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27 results on '"Freedman, SJ"'

1. Erratum: Measurement of the 2νββ Decay Half-Life of ^{130}Te with CUORE [Phys. Rev. Lett. 126, 171801 (2021)].

Author

Adams DQ, Alduino C, Alfonso K, Avignone FT, Azzolini O, Bari G, Bellini F, Benato G, Biassoni M, Branca A, Brofferio C, Bucci C, Camilleri J, Caminata A, Campani A, Canonica L, Cao XG, Capelli S, Cappelli L, Cardani L, Carniti P, Casali N, Chiesa D, Clemenza M, Copello S, Cosmelli C, Cremonesi O, Creswick RJ, D'Addabbo A, Dafinei I, Davis CJ, Dell'Oro S, Di Domizio S, Dompè V, Fang DQ, Fantini G, Faverzani M, Ferri E, Ferroni F, Fiorini E, Franceschi MA, Freedman SJ, Fu SH, Fujikawa BK, Giachero A, Gironi L, Giuliani A, Gorla P, Gotti C, Gutierrez TD, Han K, Heeger KM, Huang RG, Huang HZ, Johnston J, Keppel G, Kolomensky YG, Ligi C, Ma L, Ma YG, Marini L, Maruyama RH, Mayer D, Mei Y, Moggi N, Morganti S, Napolitano T, Nastasi M, Nikkel J, Nones C, Norman EB, Nucciotti A, Nutini I, O'Donnell T, Ouellet JL, Pagan S, Pagliarone CE, Pagnanini L, Pallavicini M, Pattavina L, Pavan M, Pessina G, Pettinacci V, Pira C, Pirro S, Pozzi S, Previtali E, Puiu A, Rosenfeld C, Rusconi C, Sakai M, Sangiorgio S, Schmidt B, Scielzo ND, Sharma V, Singh V, Sisti M, Speller D, Surukuchi PT, Taffarello L, Terranova F, Tomei C, Vetter KJ, Vignati M, Wagaarachchi SL, Wang BS, Welliver B, Wilson J, Wilson K, Winslow LA, Zimmermann S, and Zucchelli S

Abstract

This corrects the article DOI: 10.1103/PhysRevLett.126.171801.

Published
2023
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2. New Direct Limit on Neutrinoless Double Beta Decay Half-Life of ^{128}Te with CUORE.

Author

Adams DQ, Alduino C, Alfonso K, Avignone FT, Azzolini O, Bari G, Bellini F, Benato G, Beretta M, Biassoni M, Branca A, Brofferio C, Bucci C, Camilleri J, Caminata A, Campani A, Canonica L, Cao XG, Capelli S, Capelli C, Cappelli L, Cardani L, Carniti P, Casali N, Celi E, Chiesa D, Clemenza M, Copello S, Cremonesi O, Creswick RJ, D'Addabbo A, Dafinei I, Del Corso F, Dell'Oro S, Di Domizio S, Di Lorenzo S, Dompè V, Fang DQ, Fantini G, Faverzani M, Ferri E, Ferroni F, Fiorini E, Franceschi MA, Freedman SJ, Fu SH, Fujikawa BK, Ghislandi S, Giachero A, Gianvecchio A, Gironi L, Giuliani A, Gorla P, Gotti C, Gutierrez TD, Han K, Hansen EV, Heeger KM, Huang RG, Huang HZ, Johnston J, Keppel G, Kolomensky YG, Kowalski R, Liu R, Ma L, Ma YG, Marini L, Maruyama RH, Mayer D, Mei Y, Morganti S, Napolitano T, Nastasi M, Nikkel J, Nones C, Norman EB, Nucciotti A, Nutini I, O'Donnell T, Olmi M, Ouellet JL, Pagan S, Pagliarone CE, Pagnanini L, Pallavicini M, Pattavina L, Pavan M, Pessina G, Pettinacci V, Pira C, Pirro S, Pozzi S, Previtali E, Puiu A, Quitadamo S, Ressa A, Rosenfeld C, Sangiorgio S, Schmidt B, Scielzo ND, Sharma V, Singh V, Sisti M, Speller D, Surukuchi PT, Taffarello L, Terranova F, Tomei C, Vetter KJ, Vignati M, Wagaarachchi SL, Wang BS, Welliver B, Wilson J, Wilson K, Winslow LA, Zimmermann S, and Zucchelli S

Subjects
Half-Life, Bayes Theorem, Granisetron
Abstract

The Cryogenic Underground Observatory for Rare Events (CUORE) at Laboratori Nazionali del Gran Sasso of INFN in Italy is an experiment searching for neutrinoless double beta (0νββ) decay. Its main goal is to investigate this decay in ^{130}Te, but its ton-scale mass and low background make CUORE sensitive to other rare processes as well. In this Letter, we present our first results on the search for 0νββ decay of ^{128}Te, the Te isotope with the second highest natural isotopic abundance. We find no evidence for this decay, and using a Bayesian analysis we set a lower limit on the ^{128}Te 0νββ decay half-life of T_{1/2}>3.6×10^{24}  yr (90% CI). This represents the most stringent limit on the half-life of this isotope, improving by over a factor of 30 the previous direct search results, and exceeding those from geochemical experiments for the first time.

