D. Lalanne
University of Paris-Sud
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Featured researches published by D. Lalanne.
Physical Review C | 2009
J. Argyriades; R. Arnold; C. Augier; J. Baker; A. S. Barabash; A. Basharina-Freshville; M. Bongrand; G. Broudin; V. Brudanin; A. J. Caffrey; E. Chauveau; Z. Daraktchieva; D. Durand; V. Egorov; N. Fatemi-Ghomi; R. L. Flack; Ph. Hubert; J. Jerie; S. Jullian; M. Kauer; S. King; A. Klimenko; O. Kochetov; S. I. Konovalov; V. Kovalenko; D. Lalanne; T. Lamhamdi; K. Lang; Y. Lemière; C. Longuemare
The half-life for double-{beta} decay of {sup 150}Nd has been measured by the NEMO-3 experiment at the Modane Underground Laboratory. Using 924.7 days of data recorded with 36.55 g of {sup 150}Nd, we measured the half-life for 2{nu}{beta}{beta} decay to be T{sub 1/2}{sup 2{nu}}=(9.11{sub -0.22}{sup +0.25}(stat.){+-}0.63(syst.))x10{sup 18} yr. The observed limit on the half-life for neutrinoless double-{beta} decay is found to be T{sub 1/2}{sup 0{nu}}>1.8x10{sup 22} yr at 90% confidence level. This translates into a limit on the effective Majorana neutrino mass of <4.0-6.3 eV if the nuclear deformation is taken into account. We also set limits on models involving Majoron emission, right-handed currents, and transitions to excited states.
Nuclear Physics | 1999
R. Arnold; C. Augier; J. Baker; A. S. Barabash; D. Blum; V. Brudanin; A. J. Caffrey; Jean-Eric Campagne; E. Caurier; D. Dassie; V. Egorov; T. Filipova; R. Gurriaran; J.L. Guyonnet; F. Hubert; Ph. Hubert; S. Jullian; I. Kisel; O. Kochetov; V.N. Kornoukhov; V. Kovalenko; D. Lalanne; F. Laplanche; F. Leccia; I. Linck; C. Longuemare; Ch. Marquet; F. Mauger; H.W. Nicholson; I. Pilugin
Abstract After 10357 h of running the NEMO-2 tracking detector with an isotopically enriched zirconium source (0.084 mol yr of 96Zr), a ββ2ν decay half-life of T1/2=(2.1+0.8(stat)−0.4(stat)±0.2(syst))·1019 y was measured. Limits with a 90% C.L. on the 96Zr half-lives of 1.0·1021 y for ββ0ν decay to the ground state, 3.9·1020 y to the 2+ excited state and 3.5·1020 y for ββ0νχ0 decay with a Majoron (χ0) were obtained. The data also provide direct limits at the 90% C.L. for the 94Zr half-lives. These limits are 1.1·1017 y for ββ2ν decay to the ground state, 1.9·1019 y for ββ0ν decay to the ground state and 2.3·1018 y for ββ0νχ0 decay to ground state.
Nuclear Physics | 2007
R. Arnold; V. I. Umatov; C.S. Sutton; F. Piquemal; V. Timkin; L. Vála; F. Hubert; A. J. Caffrey; V. Kovalenko; J. Baker; I. Vanyushin; L. Simard; V. Vorobel; J. Jerie; I. Stekl; V. Brudanin; O. Kochetov; S. Jullian; R. Saakyan; G. Broudin; V. Egorov; V.I. Tretyak; V. Vasiliev; G. Szklarz; X. Sarazin; Y. Lemière; N. Fatemi-Ghomi; S. I. Konovalov; A. Nachab; Ts. Vylov
The double beta decay of 100Mo to the 0^+_1 and 2^+_1 excited states of 100Ru is studied using the NEMO 3 data. After the analysis of 8024 h of data the half-life for the two-neutrino double beta decay of 100Mo to the excited 0^+_1 state is measured to be T^(2nu)_1/2 = [5.7^{+1.3}_{-0.9}(stat)+/-0.8(syst)]x 10^20 y. The signal-to-background ratio is equal to 3. Information about energy and angular distributions of emitted electrons is also obtained. No evidence for neutrinoless double beta decay to the excited 0^+_1 state has been found. The corresponding half-life limit is T^(0nu)_1/2(0^+ -->0^+_1)>8.9 x 10^22 y (at 90% C.L.). The search for the double beta decay to the 2^+_1 excited state has allowed the determination of limits on the half-life for the two neutrino mode T^(2nu)_1/2(0^+ -->2^+_1)>1.1 x 10^21 y (at 90% C.L.) and for the neutrinoless mode T^(0nu)_1/2(0^+ -->2^+_1)>1.6 x 10^23 y (at 90% C.L.).
