COBRA A new Approach to -Decay UK HEP Forum, Abingdon, May 11 th, 2003 Daniel Muenstermann University of Dortmund www.COBRA.physik.uni-dortmund.de COBRA.

Slides:



Advertisements
Similar presentations
SNOLAB TRIUMF 5YP August 3, 2007 Outline Science Experiments Status TRIUMF/SNOLAB relationship Detailed list of collaborative efforts.
Advertisements

NEMO-3 experiment First Results and Future Prospects Ruben Saakyan, UCL UK HEP Neutrino Forum The Coseners House, Abingdon.
Cuoricino results for 2 decay to the first excited state 0 + Sergio Di Domizio for the Cuoricino Collaboration Università and INFN Genova Athens, June.
IS THE NEUTRINO A MAJORANA OR A DIRAC PARTICLE ? Ettore Fiorini, Bologna June or Lepton number conservation or violation Has neutrino a finite.
Proposal to join NEMO-3  decay experiment P. Adamson, R. Saakyan, J. Thomas UCL 27 January 2003.
SuperNEMO Thoughts about next generation NEMO experiment Ruben Saakyan UCL.
Double Beta Decay review
Double Beta Decay L=2 2: (A,Z)  (A,Z+2) + 2e- + 2ne
K. Zuber, Uni. Sussex IDEA Meeting, Milano 9. Nov Status of COBRA.
COBRA Kai Zuber University of Sussex 5 th SNOLAB Workshop,
September 14, 2007Hardy Simgen, TAUP 2007 / Sendai1 Status of the GERDA experiment Hardy Simgen Max-Planck-Institut für Kernphysik Heidelberg on behalf.
M. Dracos 1 Double Beta experiment with emulsions?
GERDA: GERmanium Detector Array
Erice, Kai Zuber1 Status of the COBRA Experiment K. Zuber, TU Dresden.
Status of COBRA K. Zuber, Univ. of Sussex Blaubeuren, July 2007.
DBD matrix elements Welcome and aim of the workshop Experimental situation Outcome.
From CUORICINO to CUORE: To probe the inverted hierarchy region On behalf of the CUORE collaboration DUSL Meeting, Washington DC November 2,-4, 2007 Frank.
Daniel Lenz, University of Wisconsin, Madison 11/05/ APS DNP Cryogenic search for neutrinoless double beta decay Daniel Lenz on behalf of the CUORE.
No s is good s Sheffield Physoc 21/04/2005 Jeanne Wilson A historical introduction to neutrinoless double beta decay.
The COBRA Double Beta Decay Search Experiment
Potassium Geo-neutrino Detection Mark Chen Queen’s University Neutrino Geophysics, Honolulu, Hawaii December 15, 2005.
M. Dracos, CEA, 10/04/ Double Beta experiment with emulsions?
COBRA Double Beta Decay Experiment D.Y. Stewart, Dr. Y.A. Ramachers, Prof. P.F.Harrison Experimental Particle Physics Group University of Warwick What.
Contents Lecture 1 General introduction What is measured in DBD ? Neutrino oscillations and DBD Other BSM physics and DBD Nuclear matrix elements Lecture.
Double beta decay Ruben Saakyan UCL 25 March 2004.
NEMO-3  experiment First Results and Future Prospects Ruben Saakyan, UCL UK HEP Neutrino Forum The Cosener’s House, Abingdon.
GERmanium Detector Array – a Search for Neutrinoless Double Beta Decay X. Liu - MPI für Physik, München Symposium – symmetries and phases in the universe,
CRESST Cryogenic Rare Event Search with Superconducting Thermometers Max-Planck-Institut für Physik University of Oxford Technische Universität München.
From Cuoricino to CUORE: towards the inverted hierarchy region Andrea Giuliani On behalf of the CUORE collaboration University of Insubria (Como) and INFN.
Status of COBRA 6 th SNOLAB Workshop, Picture courtesy
A screening facility for next generation low-background experiments Tom Shutt Laura Cadonati Princeton University.
THE CUORE EXPERIMENT: A SEARCH FOR NEUTRINOLESS DOUBLE BETA DECAY Marco Andrea Carrettoni on behalf of the CUORE collaboration 2 nd International Conference.
F. Cappella Univ. La Sapienza e INFN-Roma NPA4 Frascati, June NPA4 Search for double beta decay of zinc and tungsten with low background ZnWO.
Operation of bare Ge-diodes in LN/LAr 1 st IDEA meeting Como, April 8 (2004) Stefan Schoenert.
Planned Transregional Collaborative Research Center TR27: Neutrinos and Beyond Project A4: Development of segmented germanium detectors for the investigation.
Upgrade and progess on the COBRA double beta detector Sudbury, 26. August 2010 Kai Zuber.
M. Wojcik Instytute of Physics, Jagiellonian University
The CUORE experiment Thomas Bloxham Lawrence Berkeley National Lab PHENO 2011 May 9th 2011.
Underground Laboratories and Low Background Experiments Pia Loaiza Laboratoire Souterrain de Modane Bordeaux, March 16 th, 2006.
M. Wójcik for the GERDA Collaboration Institute of Physics, Jagellonian University Epiphany 2006, Kraków, Poland, 6-7 January 2006.