Published
2022
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3. Measurement of the 2νββ Decay Half-Life of ^{130}Te with CUORE.

Author

Adams DQ, Alduino C, Alfonso K, Avignone FT, Azzolini O, Bari G, Bellini F, Benato G, Biassoni M, Branca A, Brofferio C, Bucci C, Camilleri J, Caminata A, Campani A, Canonica L, Cao XG, Capelli S, Cappelli L, Cardani L, Carniti P, Casali N, Chiesa D, Clemenza M, Copello S, Cosmelli C, Cremonesi O, Creswick RJ, D'Addabbo A, Dafinei I, Davis CJ, Dell'Oro S, Di Domizio S, Dompè V, Fang DQ, Fantini G, Faverzani M, Ferri E, Ferroni F, Fiorini E, Franceschi MA, Freedman SJ, Fu SH, Fujikawa BK, Giachero A, Gironi L, Giuliani A, Gorla P, Gotti C, Gutierrez TD, Han K, Heeger KM, Huang RG, Huang HZ, Johnston J, Keppel G, Kolomensky YG, Ligi C, Ma L, Ma YG, Marini L, Maruyama RH, Mayer D, Mei Y, Moggi N, Morganti S, Napolitano T, Nastasi M, Nikkel J, Nones C, Norman EB, Nucciotti A, Nutini I, O'Donnell T, Ouellet JL, Pagan S, Pagliarone CE, Pagnanini L, Pallavicini M, Pattavina L, Pavan M, Pessina G, Pettinacci V, Pira C, Pirro S, Pozzi S, Previtali E, Puiu A, Rosenfeld C, Rusconi C, Sakai M, Sangiorgio S, Schmidt B, Scielzo ND, Sharma V, Singh V, Sisti M, Speller D, Surukuchi PT, Taffarello L, Terranova F, Tomei C, Vetter KJ, Vignati M, Wagaarachchi SL, Wang BS, Welliver B, Wilson J, Wilson K, Winslow LA, Zimmermann S, and Zucchelli S

Abstract

We measured two-neutrino double beta decay of ^{130}Te using an exposure of 300.7 kg yr accumulated with the CUORE detector. Using a Bayesian analysis to fit simulated spectra to experimental data, it was possible to disentangle all the major background sources and precisely measure the two-neutrino contribution. The half-life is in agreement with past measurements with a strongly reduced uncertainty: T_{1/2}^{2ν}=7.71_{-0.06}^{+0.08}(stat)_{-0.15}^{+0.12}(syst)×10^{20}  yr. This measurement is the most precise determination of the ^{130}Te 2νββ decay half-life to date.

Published
2021
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4. Improved Limit on Neutrinoless Double-Beta Decay in ^{130} Te with CUORE.

Author

Adams DQ, Alduino C, Alfonso K, Avignone FT, Azzolini O, Bari G, Bellini F, Benato G, Biassoni M, Branca A, Brofferio C, Bucci C, Caminata A, Campani A, Canonica L, Cao XG, Capelli S, Cappelli L, Cardani L, Carniti P, Casali N, Chiesa D, Chott N, Clemenza M, Copello S, Cosmelli C, Cremonesi O, Creswick RJ, D'Addabbo A, D'Aguanno D, Dafinei I, Davis CJ, Dell'Oro S, Di Domizio S, Dompè V, Fang DQ, Fantini G, Faverzani M, Ferri E, Ferroni F, Fiorini E, Franceschi MA, Freedman SJ, Fujikawa BK, Giachero A, Gironi L, Giuliani A, Gorla P, Gotti C, Gutierrez TD, Han K, Heeger KM, Huang RG, Huang HZ, Johnston J, Keppel G, Kolomensky YG, Ligi C, Ma YG, Ma L, Marini L, Maruyama RH, Mei Y, Moggi N, Morganti S, Napolitano T, Nastasi M, Nikkel J, Nones C, Norman EB, Novati V, Nucciotti A, Nutini I, O'Donnell T, Ouellet JL, Pagliarone CE, Pagnanini L, Pallavicini M, Pattavina L, Pavan M, Pessina G, Pettinacci V, Pira C, Pirro S, Pozzi S, Previtali E, Puiu A, Rosenfeld C, Rusconi C, Sakai M, Sangiorgio S, Schmidt B, Scielzo ND, Sharma V, Singh V, Sisti M, Speller D, Surukuchi PT, Taffarello L, Terranova F, Tomei C, Vignati M, Wagaarachchi SL, Wang BS, Welliver B, Wilson J, Wilson K, Winslow LA, Zanotti L, Zimmermann S, and Zucchelli S

