuda Tokyo Metropolitan University NuFACT04 workshop July 28, 2004 at Osaka Univ.
,,,,, The Daya Bay Reactor Neutrino Experiment Liangjian Wen On behalf of the Daya Bay Collaboration Institute of High Energy Physics Daya Bay Detectors.
Results from RENO Soo-Bong Kim (KNRC, Seoul National University) “17 th Lomosonov Conference on Elementary Particle Physics” Moscow. Russia, Aug ,
The Daya Bay Reactor Neutrino Experiment R. D. McKeown Caltech On Behalf of the Daya Bay Collaboration CIPANP 2009.
Chasing  13 with new experiments at nuclear reactors Thierry Lasserre Saclay NuFact04, Osaka July
Optimizing the green-field beta beam NuFact 08 Valencia, Spain June 30-July 5, 2008 Walter Winter Universität Würzburg.
Karsten Heeger Beijing, January 18, 2003 Design Considerations for a  13 Reactor Neutrino Experiment with Multiple Detectors Karsten M. Heeger Lawrence.
Daya Bay Reactor Neutrino Experiment On behalf of the DayaBay collaboration Virginia Polytechnic Institute and State University Joseph ykHor YuenKeung,
Measuring  13 with Reactors Stuart Freedman HEPAP July 24, 2003 Bethesda Reactor Detector 1Detector 2 d2d2 d1d1.
6 January 2004EFI Faculty Lunch Future Neutrino Oscillation Experiments Neutrino oscillations, CP violation, and importance of  13 Accelerator vs. reactor.
Θ 13 and CP-Violation in the Lepton Sector SEESAW25 Institut Henri Poincaré, Paris Caren Hagner Universität Hamburg SEESAW25 Institut Henri Poincaré, Paris.
  Measurement with Double Chooz IDM chasing the missing mixing angle e  x.
Karsten Heeger, Univ. of Wisconsin Yale University, March 1, 2010  13 from Global Fits current best limit sin 2 2θ 13 < CL Fogli, et al., arXiv:0905:3549.
More material for P5 Milind Diwan for the Homestake neutrino detector group 3/1/2008.
1 Daya Bay Reactor Neutrino Oscillation Experiment Jen-Chieh Peng International Workshop on “Double Beta Decay and Neutrinos” Osaka, Japan, June 11-13,
NWG Presentation Heeger, Freedman, Kadel, Luk LBNL, April 11, 2003 Reactor Neutrino Measurement of  13 Searching for Subdominant Oscillations in e  ,
Results on  13 Neutrino Oscillations from Reactor Experiments Soo-Bong Kim (KNRC, Seoul National University) “INPC 2013, Firenze, June 2-7, 2013”
Braidwood Engineering/R&D Proposal
Experimental Hall in Mountain Regions
NEUTRINO OSCILLATION MEASUREMENTS WITH REACTORS
Baseline Design for Braidwood
Marco Oriunno (SLAC), March 12, 2014 MDI WG
Braidwood Prototype Test
$150K Chicago/ANL seed funding for Braidwood site investigation
A reactor experiment to measure 13
Simulation for DayaBay Detectors
The Braidwood Reactor Neutrino Experiment
Daya Bay Neutrino Experiment
Daya Bay Neutrino Experiment
Presentation transcript:

July 28, 2004Tim Bolton NUFACT OSAKA 1 Reactor  13 in the USA Will discuss  Physics case for a “medium” sin 2 2  13 ≤0.01 reactor experiment.  Status of “Midwest”  13 project at Braidwood, Illinois. Will not discuss  Highly advanced, but regrettably suspended Diablo Canyon project.  American involvement in Double-Chooz, Daya Bay, KASKA, and other international efforts beyond US borders.  US political situation, reactor or otherwise.

July 28, 2004Tim Bolton NUFACT OSAKA 2 Physics Case for sin 2 2  13 ≤0.01 Reactor-only:  Uniquely clean and precise measurement of  13.  Medium Braidwood style experiment exploits both rate and shape. Reactor+T2K/No a (M. Shaevitz)  Medium experiment resolves (45±  23 )° degeneracy for  23.  Small D-Chooz type experiment may leave ambiguity. But for T2K/No a with + running:  Minimal impact on mass hierarchy from reactors.  Modest impact on CP violation from reactors.  Caveat: A D-Chooz null result would make this physics tough for everybody. Huber et al. hep-ph/

July 28, 2004Tim Bolton NUFACT OSAKA 3 M. Shaevitz Study:  sin 2 2  13 (true)=0  sin 2 2  13 (true)=0.05 Reactors get  13 !

July 28, 2004Tim Bolton NUFACT OSAKA 4  deg. reflection degeneracy 1.5%  sin 2 2  23  Medium Braidwood-like reactor + / off-axis resolves ambiguity.  Result holds even without high precision  23.  D-Chooz may leave degenerate solutions, even with precise  23.

July 28, 2004Tim Bolton NUFACT OSAKA 5 Precision MeV Physics  Robust observable, first order flux cancellation.  Addresses “NuTeV anomaly” at NuTeV precision.  Interesting EW tests (ST plane) at Q 2 =0.  Challenging singles measurement, needs: Depth to suppress  spallation. Borexino-level radioactivity. Use of low background energy window. ≤ 1% systematics (calibrations).