Neutrinoless double-beta decay and the SuperNEMO project. Darren Price University of Manchester 24 November, 2004.
What is MaGe? MJ outputGERDA output MaGe is a Monte Carlo simulation package dedicated to experiments searching for 0 2  decay in 76 Ge. Created by the.
M. Wójcik Instytut Fizyki, Uniwersytet Jagielloński Instytut Fizyki Doświadczalnej, Uniwersytet Warszawski Warszawa, 10 Marca 2006.
Position sensitive CZT detectors for the COBRA neutrinoless double beta decay project Brian Fulton University of York Neutrinoless double beta decay The.
CTF at Gran Sasso (overview of the hardware) Richard Ford (SNOLAB) (who has not been in the collaboration since 2004) March 19 th 2010.
Cracow Epiphany Conference on Physics in Underground Laboratories and its Connection with LHC Cracow, Poland The GERDA Experiment at Gran.
K. Zuber, Uni. Sussex Status of COBRA IDEA Meeting, Zaragoza 7 Nov
28 May 2008NEMO-3 Neutrino081 NEMO-3 A search for double beta decay Robert L. Flack University College London On behalf of the NEMO-3 collaboration.
NEMO3 experiment: results G. Broudin-Bay LAL (CNRS/ Université Paris-Sud 11) for the NEMO collaboration Moriond EW conference La Thuile, March 2008.
Activities on double beta decay search experiments in Korea 1.Yangyang Underground laboratory 2.Double beta decay search with HPGe & CsI(Tl) 3.Metal Loaded.
Double Beta Decay Experiments Jeanne Wilson University of Sussex 29/06/05, RAL.
1 Performance and Physics with the CsI(Tl) Array at the Kuo-Sheng Reactor Neutrino Laboratory  Physics with CsI(Tl) detector  Period -2 configuration.
A screening facility for next generation low-background experiments Tom Shutt Case Western Reserve University.
The COBRA Experiment Jeanne Wilson University of Sussex, UK On behalf of the COBRA Collaboration TAUP 2007, Sendai, Japan.
GERDA – a Search for Neutrinoless Double Beta Decay MPI für Physik, München Neutrinoless double beta decay and the GERDA experimentThe detector array and.
M.Altmann, GERDA Status Report SNOLAB Workshop IV, Investigating Neutrinoless Double Beta Decay Status of the GERDA Experiment Michael Altmann.
Double Beta Decay - status and future Double beta decay basics Double beta decay basics Experimental challenges Experimental challenges Current experimental.
Second Workshop on large TPC for low energy rare event detection, Paris, December 21 st, 2004.
Phase I: Use available 76 Ge diodes from Heidelberg- Moscow and IGEX experiments (~18 kg). Scrutinize with high siginificance current evidence. Phase II:
1 Double Beta Decay of 150 Nd in the NEMO 3 Experiment Nasim Fatemi-Ghomi (On behalf of the NEMO 3 collaboration) The University of Manchester IOP HEPP.
November 19, 2007Hardy Simgen, IDEA-Meeting Paris Status of the GERDA experiment Hardy Simgen Max-Planck-Institut für Kernphysik Heidelberg on behalf.
COBRA – CZT detectors for neutrinoless double beta decay measurements Martin Freer, University of Birmingham.
Search for Neutrinoless Double Beta Decay with NEMO-3 Zornitza Daraktchieva University College London On behalf of the NEMO3 collaboration PANIC08, Eilat,
Neutrinoless double beta decay (0  ) CdTe Semico nductor Band gap (eV) Electron mobility (cm 2 /V/s) Hole mobility (cm 2 /V/s) Density (g/cm 3.
NEXT: A Neutrinoless 2  Experiment with a Gaseous XeTPC Thorsten Lux IFAE Barcelona in behalf of the NEXT Collaboration.
The COBRA Experiment: Future Prospects
Experiments on Neutrino Nature and Mass
Prompt Gamma Activation Analysis on 76Ge
Deep learning possibilities for GERDA
GERDA Test Stands for Segmented Germanium Detectors
Presentation transcript:

COBRA A new Approach to -Decay UK HEP Forum, Abingdon, May 11 th, 2003 Daniel Muenstermann University of Dortmund COBRA

What is COBRA about? COBRA aims to study -decays of Cd, Zn and Te isotopes. deals with and evolves low-level physics. is currently based in the UK (Univ. of Oxford, K. Zuber, spokesperson) Germany (Univ. of Dortmund) Italy (LNGS)

COBRA Why is (0 ) -decay an opportunity? It can determine the nature of the neutrino (Majorana vs. Dirac particle). n n p p e e Leptoquarks, Rp violating SUSY It might help to disclose other modifications of weak processes like right-handed weak currents n n p p L=2, Eff. Majorana masses It can reveal the rest-mass of the electron neutrino on an absolute scale.