Abstract

We report new results from the search for neutrinoless double-beta decay in ^{130} Te with the CUORE detector. This search benefits from a fourfold increase in exposure, lower trigger thresholds, and analysis improvements relative to our previous results. We observe a background of (1.38±0.07)×10^{-2}  counts/(keV kg yr)) in the 0νββ decay region of interest and, with a total exposure of 372.5 kg yr, we attain a median exclusion sensitivity of 1.7×10^{25}  yr. We find no evidence for 0νββ decay and set a 90% credibility interval Bayesian lower limit of 3.2×10^{25}  yr on the ^{130} Te half-life for this process. In the hypothesis that 0νββ decay is mediated by light Majorana neutrinos, this results in an upper limit on the effective Majorana mass of 75-350 meV, depending on the nuclear matrix elements used.

Published
2020
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5. First Results from CUORE: A Search for Lepton Number Violation via 0νββ Decay of ^{130}Te.

Author

Alduino C, Alessandria F, Alfonso K, Andreotti E, Arnaboldi C, Avignone FT, Azzolini O, Balata M, Bandac I, Banks TI, Bari G, Barucci M, Beeman JW, Bellini F, Benato G, Bersani A, Biare D, Biassoni M, Bragazzi F, Branca A, Brofferio C, Bryant A, Buccheri A, Bucci C, Bulfon C, Camacho A, Caminata A, Canonica L, Cao XG, Capelli S, Capodiferro M, Cappelli L, Cardani L, Cariello M, Carniti P, Carrettoni M, Casali N, Cassina L, Cereseto R, Ceruti G, Chiarini A, Chiesa D, Chott N, Clemenza M, Conventi D, Copello S, Cosmelli C, Cremonesi O, Crescentini C, Creswick RJ, Cushman JS, D'Addabbo A, D'Aguanno D, Dafinei I, Datskov V, Davis CJ, Del Corso F, Dell'Oro S, Deninno MM, Di Domizio S, Di Vacri ML, Di Paolo L, Drobizhev A, Ejzak L, Faccini R, Fang DQ, Faverzani M, Ferri E, Ferroni F, Fiorini E, Franceschi MA, Freedman SJ, Fujikawa BK, Gaigher R, Giachero A, Gironi L, Giuliani A, Gladstone L, Goett J, Gorla P, Gotti C, Guandalini C, Guerzoni M, Gutierrez TD, Haller EE, Han K, Hansen EV, Heeger KM, Hennings-Yeomans R, Hickerson KP, Huang HZ, Iannone M, Ioannucci L, Kadel R, Keppel G, Kogler L, Kolomensky YG, Leder A, Ligi C, Lim KE, Liu X, Ma YG, Maiano C, Maino M, Marini L, Martinez M, Martinez Amaya C, Maruyama RH, Mei Y, Moggi N, Morganti S, Mosteiro PJ, Nagorny SS, Napolitano T, Nastasi M, Nisi S, Nones C, Norman EB, Novati V, Nucciotti A, Nutini I, O'Donnell T, Olcese M, Olivieri E, Orio F, Orlandi D, Ouellet JL, Pagliarone CE, Pallavicini M, Palmieri V, Pattavina L, Pavan M, Pedretti M, Pedrotta R, Pelosi A, Pessina G, Pettinacci V, Piperno G, Pira C, Pirro S, Pozzi S, Previtali E, Reindl F, Rimondi F, Risegari L, Rosenfeld C, Rossi C, Rusconi C, Sakai M, Sala E, Salvioni C, Sangiorgio S, Santone D, Schaeffer D, Schmidt B, Schmidt J, Scielzo ND, Singh V, Sisti M, Smith AR, Stivanello F, Taffarello L, Tatananni L, Tenconi M, Terranova F, Tessaro M, Tomei C, Ventura G, Vignati M, Wagaarachchi SL, Wallig J, Wang BS, Wang HW, Welliver B, Wilson J, Wilson K, Winslow LA, Wise T, Zanotti L, Zarra C, Zhang GQ, Zhu BX, Zimmermann S, and Zucchelli S

Abstract

The CUORE experiment, a ton-scale cryogenic bolometer array, recently began operation at the Laboratori Nazionali del Gran Sasso in Italy. The array represents a significant advancement in this technology, and in this work we apply it for the first time to a high-sensitivity search for a lepton-number-violating process: ^{130}Te neutrinoless double-beta decay. Examining a total TeO&#95;{2} exposure of 86.3 kg yr, characterized by an effective energy resolution of (7.7±0.5)  keV FWHM and a background in the region of interest of (0.014±0.002)  counts/(keV kg yr), we find no evidence for neutrinoless double-beta decay. Including systematic uncertainties, we place a lower limit on the decay half-life of T&#95;{1/2}^{0ν}(^{130}Te)>1.3×10^{25}  yr (90% C.L.); the median statistical sensitivity of this search is 7.0×10^{24}  yr. Combining this result with those of two earlier experiments, Cuoricino and CUORE-0, we find T&#95;{1/2}^{0ν}(^{130}Te)>1.5×10^{25}  yr (90% C.L.), which is the most stringent limit to date on this decay. Interpreting this result as a limit on the effective Majorana neutrino mass, we find m&#95;{ββ}<(110-520)  meV, where the range reflects the nuclear matrix element estimates employed.

