Beta Neutrino Correlation Measurement with Trapped Radioactive Ions

Slides:



Advertisements
Similar presentations
LRP2010 WG5 Fundamental Interactions Nathal Severijns ( K.U.Leuven) for WG5 Scoping workshop Frankfurt, October th 2009.
Advertisements

Grupo de Física Nuclear Experimental IEMIEM CSIC Curso de Doctorado Estructura Nuclear M.J.G. Borge, IEM, CSIC 8 Junio 2007 Estudio experimental de la.
Fast-Timing with LaBr 3 :Ce Detectors and the Half-life of the I π = 4 – Intruder State in 34 P (…and some other stuff maybe..) Paddy Regan University.
Tests of symmetries with nuclei (in nuclear b decay)
Structure of the ECEC candidate daughter 112 Cd P.E. Garrett University of Guelph TRIUMF Excellence Cluster “Universe”, Technische Universität München.
GEANT4 Simulations of TIGRESS
JYFLTRAP: Spectroscopy with multi-trap facility Facility Mass purified beams In-trap spectroscopy Future plans.
Present status of  -decay studies… …in nuclear mirror transitions Oscar Naviliat-Cuncic National Superconducting Cyclotron Laboratory and Department of.
High precision study of the  decay of 42 Ti  V ud matrix element and nuclear physics  Experimental and theoretical precisions  New cases: goals and.
Precision mass measurements for fundamental studies Tommi Eronen Max-Planck-Institut für Kernphysik Heidelberg, Germany.
Study of  - correlations with LPCTrap Dominique Durand LPC Caen, ENSICAEN, Université de Caen, CNRS/IN2P3, Caen, France On behalf of the LPCTrap collaboration.
Teresa Kurtukian-Nieto Centre d’Etudes Nucléaires de Bordeaux Gradignan Precision half-life determination of the superallowed 0 + → 0 + β + -emmiters 42.
Precision measurement of the half-life and branching ratio of the T=1/2 mirror β decay of 37 K T. Kurtukian-Nieto, P. Ascher, B. Blank, G. Canchel, M.
 asymmetry parameter measurements in nuclear  -decay as a probe for non-Standard Model physics K.U.Leuven, Univ. Bonn, NPI Rez (Prague), ISOLDE CERN.
Reaction rates in the Laboratory Example I: 14 N(p,  ) 15 O stable target  can be measured directly: slowest reaction in the CNO cycle  Controls duration.
Reaction rates in the Laboratory Example I: 14 N(p,  ) 15 O stable target  can be measured directly: slowest reaction in the CNO cycle  Controls duration.
1 TCP06 Parksville 8/5/06 Electron capture branching ratios for the nuclear matrix elements in double-beta decay using TITAN ◆ Nuclear matrix elements.
I. Giomataris NOSTOS Neutrino studies with a tritium source Neutrino Oscillations with triton neutrinos The concept of a spherical TPC Measurement of.
Cross section measurements at LNL M.Mezzetto (INFN-Pd) on behalf of INFN-LNL: M. Cinausero, G. De Angelis,G. Prete.
EURISOL Instrumentation Reaching the drip lines Best way to reach drip lines: fragmentation or in-flight fission e.g. 48 Ni, 100 Sn, 78 Ni etc  fragment.
Lawrence Livermore National Laboratory Nicholas Scielzo Lawrence Fellow Physics Division, Physical Sciences LLNL-PRES Lawrence Livermore National.
Neutron scattering systems for calibration of dark matter search and low-energy neutrino detectors A.Bondar, A.Buzulutskov, A.Burdakov, E.Grishnjaev, A.Dolgov,
1 Beta Neutrino Correlation and T-Violation Experiment in Nuclear Beta Decay Rikkyo Univ. Jiro Murata Collaboration Rikkyo Univ. / RIKEN Asahi ANL / Titech.
 -capture measurements with the Recoil-Separator ERNA Frank Strieder Institut für Physik mit Ionenstrahlen Ruhr-Universität Bochum HRIBF Workshop – Nuclear.
Lawrence Livermore National Laboratory Nicholas Scielzo Lawrence Fellow Physics Division, Physical Sciences LLNL-PRES Lawrence Livermore National.
The REXTRAP Penning Trap Pierre Delahaye, CERN/ISOLDE Friedhelm Ames, Pierre Delahaye, Fredrik Wenander and the REXISOLDE collaboration TAS workshop, LPC.