July 28, 2004Tim Bolton NUFACT OSAKA 6 Braidwood Experiment Details  People.  Location.  Layout.  Detectors.  R&D.  Schedule.

July 28, 2004Tim Bolton NUFACT OSAKA 7  ANL: M. Goodman, V. Guarino, D. Reyna  Chicago: E. Abouzaid, K. Anderson, E. Blucher, J. Pilcher, M. Worcester  Columbia: J. Conrad, J. Link, M. Shaevitz  FNAL: L. Bartoszek, D. Finley, H. Jostlein, C. Laughton, R. Stefanski  Kansas State: T. Bolton, J. Foster, G. Horton-Smith, D. Onoprienko, N. Stanton  Michigan: B. Roe  Oxford: S. Biller, N. Jelley  Pittsburgh: D. Naples, V. Paolone  Texas: J. Klein Midwest  13 Collaboration

July 28, 2004Tim Bolton NUFACT OSAKA 8 Location  <50 km from two US national labs: Fermilab + Argonne National Lab.  ANL has ~50 years of reactor expertise.

July 28, 2004Tim Bolton NUFACT OSAKA 9 Reactor Complex But:  Cost risk associated with “green field” site.  Reactor managment presently encouraging, but tough decisions lie ahead.

July 28, 2004Tim Bolton NUFACT OSAKA 10 Basic Scheme  One near detector at ~270m; at least two far detectors at ~1700m.  Near and far detectors at 450 mwe depth (if bore hole samples confirm).  Identical 6.5m diameter 3-zone (a la D-Chooz) spheres.  Gd-loaded LS fiducial in ton range, depending on buffer optimization.  LS  -catcher + non-scintillating buffer.  Passive and active external shielding.  Detectors fully constructed at surface sites.  Detectors lowered down shafts (a la KASKA).  Detectors movable via surface transport for cross calibration.

July 28, 2004Tim Bolton NUFACT OSAKA 11 Layout Schematic Note: reactor management has agreed to shorten near access tunnel length from 300m to 50m ($$$!).

July 28, 2004Tim Bolton NUFACT OSAKA 12 Aerial View

July 28, 2004Tim Bolton NUFACT OSAKA 13 Mechanical Conceptual Design  Lifting points allow full assembly at surface.  Permits far detectors to move to near site for cross calibration.

July 28, 2004Tim Bolton NUFACT OSAKA 14 “Hoist and Roll” Scheme  “Common” procedure in industry.  Considerably cheaper than tunneling.  Favorable terrain at Braidwood site using truck on gravel road or rails, depending on load stresses.  Clearly requires careful design/implementation studies (underway). Left: 750 ton test lift by crawler crane. Right: 200 ton drilling equipment on gantry + self-propelled platform trailer. (ALE Lastra).

July 28, 2004Tim Bolton NUFACT OSAKA 15 Hall Layout

July 28, 2004Tim Bolton NUFACT OSAKA 16

July 28, 2004Tim Bolton NUFACT OSAKA 17 Acrylic Sphere Support  Multiple <2.5 cm dia. Spacers.  Assumes simultaneous filling for neutral buoyancy.  Ongoing work at ANL, U. Chicago.

July 28, 2004Tim Bolton NUFACT OSAKA 18 Software  Parametric and full G4 hit-level simulations (D. Onoprienko).  Good agreement with Chooz measurements (after some pain).  Optimizing geometry (R FID vs. R  -C vs. R BUF ).

July 28, 2004Tim Bolton NUFACT OSAKA 19 Cost/Schedule  Detailed estimate prepared for underground construction at Braidwood site prepared by independent consultants (Hilton and Associates, Inc.).  Included civil construction; outfitting with pumps; elevators, ventilation, etc.; and decommissioning costs at experiment end.  Permanent surface structures, detectors not yet included.  Detail level sufficient for re-scaling to optimized layouts. First iteration: two 300 mwe shafts, different detector hall designs, 300m tunnel for near site access: $35M cost, 39 month construction schedule. Revised layout: considerably shortened near access tunnel, 450 mwe depth (160m rock+20m soil). Cost in $25-35M range, <24 month construction schedule.  Detector cost (from MiniBoone scaling) ~ $8M/detector.

July 28, 2004Tim Bolton NUFACT OSAKA 20 Summary  Compelling physics case for a sin 2 2  13 ≤0.01 experiment. Medium scale reactor best short-term choice. Importantly extends Double-Chooz capabilities (provide ~3×better sin 2 2  13 sensitivity; with LBL, resolve  degree reflection degeneracy; open new field of precision MeV physics.)  Braidwood site an attractive choice: High power modern reactor complex with cooperative management. Simple layout with deep near site and possibility of movable detectors. Access to national lab infrastructure.  Current status: Active lab + university-based R&D. Bore hole study at Braidwood soon that follows up detailed costing studies. Preparing R&D proposal this Fall towards full proposal in 2005.