Published
2018
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6. Search for Neutrinoless Double-Beta Decay of (130)Te with CUORE-0.

Author

Alfonso K, Artusa DR, Avignone FT 3rd, Azzolini O, Balata M, Banks TI, Bari G, Beeman JW, Bellini F, Bersani A, Biassoni M, Brofferio C, Bucci C, Caminata A, Canonica L, Cao XG, Capelli S, Cappelli L, Carbone L, Cardani L, Casali N, Cassina L, Chiesa D, Chott N, Clemenza M, Copello S, Cosmelli C, Cremonesi O, Creswick RJ, Cushman JS, Dafinei I, Dally A, Dell'Oro S, Deninno MM, Di Domizio S, Di Vacri ML, Drobizhev A, Ejzak L, Fang DQ, Faverzani M, Fernandes G, Ferri E, Ferroni F, Fiorini E, Freedman SJ, Fujikawa BK, Giachero A, Gironi L, Giuliani A, Gorla P, Gotti C, Gutierrez TD, Haller EE, Han K, Hansen E, Heeger KM, Hennings-Yeomans R, Hickerson KP, Huang HZ, Kadel R, Keppel G, Kolomensky YG, Lim KE, Liu X, Ma YG, Maino M, Martinez M, Maruyama RH, Mei Y, Moggi N, Morganti S, Nisi S, Nones C, Norman EB, Nucciotti A, O'Donnell T, Orio F, Orlandi D, Ouellet JL, Pagliarone CE, Pallavicini M, Palmieri V, Pattavina L, Pavan M, Pedretti M, Pessina G, Pettinacci V, Piperno G, Pirro S, Pozzi S, Previtali E, Rosenfeld C, Rusconi C, Sala E, Sangiorgio S, Santone D, Scielzo ND, Sisti M, Smith AR, Taffarello L, Tenconi M, Terranova F, Tomei C, Trentalange S, Ventura G, Vignati M, Wagaarachchi SL, Wang BS, Wang HW, Wielgus L, Wilson J, Winslow LA, Wise T, Zanotti L, Zarra C, Zhang GQ, Zhu BX, and Zucchelli S

Abstract

We report the results of a search for neutrinoless double-beta decay in a 9.8 kg yr exposure of (130)Te using a bolometric detector array, CUORE-0. The characteristic detector energy resolution and background level in the region of interest are 5.1±0.3  keV FWHM and 0.058±0.004(stat)±0.002(syst)counts/(keV kg yr), respectively. The median 90% C.L. lower-limit half-life sensitivity of the experiment is 2.9×10(24)  yr and surpasses the sensitivity of previous searches. We find no evidence for neutrinoless double-beta decay of (130)Te and place a Bayesian lower bound on the decay half-life, T(1/2)(0ν)>2.7×10(24)  yr at 90% C.L. Combining CUORE-0 data with the 19.75 kg yr exposure of (130)Te from the Cuoricino experiment we obtain T(1/2)(0ν)>4.0×10(24)  yr at 90% C.L. (Bayesian), the most stringent limit to date on this half-life. Using a range of nuclear matrix element estimates we interpret this as a limit on the effective Majorana neutrino mass, m(ββ)<270-760  meV.

Published
2015
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7. Limit on neutrinoless ββ decay of 136Xe from the first phase of KamLAND-Zen and comparison with the positive claim in 76Ge.

Author

Gando A, Gando Y, Hanakago H, Ikeda H, Inoue K, Ishidoshiro K, Kato R, Koga M, Matsuda S, Mitsui T, Motoki D, Nakada T, Nakamura K, Obata A, Oki A, Ono Y, Otani M, Shimizu I, Shirai J, Suzuki A, Takemoto Y, Tamae K, Ueshima K, Watanabe H, Xu BD, Yamada S, Yoshida H, Kozlov A, Yoshida S, Banks TI, Freedman SJ, Fujikawa BK, Han K, O'Donnell T, Berger BE, Efremenko Y, Karwowski HJ, Markoff DM, Tornow W, Detwiler JA, Enomoto S, and Decowski MP

Abstract

We present results from the first phase of the KamLAND-Zen double-beta decay experiment, corresponding to an exposure of 89.5 kg yr of (136)Xe. We obtain a lower limit for the neutrinoless double-beta decay half-life of T(1/2)(0ν)>1.9×10(25) yr at 90% C.L. The combined results from KamLAND-Zen and EXO-200 give T(1/2)(0ν)>3.4×10(25) yr at 90% C.L., which corresponds to a Majorana neutrino mass limit of <(120-250) meV based on a representative range of available matrix element calculations. Using those calculations, this result excludes the Majorana neutrino mass range expected from the neutrinoless double-beta decay detection claim in (76)Ge, reported by a part of the Heidelberg-Moscow Collaboration, at more than 97.5% C.L.

