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1.
Phys Rev Lett ; 126(12): 121801, 2021 Mar 26.
Artigo em Inglês | MEDLINE | ID: mdl-33834796

RESUMO

The rare decay K_{L}→π^{0}νν[over ¯] was studied with the dataset taken at the J-PARC KOTO experiment in 2016, 2017, and 2018. With a single event sensitivity of (7.20±0.05_{stat}±0.66_{syst})×10^{-10}, three candidate events were observed in the signal region. After unveiling them, contaminations from K^{±} and scattered K_{L} decays were studied, and the total number of background events was estimated to be 1.22±0.26. We conclude that the number of observed events is statistically consistent with the background expectation. For this dataset, we set an upper limit of 4.9×10^{-9} on the branching fraction of K_{L}→π^{0}νν[over ¯] at the 90% confidence level.

2.
Phys Rev Lett ; 122(2): 021802, 2019 Jan 18.
Artigo em Inglês | MEDLINE | ID: mdl-30720307

RESUMO

A search for the rare decay K_{L}→π^{0}νν[over ¯] was performed. With the data collected in 2015, corresponding to 2.2×10^{19} protons on target, a single event sensitivity of (1.30±0.01_{stat}±0.14_{syst})×10^{-9} was achieved and no candidate events were observed. We set an upper limit of 3.0×10^{-9} for the branching fraction of K_{L}→π^{0}νν[over ¯] at the 90% confidence level (C.L.), which improved the previous limit by almost an order of magnitude. An upper limit for K_{L}→π^{0}X^{0} was also set as 2.4×10^{-9} at the 90% C.L., where X^{0} is an invisible boson with a mass of 135 MeV/c^{2}.

3.
Rev Sci Instrum ; 88(6): 063105, 2017 Jun.
Artigo em Inglês | MEDLINE | ID: mdl-28667968

RESUMO

We developed a fast X-ray detector system for nuclear resonant scattering (NRS) experiments. Our system employs silicon avalanche photo-diode (Si-APD) as a fast X-ray sensor. The system is able to acquire both timing and energy of a single X-ray photon simultaneously in a high rate condition, 106 counts per second for one Si-APD. The performance of the system was investigated in SPring-8, a synchrotron radiation facility in Japan. Good time resolution of 120 ps (FWHM) was achieved with a slight tail distribution in the time spectrum by a level of 10-9 at 1 ns apart from the peak. Using this system, we successfully observed the NRS from the 26.27-keV level of mercury-201, which has a half-life of 630(50) ps. We also demonstrated the reduction of background events caused by radioactive decays in a radioactive sample by discriminating photon energy.

10.
Phys Rev Lett ; 102(5): 051802, 2009 Feb 06.
Artigo em Inglês | MEDLINE | ID: mdl-19257503

RESUMO

We performed a search for a light pseudoscalar particle X in the decay K_{L};{0}-->pi;{0}pi;{0}X, X-->gammagamma with the E391a detector at KEK. Such a particle with a mass of 214.3 MeV/c;{2} was suggested by the HyperCP experiment. We found no evidence for X and set an upper limit on the product branching ratio for K_{L};{0}-->pi;{0}pi;{0}X, X-->gammagamma of 2.4x10;{-7} at the 90% confidence level. Upper limits on the branching ratios in the mass region of X from 194.3 to 219.3 MeV/c;{2} are also presented.

11.
Phys Rev Lett ; 100(20): 201802, 2008 May 23.
Artigo em Inglês | MEDLINE | ID: mdl-18518524

RESUMO

We performed a search for the K L0-->pi0nu nu[over] decay at the KEK 12-GeV proton synchrotron. No candidate events were observed. An upper limit on the branching ratio for the decay was set to be 6.7 x 10(-8) at the 90% confidence level.

12.
Biochem Biophys Res Commun ; 285(5): 1237-43, 2001 Aug 03.
Artigo em Inglês | MEDLINE | ID: mdl-11478789

RESUMO

K252a, an indrocarbazole derivative and protein kinase inhibitor, is reported to promote myogenic differentiation in C2 mouse myoblasts. We examined the effects of K252a on QM-RSV cells, quail myoblasts transformed with a temperature-sensitive mutant of Rous sarcoma virus. K252a promoted myotube formation of QM-RSV cells. Presumptive QM-RSV cells also formed multinucleated cells when exposed to K252a. However, the expression of myogenin, a muscle regulatory factor, was not stimulated in the presence of the drug, suggesting that it promotes membrane fusion but not myogenic differentiation. To confirm the promotion of membrane fusion by K252a, presumptive C2 cells, which are strongly resistant to HVJ-mediated cell fusion, were fused by HVJ (Sendai virus) after K252a treatment. Presumptive C2 cells treated with K252a fused with HVJ, demonstrating that K252a causes the cells to enter a fusion-capable state. The amount of membrane cholesterol, a factor that decreases membrane fluidity, fell in K252a-treated C2 cells. The results suggest that a decrease of membrane cholesterol is a cause of the change that renders myoblast membrane susceptible to fusion in the presence of K252a.


Assuntos
Carbazóis/farmacologia , Membrana Celular/efeitos dos fármacos , Fusão de Membrana/efeitos dos fármacos , Músculo Esquelético/efeitos dos fármacos , Animais , Diferenciação Celular/efeitos dos fármacos , Fusão Celular/métodos , Linhagem Celular Transformada , Membrana Celular/química , Membrana Celular/metabolismo , Células Cultivadas , Colesterol/análise , Colesterol/metabolismo , Imunofluorescência , Alcaloides Indólicos , Fluidez de Membrana/efeitos dos fármacos , Fusão de Membrana/fisiologia , Camundongos , Camundongos Endogâmicos C3H , Músculo Esquelético/citologia , Músculo Esquelético/metabolismo , Miogenina/biossíntese , Codorniz , Temperatura
13.
Phys Rev Lett ; 92(5): 054802, 2004 Feb 06.
Artigo em Inglês | MEDLINE | ID: mdl-14995314

RESUMO

For high luminosity in electron-positron linear colliders, it is essential to generate low vertical emittance beams. We report on the smallest vertical emittance achieved in single-bunch-mode operation of the Accelerator Test Facility, which satisfies the requirement of the x-band linear collider. The emittances were measured with a laser-wire beam-profile monitor installed in the damping ring. The bunch length and the momentum spread of the beam were also recorded under the same conditions. The smallest vertical rms emittance measured at low intensity is 4 pm at a beam energy of 1.3 GeV, which corresponds to the normalized emittance of 1.0x1.0(-8) m. It increases by a factor of 1.5 for a bunch intensity of 10(10) electrons. The measured data agreed to the calculation of intrabeam scattering within much better than a factor of 2.

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