Podzemní laboratoř LSM - česká účast ve výzkumné infrastruktuře evropského významu
- NázevTitle
- Podzemní laboratoř LSM - česká účast ve výzkumné infrastruktuře evropského významuUnderground laboratory LSM - Czech participation to European-level research infrastructure
- PoskytovatelProvider
- Evropská komiseEuropean Commission
- ProgramProgramme
- OPVVV - Operační program Výzkum, vývoj a vzdělávání - Strukturální fondy EUOperational Programme – Research, Development and Education – Structural Funds EU
- Kód CEPCEP code
- EF16_013/0001733
- Datum zahájeníStart date
- 2017-01-01
- Datum ukončeníEnd date
- 2019-12-31
- Vztah ČVUTCTU relation
- ČVUT je v pozici příjemce/koordinátor a alespoň jeden z ostatních partnerů je také "příjemce"CTU is a beneficiary/coordinator, and at least one of the other partners also has the role of "a beneficiary"
- Řešitel ČVUTCTU investigator
- doc. Ing. Ivan Štekl, CSc.
- Řešitelský tým (ÚTEF)Team (UTEF)
- (koordinátorcoordinator)
AbstraktAbstract
Cílem projektu je podpora výzkumu v podzemní laboratoři LSM (Francie), upgrade výzkumné infrastruktury a řízení. Aktivity projektu jsou zaměřeny na neutrinovou fyziku (experimentální a teoretické studium různých módů dvojného rozpadu beta, vývoj pro potřeby budoucích experimentů), na instrumentaci a měření ultra nízké koncentrace radionuklidů a instrumentaci pro radiobiologii. Na projektu se podílí Ústav technické a experimentální fyziky ČVUT a Státní ústav radiační ochrany, v.v.i.
Cílem projektu je podpora výzkumu v podzemní laboratoři LSM (Francie), upgrade výzkumné infrastruktury a řízení. Aktivity projektu jsou zaměřeny na neutrinovou fyziku (experimentální a teoretické studium různých módů dvojného rozpadu beta, vývoj pro potřeby budoucích experimentů), na instrumentaci a měření ultra nízké koncentrace radionuklidů a instrumentaci pro radiobiologii. Na projektu se podílí Ústav technické a experimentální fyziky ČVUT a Státní ústav radiační ochrany, v.v.i.
VýsledkyResults
- Environmental radionuclides as contaminants of HPGe gamma-ray spectrometers: Monte Carlo simulations for Modane underground laboratoryEnvironmental radionuclides as contaminants of HPGe gamma-ray spectrometers: Monte Carlo simulations for Modane underground laboratory
- Study of Reconstruction Precision of Double Beta Decay Vertex for SuperNEMO DemonstratorStudy of Reconstruction Precision of Double Beta Decay Vertex for SuperNEMO Demonstrator
- COBRA Collaboration Meeting Prague 2019COBRA Collaboration Meeting Prague 2019
- Reproduction of exact solutions of Lipkin model by nonlinear higher random-phase approximationReproduction of exact solutions of Lipkin model by nonlinear higher random-phase approximation
- Neutrino mass, electron capture, and the shake-off contributionsNeutrino mass, electron capture, and the shake-off contributions
- Favored Neutrino Mass Mechanisms of the 0nbb-Decay Unified by an Interpolating FormulaFavored Neutrino Mass Mechanisms of the 0nbb-Decay Unified by an Interpolating Formula
- Search for the double-beta decay of 82Se to the excited states of 82Kr with NEMO-3Search for the double-beta decay of 82Se to the excited states of 82Kr with NEMO-3
- Search for Neutrinoless Quadruple-beta Decay of Nd-150 with the NEMO-3 DetectorSearch for Neutrinoless Quadruple-beta Decay of Nd-150 with the NEMO-3 Detector
- Low-scale seesaw from neutrino condensationLow-scale seesaw from neutrino condensation
- Measurement of the 2 nu beta beta decay half-life and search for the 0 nu beta beta decay of Cd-116 with the NEMO-3 detectorMeasurement of the 2 nu beta beta decay half-life and search for the 0 nu beta beta decay of Cd-116 with the NEMO-3 detector
- 0 nu beta beta-decay nuclear matrix element for light and heavy neutrino mass mechanisms from deformed quasiparticle random-phase approximation calculations for Ge-76, Se-82, Te-130, Xe-136, and Nd-150 with isospin restoration0 nu beta beta-decay nuclear matrix element for light and heavy neutrino mass mechanisms from deformed quasiparticle random-phase approximation calculations for Ge-76, Se-82, Te-130, Xe-136, and Nd-150 with isospin restoration