Published
2013
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8. Measurement of muon capture on the proton to 1% precision and determination of the pseudoscalar coupling gP.

Author

Andreev VA, Banks TI, Carey RM, Case TA, Clayton SM, Crowe KM, Deutsch J, Egger J, Freedman SJ, Ganzha VA, Gorringe T, Gray FE, Hertzog DW, Hildebrandt M, Kammel P, Kiburg B, Knaack S, Kravtsov PA, Krivshich AG, Lauss B, Lynch KR, Maev EM, Maev OE, Mulhauser F, Petitjean C, Petrov GE, Prieels R, Schapkin GN, Semenchuk GG, Soroka MA, Tishchenko V, Vasilyev AA, Vorobyov AA, Vznuzdaev ME, and Winter P

Abstract

The MuCap experiment at the Paul Scherrer Institute has measured the rate Λ(S) of muon capture from the singlet state of the muonic hydrogen atom to a precision of 1%. A muon beam was stopped in a time projection chamber filled with 10-bar, ultrapure hydrogen gas. Cylindrical wire chambers and a segmented scintillator barrel detected electrons from muon decay. Λ(S) is determined from the difference between the μ(-) disappearance rate in hydrogen and the free muon decay rate. The result is based on the analysis of 1.2 × 10(10) μ(-) decays, from which we extract the capture rate Λ(S) = (714.9 ± 5.4(stat) ± 5.1(syst)) s(-1) and derive the proton's pseudoscalar coupling g(P)(q(0)(2) = -0.88 m(μ)(2)) = 8.06 ± 0.55.

Published
2013
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10. New limit on time-reversal violation in beta decay.

Author

Mumm HP, Chupp TE, Cooper RL, Coulter KP, Freedman SJ, Fujikawa BK, García A, Jones GL, Nico JS, Thompson AK, Trull CA, Wilkerson JF, and Wietfeldt FE

Abstract

We report the results of an improved determination of the triple correlation DP·(p(e)×p(v)) that can be used to limit possible time-reversal invariance in the beta decay of polarized neutrons and constrain extensions to the standard model. Our result is D=[-0.96±1.89(stat)±1.01(sys)]×10(-4). The corresponding phase between gA and gV is ϕAV=180.013°±0.028° (68% confidence level). This result represents the most sensitive measurement of D in nuclear β decay.

Published
2011
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11. Precision measurement of neutrino oscillation parameters with KamLAND.

Author

Abe S, Ebihara T, Enomoto S, Furuno K, Gando Y, Ichimura K, Ikeda H, Inoue K, Kibe Y, Kishimoto Y, Koga M, Kozlov A, Minekawa Y, Mitsui T, Nakajima K, Nakajima K, Nakamura K, Nakamura M, Owada K, Shimizu I, Shimizu Y, Shirai J, Suekane F, Suzuki A, Takemoto Y, Tamae K, Terashima A, Watanabe H, Yonezawa E, Yoshida S, Busenitz J, Classen T, Grant C, Keefer G, Leonard DS, McKee D, Piepke A, Decowski MP, Detwiler JA, Freedman SJ, Fujikawa BK, Gray F, Guardincerri E, Hsu L, Kadel R, Lendvai C, Luk KB, Murayama H, O'Donnell T, Steiner HM, Winslow LA, Dwyer DA, Jillings C, Mauger C, McKeown RD, Vogel P, Zhang C, Berger BE, Lane CE, Maricic J, Miletic T, Batygov M, Learned JG, Matsuno S, Pakvasa S, Foster J, Horton-Smith GA, Tang A, Dazeley S, Downum KE, Gratta G, Tolich K, Bugg W, Efremenko Y, Kamyshkov Y, Perevozchikov O, Karwowski HJ, Markoff DM, Tornow W, Heeger KM, Piquemal F, and Ricol JS

Abstract

The KamLAND experiment has determined a precise value for the neutrino oscillation parameter Deltam21(2) and stringent constraints on theta12. The exposure to nuclear reactor antineutrinos is increased almost fourfold over previous results to 2.44 x 10(32) proton yr due to longer livetime and an enlarged fiducial volume. An undistorted reactor nu[over]e energy spectrum is now rejected at >5sigma. Analysis of the reactor spectrum above the inverse beta decay energy threshold, and including geoneutrinos, gives a best fit at Deltam21(2)=7.58(-0.13)(+0.14)(stat) -0.15+0.15(syst) x 10(-5) eV2 and tan2theta12=0.56(-0.07)+0.10(stat) -0.06+0.10(syst). Local Deltachi2 minima at higher and lower Deltam21(2) are disfavored at >4sigma. Combining with solar neutrino data, we obtain Deltam21(2)=7.59(-0.21)+0.21 x 10(-5) eV2 and tan2theta12=0.47(-0.05)+0.06.