Physical Review D | 2014
R. Arnold; C. Augier; J. Baker; A. S. Barabash; A. Basharina-Freshville; S. Blondel; S. Blot; M. Bongrand; V. Brudanin; J. Busto; A.J. Caffrey; C. Cerna; A. Chapon; E. Chauveau; D. Duchesneau; D. Durand; V. Egorov; G. Eurin; J. J. Evans; R. Flack; X. Garrido; H. Gómez; B. Guillon; P. Guzowski; R. Hodák; Ph. Hubert; C. Hugon; S. Jullian; A. Klimenko; O. Kochetov
We report the results of a search for the neutrinoless double-β decay (0νββ) of Mo100, using the NEMO-3 detector to reconstruct the full topology of the final state events. With an exposure of 34.7u2009u2009kg·y, no evidence for the 0νββ signal has been found, yielding a limit for the light Majorana neutrino mass mechanism of T1/2(0νββ)>1.1×1024 years (90% C.L.) once both statistical and systematic uncertainties are taken into account. Depending on the nuclear matrix elements this corresponds to an upper limit on the Majorana effective neutrino mass of ⟨mν⟩<0.3–0.9u2009u2009eV (90% C.L.). Constraints on other lepton number violating mechanisms of 0νββ decays are also given. Searching for high-energy double electron events in all suitable sources of the detector, no event in the energy region [3.2–10] MeV is observed for an exposure of 47u2009u2009kg·y.
Jetp Letters | 2004
R. Arnold; C. Augier; J. Baker; A. S. Barabash; V. Brudanin; A. J. Caffrey; V. Egorov; J.L. Guyonnet; F. Hubert; Ph. Hubert; L. Jenner; C. Jollet; S. Jullian; A. Klimenko; O. Kochetov; S. I. Konovalov; V. Kovalenko; D. Lalanne; F. Leccia; I. Linck; C. Longuemare; G. Lutter; Ch. Marquet; F. Mauger; H.W. Nicholson; H. Ohsumi; F. Piquemal; J. L. Reyss; R. Saakyan; X. Sarazin
AbstractAfter analysis of 5797 h of data from the detector NEMO3, new limits on neutrinoless double beta decay of 100Mo (T1/2>3.1×1023y, 90% CL) and 82Se (T1/2>1.4×1023y, 90% CL) have been obtained. The corresponding limits on the effective majorana neutrino mass are: 〈mv〉<(0.8–1.2) eV and 〈mv〉<(1.5–3.1) eV, respectively. Also the limits on double-beta decay with Majoron emission are: T1/2>1.4×1022y (90% CL) for 100Mo and T1/2>1.2×1022y (90% CL) for 82Se. Corresponding bounds on the Majoron-neutrino coupling constant are 〈 gee〉<(0.5–0.9)×10−4 and <(0.7−1.6)×10−4. Two-neutrino 2β-decay half-lives have been measured with a high accuracy, n
Physical Review Letters | 2011
R. Arnold; C. Augier; J. Baker; A. S. Barabash; A. Basharina-Freshville; S. Blondel; M. Bongrand; G. Broudin-Bay; V. Brudanin; A. J. Caffrey; A. Chapon; E. Chauveau; D. Durand; V. Egorov; R. Flack; X. Garrido; J. Grozier; B. Guillon; Ph. Hubert; C. M. Jackson; S. Jullian; M. Kauer; A. Klimenko; O. Kochetov; S. I. Konovalov; V. Kovalenko; D. Lalanne; T. Lamhamdi; K. Lang; Z. Liptak
Physical Review D | 2016
R. Arnold; C. Augier; A. M. Bakalyarov; J. Baker; A. S. Barabash; A. Basharina-Freshville; S. Blondel; S. Blot; M. Bongrand; V. Brudanin; J. Busto; A.J. Caffrey; S. Calvez; M. Cascella; C. Cerna; J. P. Cesar; A. Chapon; E. Chauveau; A. Chopra; D. Duchesneau; D. Durand; V. Egorov; G. Eurin; J. J. Evans; L. Fajt; D. Filosofov; R. L. Flack; X. Garrido; Haley Louise Gomez; B. Guillon
T_{1/2}^{100_{Mo} } = [7.68 pm 0.02(stat) pm 0.54(syst)] times 10^{18} y
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2001
R. Arnold; C. Augier; J. Baker; A. S. Barabash; O. Bing; D. Blum; V. Brudanin; A. J. Caffrey; Jean-Eric Campagne; E. Caurier; D. Dassie; V. Egorov; K. Errahmane; T. Filipova; J.L. Guyonnet; F. Hubert; Ph. Hubert; S. Jullian; O. Kochetov; I. Kisel; V.N. Kornoukhov; V. Kovalenko; V.F. Kuzichev; D. Lalanne; F. Laplanche; F. Leccia; I. Linck; C. Longuemare; Ch. Marquet; F. Mauger
Physical Review D | 2016
R. Arnold; C. Augier; J. Baker; A. S. Barabash; A. Basharina-Freshville; S. Blondel; S. Blot; M. Bongrand; V. Brudanin; J. Busto; A. J. Caffrey; S. Calvez; M. Cascella; C. Cerna; J. P. Cesar; A. Chapon; E. Chauveau; A. Chopra; D. Duchesneau; D. Durand; V. Egorov; G. Eurin; J. J. Evans; L. Fajt; D. Filosofov; R. L. Flack; X. Garrido; H. Gómez; B. Guillon; P. Guzowski
n and n
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1997
R. Arnold; C. Augier; A. S. Barabash; D. Blum; V. Brudanin; Jean-Eric Campagne; D. Dassie; V. Egorov; R. Eschbach; J.L. Guyonnet; F. Hubert; Ph. Hubert; S. Jullian; I. Kisel; O. Kochetov; V. N. Kornoukov; V. Kovalenko; D. Lalanne; F. Laplanche; F. Leccia; I. Linck; C. Longuemare; F. Mauger; P. Mennrath; H.W. Nicholson; A.A. Nozdrin; F. Piquemal; O. Purtov; J. L. Reyss; F. Scheibling