1 / 13

The Nab Experiment

The Nab Experiment. 2012-10-26 Christopher Crawford DNP Fall Meeting, Newport Beach, CA University of Kentucky. Correlations in Neutron Decay. Parity violation implies a rich phenomenology in neutron decay.

atara
Download Presentation

The Nab Experiment

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. The Nab Experiment 2012-10-26 Christopher Crawford DNP Fall Meeting, Newport Beach, CA University of Kentucky

  2. Correlations in Neutron Decay Parity violation implies a rich phenomenology in neutron decay. V-A implies that all experimental quantities can be related to the axial and vector coupling constants gA and gV. • Neutron beta decay measurements give: • Test of CKM unitarity • Test of CVC / search for SCC • Test of tensor or scalar couplings Jackson et al., PR 106, 517 (1957) Goals: Nab: δa/a = 0.1%, δb = 0.1% abBA: δA/A = 0.1%, δB/B=0.1% DNP Fall Meeting, Newport Beach, CA

  3. Determination of Vud matrix element 0 . 9 8 0 Kaons +Unitarity [PDG 2010] 0 . 9 7 5 ft(0+→0+) [Hardy09] ft(0+→0+) [Liang09 – DD-ME2] PIBETA [Pocanic04] ft(0+→0+) [Liang09 – PKO1] Vud 0 . 9 7 0 τn [MAMBO II] τn [Serebrov05] λ [PDG 2010] 0 . 9 6 5 A [UCNA 2010] τn [PDG 2010] 0 . 9 6 0 - 1 . 2 9 0 - 1 . 2 8 0 - 1 . 2 7 0 - 1 . 2 6 0 λ= gA/gV courtesy S. Baessler A [PERKEO II, prel.] DNP Fall Meeting, Newport Beach, CA

  4. Sensitivity to scalar/tensor couplings Left-handed currents Right-handed currents Present limits (n decay data) SM: (0,0) Future limits, assuming a= -0.1059(1), A= -0.11860(3), B = 0.987(1), τn= 882.2(8) s G. Konrad, S.B. et al., ArXiv:1007.3027; courtesy S. Baessler DNP Fall Meeting, Newport Beach, CA

  5. Nab cos(θ) spectrometer Proton phase space (Dalitz plot) Probability (arb. units) 1.5 Ee = 1.25 700 keV cos θeν = 1 236 keV 1 0.75 75 keV pp2 [MeV2/c2] cos θeν = 0 0.5 cos θeν = -1 450 keV 0.25 0 0 0.2 0.4 0.6 0.8 courtesy S. Baessler DNP Fall Meeting, Newport Beach, CA Ee [MeV]

  6. Proton TOF measurement 30 kV Segmented Si detector Adiabatic conversion TOF region (field rB∙B0) magnetic filter region (field B0) decay volume (field rB,DV∙B0) 0 kV Neutron beam 0 kV • Magnetic filter and longitudinalization of proton momentum 5 Si detector 4 3 B (on axis) z 2 Decay Magnetic Field volume 1 0 2 5 -1 0 1 3 4 z [m] Proton Trajectory courtesy S. Baessler DNP Fall Meeting, Newport Beach, CA

  7. Detector response function Simulated counts [A.U.] Ee= 300 keV Ee = 500 keV Ee = 700 keV 0 0.002 0.004 0.006 1/tp2[µs-2] • TOF vs. pp assuming adiabatic proton spin transport • Edges confirm calibration • Slope of central part used to extract correlation ‘a’ courtesy S. Baessler DNP Fall Meeting, Newport Beach, CA

  8. Fierz interference term ‘b’ ) s t i n u . b r a ( 5 10 d l b = +0.1 e i 4 10 SM Y 3 10 d l e i 2 Y 10 1 10 0 2 0 0 4 0 0 6 0 0 8 0 0 1 E ( k e V ) e , k i n 0 50 100 150 200 250 300 detected Ee [keV] • From the shape of the electron energy spectrum • Systematic uncertainties • Electron energy resolution • background Detector response to decay electron with Ee = 300 keV 2% of events in tail (deadlayer, external bremsstrahlung) Goal: Δb ~ 3×10-3 courtesy S. Baessler DNP Fall Meeting, Newport Beach, CA