Published
2008
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12. Measurement of the muon capture rate in hydrogen gas and determination of the proton's pseudoscalar coupling gP.

Author

Andreev VA, Banks TI, Case TA, Chitwood DB, Clayton SM, Crowe KM, Deutsch J, Egger J, Freedman SJ, Ganzha VA, Gorringe T, Gray FE, Hertzog DW, Hildebrandt M, Kammel P, Kiburg B, Knaack S, Kravtsov PA, Krivshich AG, Lauss B, Lynch KL, Maev EM, Maev OE, Mulhauser F, Ozben CS, Petitjean C, Petrov GE, Prieels R, Schapkin GN, Semenchuk GG, Soroka MA, Tishchenko V, Vasilyev AA, Vorobyov AA, Vznuzdaev ME, and Winter P

Abstract

The rate of nuclear muon capture by the proton has been measured using a new technique based on a time projection chamber operating in ultraclean, deuterium-depleted hydrogen gas, which is key to avoiding uncertainties from muonic molecule formation. The capture rate from the hyperfine singlet ground state of the microp atom was obtained from the difference between the micro(-) disappearance rate in hydrogen and the world average for the micro(+) decay rate, yielding Lambda(S)=725.0+/-17.4 s(-1), from which the induced pseudoscalar coupling of the nucleon, g(P)(q(2)=-0.88m(2)(micro))=7.3+/-1.1, is extracted.

Published
2007
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13. Search for the invisible decay of neutrons with KamLAND.

Author

Araki T, Enomoto S, Furuno K, Gando Y, Ichimura K, Ikeda H, Inoue K, Kishimoto Y, Koga M, Koseki Y, Maeda T, Mitsui T, Motoki M, Nakajima K, Nakamura K, Ogawa H, Ogawa M, Owada K, Ricol JS, Shimizu I, Shirai J, Suekane F, Suzuki A, Tada K, Takeuchi S, Tamae K, Tsuda Y, Watanabe H, Busenitz J, Classen T, Djurcic Z, Keefer G, Leonard DS, Piepke A, Yakushev E, Berger BE, Chan YD, Decowski MP, Dwyer DA, Freedman SJ, Fujikawa BK, Goldman J, Gray F, Heeger KM, Hsu L, Lesko KT, Luk KB, Murayama H, O'Donnell T, Poon AW, Steiner HM, Winslow LA, Jillings C, Mauger C, McKeown RD, Vogel P, Zhang C, Lane CE, Miletic T, Guillian G, Learned JG, Maricic J, Matsuno S, Pakvasa S, Horton-Smith GA, Dazeley S, Hatakeyama S, Rojas A, Svoboda R, Dieterle BD, Detwiler J, Gratta G, Ishii K, Tolich N, Uchida Y, Batygov M, Bugg W, Efremenko Y, Kamyshkov Y, Kozlov A, Nakamura Y, Karwowski HJ, Markoff DM, Rohm RM, Tornow W, Wendell R, Chen MJ, Wang YF, and Piquemal F

Abstract

The Kamioka Liquid scintillator Anti-Neutrino Detector is used in a search for single neutron or two-neutron intranuclear disappearance that would produce holes in the -shell energy level of (12)C nuclei. Such holes could be created as a result of nucleon decay into invisible modes (inv), e.g., n--> 3v or nn--> 2v. The deexcitation of the corresponding daughter nucleus results in a sequence of space and time-correlated events observable in the liquid scintillator detector. We report on new limits for one- and two-neutron disappearance: tau(n--> inv) > 5.8 x 10(29) years and tau (nn--> inv) > 1.4 x 10(30) years at 90% C.L. These results represent an improvement of factors of approximately 3 and >10(4) and over previous experiments.

Published
2006
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14. Measurement of neutrino oscillation with KamLAND: evidence of spectral distortion.