COBRA More on + + decays There are 3 possible modes: + +: (A,Z) (A,Z-2) + 2 e + (+2 e )(Q - 4 m e c 2 ) + /EC:e - + (A,Z) (A,Z-2) + e + (+2 e ) (Q - 2 m e c 2 ) EC/EC:2 e - + (A,Z) (A,Z-2) (+2 e ) (Q) (eV) + + -ellipsoid Heidelberg- Moscow evidence + + decays are dominated by right-handed weak currents ! EC/EC is preferred by phase space!

COBRA Why is CdZnTe a favourable material? 116 Cd:Q-Value at 2.8 MeV, above all naturally occuring -lines 130 Te:has large natural abundance (34 %) sits in compton gap of 208 Tl direct comparison to geochemical experiments 106 Cd: + + -decay at 2.7 MeV possible, but + /EC or EC/EC decays preferred by phase space It contains 9 -isotopes, among them potential for a background-free experiment where mass limits grow linear in measurement time!

COBRA Why are CdZnTe semiconductor detectors advantagous devices? good energy resolution (compared to scintillators) high density compared to gaseous ionisation detectors, large source masses no cooling needed with CdZnTe industrially available, commercial development in progress in our case: source = detector particle tracking is possible with pixel-devices (solid-state-TPC) operation in cryogenic mode possible

COBRA Reality strikes back: Current Limitations of CdZnTe Crystal growth:large quantities: 1 cm 3 cubes selected detectors: 16 cm 3 cubes Large hole trapping: Use selective electron readout Therefore: Instead of few large crystals (Heidelberg-Moscow = 1-3 kg) build an array of small detectors

COBRA Idea: Build an array of CdZnTe detectors. Characteristics of COBRA: minimal use of construction material close to the detectors necessary as no cooling is needed source = detector 9 -isotopes measured simultaneously

COBRA Early Achievements of COBRA First ad-hoc efforts with commercial 0.5 cm 3 detector and MCA-based readout: Veto and shield are working 2 publications with new and improved limits: Muenstermann and Zuber: An alternative Search for the Electron Capture of 123 Te, J. Phys. G: Nucl. Part. Phys. 29 (2003) B1-B4 Kiel, Muenstermann and Zuber: A Search for various Double Beta Decay Modes of Cd, Te and Zn Isotopes, nucl-ex/ , to be published in Nucl. Phys. A

COBRA Early Achievements of COBRA Calibration spectrum with 228 Th:

COBRA Low energy part of the spectrum: Early Achievements of COBRA Background at 2.8 MeV: ~ 5 ·10 -4 events/(keV g d) 208 Tl-peak at 2.6 MeV visible. Contamination in detector or surroundings? Build own low-level mounting Spectrum with and without shield:

COBRA The Status of COBRA There is a 2 x 2 array of 1 cm 3 detectors with custom-built preamplifier electronics (still) CAMAC-based event-by-event readout passive copper and lead shielding a plastic-scintillator based cosmic muon veto

COBRA Time schedule Next week: relocation of the setup into the Gran Sasso laboratory Autumn 2003:First results due, decision about funding of 4 x 4 prototype due Spring 2004:scalable 4 x 4 prototype and scalable readout electronics operational Winter 2004:proposal for a competitive 0 -decay based on CdZnTe

COBRA ad hoc: COBRA compared to An Ideal Experiment by Steve Elliot large mass:CdZnTe detectors are available with m < 100 g Array of detectors good source radiopurity:Work in progress, no serious cosmogenic background demonstrated technology:Again, work in progress natural isotopes:Yes source = detector: Yes energy resolution (< 3 %):Yes ease of operation:Yes, but ask us in autumn... large Q value:Yes event reconstruction: With pixel detectors (3D)

COBRA Summary and Outlook COBRA uses commercially available CdZnTe detectors to measure 9 isotopes simultaneously has already improved 6 limits with comparably little effort will move from the surface to the Gran Sasso underground lab for improved low-level measurements next week is up to now a rather small collaboration, so...

COBRA Last Words Join the party! Collaborators most welcome!