- Search for sterile neutrinos at the DANSS experimentSearch for sterile neutrinos at the DANSS experiment
- Neutrinoless and Two-Neutrino Double-Beta Decay with Emission of Single Free ElectronNeutrinoless and Two-Neutrino Double-Beta Decay with Emission of Single Free Electron
- The VII International Pontecorvo Neutrino Physics SchoolThe VII International Pontecorvo Neutrino Physics School
- Bound-State Double-Beta DecayBound-State Double-Beta Decay
- SuperNEMO Collaboration MeetingSuperNEMO Collaboration Meeting
- Bound-state double-beta decayBound-state double-beta decay
- Neutrinoless double beta-decay and neutrino nonstandard interactionsNeutrinoless double beta-decay and neutrino nonstandard interactions
- Quenching of g(A) deduced from the beta-spectrum shape of Cd-113 measured with the COBRA experimentQuenching of g(A) deduced from the beta-spectrum shape of Cd-113 measured with the COBRA experiment
- Detailed studies of 100 Mo two-neutrino double beta decay in NEMO-3Detailed studies of 100 Mo two-neutrino double beta decay in NEMO-3
- Interpolating formula for the 0 nu beta beta-decay half-life in the case of light and heavy neutrino mass mechanismsInterpolating formula for the 0 nu beta beta-decay half-life in the case of light and heavy neutrino mass mechanisms
- Two neutrino double-beta decay and effective axial-vector coupling constantTwo neutrino double-beta decay and effective axial-vector coupling constant
- Development of methods for the preparation of radiopure Se-82 sources for the SuperNEMO neutrinoless double-beta decay experimentDevelopment of methods for the preparation of radiopure Se-82 sources for the SuperNEMO neutrinoless double-beta decay experiment
- Proc. of student poster session of the VII International Pontecorvo Neutrino Physics School (Prague, Czech Republic, August 20 - September 1, 2017)Proc. of student poster session of the VII International Pontecorvo Neutrino Physics School (Prague, Czech Republic, August 20 - September 1, 2017)
- VII. ročník letní školy Bruna Pontecorva proběhl v Praze7th Bruno Pontecorvo Summer School was held in Prague
- Investigating the Double Beta Decay of 58NiInvestigating the Double Beta Decay of 58Ni
- Investigation of double beta decay of 58Ni at the Modane Underground LaboratoryInvestigation of double beta decay of 58Ni at the Modane Underground Laboratory
- Tajemná neutrinaMysterious neutrinos
- Reproduction of exact solutions of Lipkin model by nonlinear higher random-phase approximationReproduction of exact solutions of Lipkin model by nonlinear higher random-phase approximation
- Final results on Se-82 double beta decay to the ground state of Kr-82 from the NEMO-3 experimentFinal results on Se-82 double beta decay to the ground state of Kr-82 from the NEMO-3 experiment
- 0v beta beta and 2v beta beta nuclear matrix elements evaluated in closure approximation, neutrino potentials and SU(4) symmetry0v beta beta and 2v beta beta nuclear matrix elements evaluated in closure approximation, neutrino potentials and SU(4) symmetry
- Investigation of β+EC, EC/EC processes in 74SeInvestigation of β+EC, EC/EC processes in 74Se
- The Large Enriched Germanium Experiment for Neutrinoless Double Beta Decay (LEGEND)The Large Enriched Germanium Experiment for Neutrinoless Double Beta Decay (LEGEND)
- The lambda Mechanism of the 0v beta beta-DecayThe lambda Mechanism of the 0v beta beta-Decay
- Nonlinear Higher Quasiparticle Random Phase ApproximationNonlinear Higher Quasiparticle Random Phase Approximation
- Double-Beta Decay with Emission of Single Free ElectronDouble-Beta Decay with Emission of Single Free Electron
- Investigation of Double Beta Decay of Ni-58 with the Obelix SpectrometerInvestigation of Double Beta Decay of Ni-58 with the Obelix Spectrometer
- Reactor antineutrino spectra and forbidden beta decaysReactor antineutrino spectra and forbidden beta decays
- Improved description of the 2νββ-decay and a possibility to determine the effective axial-vector coupling constantImproved description of the 2νββ-decay and a possibility to determine the effective axial-vector coupling constant