Author

Araki T, Eguchi K, Enomoto S, Furuno K, Ichimura K, Ikeda H, Inoue K, Ishihara K, Iwamoto T, Kawashima T, Kishimoto Y, Koga M, Koseki Y, Maeda T, Mitsui T, Motoki M, Nakajima K, Ogawa H, Owada K, Ricol JS, Shimizu I, Shirai J, Suekane F, Suzuki A, Tada K, Tajima O, Tamae K, Tsuda Y, Watanabe H, Busenitz J, Classen T, Djurcic Z, Keefer G, McKinny K, Mei DM, Piepke A, Yakushev E, Berger BE, Chan YD, Decowski MP, Dwyer DA, Freedman SJ, Fu Y, Fujikawa BK, Goldman J, Gray F, Heeger KM, Lesko KT, Luk KB, Murayama H, Poon AW, Steiner HM, Winslow LA, Horton-Smith GA, Mauger C, McKeown RD, Vogel P, Lane CE, Miletic T, Gorham PW, Guillian G, Learned JG, Maricic J, Matsuno S, Pakvasa S, Dazeley S, Hatakeyama S, Rojas A, Svoboda R, Dieterle BD, Detwiler J, Gratta G, Ishii K, Tolich N, Uchida Y, Batygov M, Bugg W, Efremenko Y, Kamyshkov Y, Kozlov A, Nakamura Y, Gould CR, Karwowski HJ, Markoff DM, Messimore JA, Nakamura K, Rohm RM, Tornow W, Wendell R, Young AR, Chen MJ, Wang YF, and Piquemal F

Abstract

We present results of a study of neutrino oscillation based on a 766 ton/year exposure of KamLAND to reactor antineutrinos. We observe 258 nu (e) candidate events with energies above 3.4 MeV compared to 365.2+/-23.7 events expected in the absence of neutrino oscillation. Accounting for 17.8+/-7.3 expected background events, the statistical significance for reactor nu (e) disappearance is 99.998%. The observed energy spectrum disagrees with the expected spectral shape in the absence of neutrino oscillation at 99.6% significance and prefers the distortion expected from nu (e) oscillation effects. A two-neutrino oscillation analysis of the KamLAND data gives Deltam(2)=7.9(+0.6)(-0.5)x10(-5) eV(2). A global analysis of data from KamLAND and solar-neutrino experiments yields Deltam(2)=7.9(+0.6)(-0.5)x10(-5) eV(2) and tan((2)theta=0.40(+0.10)(-0.07), the most precise determination to date.

Published
2005
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15. Measurement of the beta-nu correlation using magneto-optically trapped 21Na.

Author

Scielzo ND, Freedman SJ, Fujikawa BK, and Vetter PA

Abstract

The beta-neutrino correlation coefficient, a(betanu), in 21Na is inferred from detecting the beta(+) and low-energy recoil daughter nucleus. 21Na is produced at the 88-Inch Cyclotron at Lawrence Berkeley National Laboratory and 800 000 atoms are maintained in a magneto-optical trap. From the measured time of flight of recoil ions in the presence of a drift electric field, we find a(betanu)=0.5243+/-0.0091. There may be a dependence on the trapped atom population. This and other systematic uncertainties are discussed.

Published
2004
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16. High sensitivity search for nu;e's from the sun and other sources at KamLAND.

Author

Eguchi K, Enomoto S, Furuno K, Ikeda H, Ikeda K, Inoue K, Ishihara K, Iwamoto T, Kawashima T, Kishimoto Y, Koga M, Koseki Y, Maeda T, Mitsui T, Motoki M, Nakajima K, Ogawa H, Owada K, Piquemal F, Shimizu I, Shirai J, Suekane F, Suzuki A, Tada K, Tajima O, Takayama T, Tamae K, Watanabe H, Busenitz J, Djurcic Z, McKinny K, Mei DM, Piepke A, Yakushev E, Berger BE, Chan YD, Decowski MP, Dwyer DA, Freedman SJ, Fu Y, Fujikawa BK, Goldman J, Heeger KM, Lesko KT, Luk KB, Murayama H, Nygren DR, Okada CE, Poon AW, Steiner HM, Winslow LA, Horton-Smith GA, Mauger C, McKeown RD, Tipton B, Vogel P, Lane CE, Miletic T, Gorham PW, Guillian G, Learned JG, Maricic J, Matsuno S, Pakvasa S, Dazeley S, Hatakeyama S, Svoboda R, Dieterle BD, DiMauro M, Detwiler J, Gratta G, Ishii K, Tolich N, Uchida Y, Batygov M, Bugg W, Efremenko Y, Kamyshkov Y, Kozlov A, Nakamura Y, Gould CR, Karwowski HJ, Markoff DM, Messimore JA, Nakamura K, Rohm RM, Tornow W, Young AR, Chen MJ, and Wang YF

Abstract

Data corresponding to a KamLAND detector exposure of 0.28 kton yr has been used to search for nu;(e)'s in the energy range 8.3

Published
2004
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17. Search for CPT-odd decays of positronium.