{ Precision measurements of the beta neutrino correlation in the WI Electrostatic Ion Trap 3 December 2012 Sergey Vaintraub.
Fundamental Interactions Physics & Instrumentation Conclusions Conveners: P. Mueller, J. Clark G. Savard, N. Scielzo.
 angular correlations LPC-Team : G. Ban, G. Darius, P. Delahaye, D. Durand, X. Flechard, M. Herbane, M. Labalme, E. Liénard, F. Mauger, A. Mery, O. Naviliat,
A mass-purification method for REX beams
Pierre Delahaye CERN - ISOLDE
 2-proton emission  experimental set-up  decay results  2p emission from 45 Fe  perspectives Jérôme Giovinazzo – CEN Bordeaux-Gradignan – France PROCON’03.
TAS workshop 30-31/3/2004 Aspects of recoil-ion -  correlations in atomic traps A reminder why (V-A, ?S + ?T) Energy scales  basic setup  RIMS Precision.
SLAC, September 25, 2009 Searching for a U -boson with a positron beam Bogdan Wojtsekhowski Thomas Jefferson National Accelerator Facility  The light.
Muon detection in NA60  Experiment setup and operation principle  Coping with background R.Shahoyan, IST (Lisbon)
CP violation in B decays: prospects for LHCb Werner Ruckstuhl, NIKHEF, 3 July 1998.
February 12-15,2003 PROCON 2003, Legnaro-Padova, Italy Jean Charles THOMAS University of Leuven / IKS, Belgium University of Bordeaux I / CENBG, France.
T2K Status Report. The Accelerator Complex a Beamline Performance 3 First T2K run completed January to June x protons accumulated.
The HITRAP Project at GSI For the HITRAP collaboration: Frank Herfurth GSI Darmstadt.
NBI2006 Starting OPERA data-taking with the CNGS beam D.Autiero IN2P3/IPN Lyon 5/9/2006.
Correlation measurements in nuclear  -decay O.Naviliat-Cuncic Laboratoire de Physique Corpusculaire de Caen and Université de Caen Basse-Normandie NuPAC.
Atom trapping and Recoil Ion Spectrometry for  -decay (and other BSM) studies H.W. Wilschut, KVI, Groningen Or why it is easier to measure things standing.
The TRI  P programme at KVI Tests of the Standard Model at low energy Hans Wilschut KVI – Groningen Low energy tests e.g. Time reversal violation precision.
2008 European School of High-Energy Physics - Trest, Czech Republic - 19 August - 1st September Target Tracker Data Analysis In OPERA Experiment S. Dmitrievsky,
Estimates of required MPS reaction time In the merger (at the centers of respective 20deg dipoles and in between 2 lenses) rms R=250 um In the
Measurement of the super-allowed branching ratio of 22 Mg B. Blank, M. Aouadi, P. Ascher, M. Gerbaux, J. Giovinazzo, T. Goigoux, S. Grévy, T. Kurtukian.
(one of the) Request from MPB
The WITCH Experiment 5th International Symposium on Symmetries in Subatomic Physics June 18-22, 2012 KVI, Groningen G. Ban 1, M. Breitenfeldt 2, V. De.
The DESIR facility at SPIRAL2
Antiproton-proton elastic scattering as a day-1 experiment at HESR
J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting
SoLid: Recent Results and Future Prospects
New proposal for the BRIKEN campaign
The DESIR facility at SPIRAL2
Low‐energy precision measurements at the intensity frontier
Diagnostics of FRIBs beam transport line
Tests of fundamental weak interactions
Measurement of the phase of Bs mixing with Bs ϕϕ
of secondary light ion beams
of secondary light ion beams
Neutronics Studies for the Nab Experiment
Accelerator R&D for Future Neutrino Projects
Precision Measurements of Very-Short Lived Nuclei
Angela Gligorova on behalf of the AEgIS and Medipix collaborations
Progress on J-PARC hadron physics in 2016
Experimental determination of isospin mixing in nuclear states;
LPCTrap Experiment Status of Data Analysis
Beam Dump Experiments with Photon and Electron Beams
Probing the structure of weak interactions
Status and perspectives of the LNS-FRIBS facility
Presentation transcript:

Beta Neutrino Correlation Measurement with Trapped Radioactive Ions Gilles BAN LPC Caen, CNRS/IN2P3, Caen, France

Outline Motivation Context How to measure, Traps Status Conclusion

 decay to probe the weak interaction precise measurement of:  decay, probe V-A interaction Allowed transitions, unpolarized nuclei : a v W(E, θ) = W(E) [1 + e cos( q m ) + b ] c E - angular correlation coefficient a For example pure Gamow Teller transition (6He) : SM : Ci = - Ci’ real CT = 0 aGT = -1/3 Any deviation -> Tensor (GT), Scalar (Fermi) contribution -> New physics Any observable linked to  gives access to the parameter a

Context Still up to ~ 5 to 10% of non SM contribution Several measurement with traps Goal : a measurement with a precision below 1% Traps = excellent tool for measurements Matter free Clean environment Well localized source b and recoil detection

Context North america atom traps Triumf, Berkeley 38Km 0.3% scalar PRL 94, 142501 (2005) 21 Na 0.5% mix PRL 93, 102501 (2004) Europe Ion traps Cern, Ganil … For the T contribution « old experiment » Johnson 1963 1% PR 132 1149 (1963)

Correlation Measurement with 6 Helium -Pure Gamow-Teller transition (J = +1) -100% G.S to G.S. -Reasonable Half life = 0.8 s - High Q=3.51 MeV-> Tmax =1.4 keV - GANIL production rate: 108 pps

GANIL accelerators complex LIRAT LPCTrap Production target ECR source Specific Low Energy beamline for Precision Measurement with traps LIRAT Beams characteristics : 10-30 keV, 80 p mm mrad rate : ~ 108 ions/s

LPC TRAP no strong magnetic field (b) ions « at rest » in vacuum ions well localized open geometry : high detection solid angle Cooling and bunching of He collimators Paul trap as precision measurement trap - recoil ion coincidences measurements

Beamline and set up

Trap, Cooler, detectors 20 cm

Status 1998 : Start, 2003 : He cooling with H2, 2004 : Beamline completed 2005 : Commissioning run at GANIL with 6He+ -> proof of principle -> b-recoil coincidences measured from an ion trap 2006 : First data taking run (1 week) Data Out of trap decay Acc. coincidence ToF (ns) Counts -> 105 coincidences [(Da/a)stat ~ 2 %] -> LPCTrap efficiency ~ 5 10-3 % (tduty = 100 ms) -> main systematic effects identified - BG - trapped cloud imagery - detectors response & position, … 8/12

LPCTrap efficiency ~ 5 10-2 % (tduty = 100 ms) 2007-2008 : Optimization & improvement -> fine tuning of the whole setup with 6Li1+ ions (F. Duval, NIM B (2008) ) -> adding of a vacuum impedance to decrease the background -> measurement of ion cloud size (D. Rodríguez, Hyp. Int. 174 (2007)) -> precise alignement of the detectors (1/10 mm) -> adding of a 90° recoil detector -> measurement of plastic scintillator response function with e- spectrometer (Bordeaux) -> … Test in july 2008 with 6He (Ibeam ~ 4 107 pps) Raw data ~2 hours Counts LPCTrap efficiency ~ 5 10-2 % (tduty = 100 ms)  ~ 4 coincidences/s ToF (u.a.) 10/12

One week run with optimized set up ~60 000 events/h October 2008 One week run with optimized set up ~60 000 events/h 4 106 events recorded !! Statistical accuracy reach Analysis and systematics Underway… n mass reconstruction with cloud size, ion temp, BG, Out of trap, BS Geometry, shake off… ~2hours run

Conclusion Precision experiments at low energy are a powerfull tool to probe the SM b-n Correlations with traps LPC TRAP fully working and complete 6He correlation , statistics acquired (~0,5%), analysis underway, precision? other experiments with the set up

THANKS for YOUR ATTENTION !!

GANIL: Jean-Charles Thomas LPCTrap: Gilles Ban Dominique Durand Florian Duval Xavier Fléchard Etienne Liénard François Mauger Oscar Naviliat-Cuncic Philippe Velten Ex-postdoc/students Mustapha Herbane Daniel Rodriguez Guillaume Darius Pierre Delahaye Alain Mery GANIL: Jean-Charles Thomas

19Ne, 35Ar : other candidates available @ LIRAT b+ emitters e- shake off measure Mirror decays (F + GT) r = GT/F determination + precise T1/2 Vud in CKM matrix… - Alternative to 0+ -> 0+ - Competitive with n decay see arXiv:0809.0994 in http://arxiv.org/ : "Determination of |Vud| from nuclear mirror transitions" by O. Naviliat & N. Severijns LPCTrap facility is available to anyone interested by SPIRAL beams… 12/12