  9. Uncertainty Budget PLANNEDstatistical uncertainty budget: PLANNED systematic uncertainty budget: About 2×109 events can be detected in 6 weeks (Decay volume V = 246 cm3, decay density nd= 20 cm-3, 12.7 % of decay protons go to upper detector, 80% duty factor) → (Δa/a)stat < 1×10-3 can be reached Compare to Δa/a = 5 % of existing experimental results

  10. Nab Setup at the SNS • Fundamental Neutron Physics Beamline Si detectors Neutron beam Spectrometer magnet DNP Fall Meeting, Newport Beach, CA

  11. 6” ion-implanted silicon detectors • 2 mm thick, 127 pixels • 70-100 nm dead layer front fiducial volume proton, 32 keV 0.5 mm back background dark noisepedestal Dead-layer thickness measured at NCSU DNP Fall Meeting, Newport Beach, CA

  12. DAQ – Digital Signal Processing • Readout waveform (energy, time) • offline pulse shape analysis • Form e-p coincidences • 50 – 750 keV prompt electron • 30 keV proton 12 – 40 μs TOF • Energy and Timing Resolution • 2 keV electron (energy sum) • 10 ns proton TOF resolution • Resolve backscattered events • HV Optical Isolation • 30 kV potential between detectors • Event / Data rate • 5000/s electrons; 600/s protons • Accidentals <1% in 40 us window • 256 channels, 100 MHz, 12 bit ADC • 11 MB/s data rate -> 12 TB • Trigger levels • 1) DIGITIZER threshold, 2) FPGA readout, 3) CPU storage • Energy sum trigger, adjacent pixels • Read out 7 nearest neighbor pixels in each detector . digitizer FPGA main FGPA readout hits fiber optics trigger bus lines rear I/O module DNP Fall Meeting, Newport Beach, CA

  13. Nab Collaboration R. Alarcona, L.P. Alonzib, S. Baessler.b,c (Project Manager), S. Balascutaa, L. Barrón-Palos n, J.D. Bowmanc(Co-Spokesmen), M.A. Bychkovb, J. Byrned, J.R. Calarcoe, T.V. Ciancioloc, C. Crawfordf, E. Frležb, M.T. Gerickeg, F. Glückh, G.L. Greenec,i, R.K. Grzywaczi, V. Gudkovj, F.W. Hersmane, T. Itok, A. Kleink, M. Makelak, J. Martinl, S. McGovernb, S. Pageg, A. Palladinob, S.I. Penttiläc (On-site Manager), D. Počanićc (Co-Spokesmen), K.P. Rykaczewskic, A. Salas-Baccib, W.S. Wilburnk, A.Youngm a Department of Physics, Arizona State University, Tempe, AZ 85287-1504 b Department of Physics, University of Virginia, Charlottesville, VA 22904-4714 c Physics Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831 d Department of Physics and Astronomy, University of Sussex, Brighton BN19RH, UK e Department of Physics, University of New Hampshire, Durham, NH 03824 f Department of Physics and Astronomy, University of Kentucky, Lexington, KY 40506 g Department of Physics, University of Manitoba, Winnipeg, Manitoba, R3T 2N2, Canada h IEKP, Universität Karlsruhe (TH), Kaiserstraße 12, 76131 Karlsruhe, Germany iDepartment of Physics and Astronomy, University of Tennessee, Knoxville, TN 37996 j Department of Physics and Astronomy, University of South Carolina, Columbia, SC 29208 k Los AlamosNationalLaboratory, Los Alamos, NM 87545 l Department of Physics, University of Winnipeg, Winnipeg, Manitoba R3B2E9, Canada m Department of Physics, North Carolina State University, Raleigh, NC 27695-8202 n Universidad Nacional Autónoma de México, México, D.F. 04510, México DNP Fall Meeting, Newport Beach, CA

More Related