Author

Vetter PA and Freedman SJ

Abstract

We have limited a CPT-violating correlation in annihilations of polarized ortho-positronium. We searched for an asymmetry in the triple correlation s-->.(k-->(1)xk-->(2)), where k-->(1) and k-->(2) are the two largest photon momenta, and s--> is the spin of the positronium. Using the Gammasphere array of Compton-suppressed high-purity germanium detectors, we detected 2.65x10(7) events of ortho-Ps annihilation. The amplitude of a CPT-violating asymmetry in the data set is found to be 0.0026+/-0.0031, a factor of 6 smaller than previous experiments.

Published
2003
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18. Determination of the 8B neutrino spectrum.

Author

Winter WT, Freedman SJ, Rehm KE, Ahmad I, Greene JP, Heinz A, Henderson D, Janssens RV, Jiang CL, Moore EF, Mukherjee G, Pardo RC, Pennington T, Savard G, Schiffer JP, Seweryniak D, Zinkann G, and Paul M

Abstract

We have measured the total energy of the alpha particles following the beta decay of 8B by implanting 8B into a planar silicon surface barrier detector. Calibration was performed using alpha particles following the beta decay of 20Na, similarly implanted. The alpha spectrum is used to infer the 8B neutrino spectrum which is an important input in the interpretation of experiments that detect energetic neutrinos from the Sun. The alpha spectrum reported here is in disagreement with the previous best measurement which used two detectors in coincidence.

Published
2003
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19. First results from KamLAND: evidence for reactor antineutrino disappearance.

Author

Eguchi K, Enomoto S, Furuno K, Goldman J, Hanada H, Ikeda H, Ikeda K, Inoue K, Ishihara K, Itoh W, Iwamoto T, Kawaguchi T, Kawashima T, Kinoshita H, Kishimoto Y, Koga M, Koseki Y, Maeda T, Mitsui T, Motoki M, Nakajima K, Nakajima M, Nakajima T, Ogawa H, Owada K, Sakabe T, Shimizu I, Shirai J, Suekane F, Suzuki A, Tada K, Tajima O, Takayama T, Tamae K, Watanabe H, Busenitz J, Djurcic Z, McKinny K, Mei DM, Piepke A, Yakushev E, Berger BE, Chan YD, Decowski MP, Dwyer DA, Freedman SJ, Fu Y, Fujikawa BK, Heeger KM, Lesko KT, Luk KB, Murayama H, Nygren DR, Okada CE, Poon AW, Steiner HM, Winslow LA, Horton-Smith GA, McKeown RD, Ritter J, Tipton B, Vogel P, Lane CE, Miletic T, Gorham PW, Guillian G, Learned JG, Maricic J, Matsuno S, Pakvasa S, Dazeley S, Hatakeyama S, Murakami M, Svoboda RC, Dieterle BD, DiMauro M, Detwiler J, Gratta G, Ishii K, Tolich N, Uchida Y, Batygov M, Bugg W, Cohn H, Efremenko Y, Kamyshkov Y, Kozlov A, Nakamura Y, De Braeckeleer L, Gould CR, Karwowski HJ, Markoff DM, Messimore JA, Nakamura K, Rohm RM, Tornow W, Young AR, and Wang YF

Abstract

KamLAND has measured the flux of nu;(e)'s from distant nuclear reactors. We find fewer nu;(e) events than expected from standard assumptions about nu;(e) propagation at the 99.95% C.L. In a 162 ton.yr exposure the ratio of the observed inverse beta-decay events to the expected number without nu;(e) disappearance is 0.611+/-0.085(stat)+/-0.041(syst) for nu;(e) energies >3.4 MeV. In the context of two-flavor neutrino oscillations with CPT invariance, all solutions to the solar neutrino problem except for the "large mixing angle" region are excluded.

Published
2003
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20. Search for narrow sum-energy lines in electron-positron pair emission from heavy-ion collisions near the Coulomb barrier.

Author

Ahmad I I, Austin SM, Back BB, Betts RR, Calaprice FP, Chan KC, Chishti A, Chowdhury P, Conner C, Dunford RW, Fox JD, Freedman SJ, Freer M, Gazes SB, Hallin AL, Happ T, Henderson D, Kaloskamis NI, Kashy E, Kutschera W, Last J, Lister CJ, Liu M, Maier MR, Mercer DJ, Mikolas D, Perera PA, Rhein MD, Roa DE, Schiffer JP, Trainor TA, Wilt P, Winfield JS, Wolanski M, Wolfs FL, Wuosmaa AH, Xu G, Young A, and Yurkon JE

Published
1995
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26. Limits on nu -bar micro--> nu -bare oscillations.

Author

Durkin LS, Harper RW, Ling TY, Mitchell JW, Romanowski TA, Smith ES, Timko M, Freedman SJ, Napolitano J, Fujikawa BK, McKeown R, Lesko KT, Choi WC, Fazely A, Imlay RL, Metcalf WJ, Carlini RD, Donahue JB, Garvey GT, and Sandberg VD

Published
1988
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