2,313 research outputs found

    The HERA-B Ring Imaging Cherenkov Counter

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    The HERA-B RICH uses a radiation path length of 2.8 m in C_4F_10 gas and a large 24 square meters spherical mirror for imaging Cherenkov rings. The photon detector consists of 2240 Hamamatsu multi-anode photomultipliers with about 27000 channels. A 2:1 reducing two-lens telescope in front of each PMT increases the sensitive area at the expense of increased pixel size, resulting in a contribution to the resolution which roughly matches that of dispersion. The counter was completed in January of 1999, and its performance has been steady and reliable over the years it has been in operation. The design performance of the RICH was fully reached: the average number of detected photons in the RICH for a beta=1 particle was found to be 33 with a single hit resolution of 0.7 mrad and 1 mrad in the fine and coarse granularity regions, respectively.Comment: 29 pages, 23 figure

    Tests of a proximity focusing RICH with aerogel as radiator

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    Using aerogel as radiator and multianode PMTs for photon detection, a proximity focusing Cherenkov ring imaging detector has been constructed and tested in the KEK π\pi2 beam. The aim is to experimentally study the basic parameters such as resolution of the single photon Cherenkov angle and number of detected photons per ring. The resolution obtained is well approximated by estimates of contributions from pixel size and emission point uncertainty. The number of detected photons per Cherenkov ring is in good agreement with estimates based on aerogel and detector characteristics. The values obtained turn out to be rather low, mainly due to Rayleigh scattering and to the relatively large dead space between the photocathodes. A light collection system or a higher fraction of the photomultiplier active area, together with better quality aerogels are expected to improve the situation. The reduction of Cherenkov yield, for charged particle impact in the vicinity of the aerogel tile side wall, has also been measured.Comment: 4 pages, 8 figure

    A novel type of proximity focusing RICH counter with multiple refractive index aerogel radiator

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    A proximity focusing ring imaging Cherenkov detector, with the radiator consisting of two or more aerogel layers of different refractive indices, has been tested in 1-4 GeV/c pion beams at KEK. Essentially, a multiple refractive index aerogel radiator allows for an increase in Cherenkov photon yield on account of the increase in overall radiator thickness, while avoiding the simultaneous degradation in single photon angular resolution associated with the increased uncertainty of the emission point. With the refractive index of consecutive layers suitably increasing in the downstream direction, one may achieve overlapping of the Cherenkov rings from a single charged particle. In the opposite case of decreasing refractive index, one may obtain well separated rings. In the former combination an approximately 40% increase in photon yield is accompanied with just a minor degradation in single photon angular resolution. The impact of this improvement on the pion/kaon separation at the upgraded Belle detector is discussed.Comment: submitted to Nucl. Instr. Meth.

    Aging Studies for the Large Honeycomb Drift Tube System of the Outer Tracker of HERA-B

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    The HERA-B Outer Tracker consists of drift tubes folded from polycarbonate foil and is operated with Ar/CF4/CO2 as drift gas. The detector has to stand radiation levels which are similar to LHC conditions. The first prototypes exposed to radiation in HERA-B suffered severe radiation damage due to the development of self-sustaining currents (Malter effect). In a subsequent extended R&D program major changes to the original concept for the drift tubes (surface conductivity, drift gas, production materials) have been developed and validated for use in harsh radiation environments. In the test program various aging effects (like Malter currents, gain loss due to anode aging and etching of the anode gold surface) have been observed and cures by tuning of operation parameters have been developed.Comment: 14 pages, 6 figures, to be published in the Proceedings of the International Workshop On Aging Phenomena In Gaseous Detectors, 2-5 Oct 2001, Hamburg, German

    Search for CP Violation in the Decays D0KS0P0D^0\rightarrow K^0_S P^0

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    We have searched for CP violation in the decays D0KS0P0D^0\rightarrow K^0_S P^0 where P0P^0 denotes a neutral pseudo-scalar meson which is either a π0\pi^0, η\eta, or η\eta' using KEKB asymmetric-energy e+ee^+e^- collision data corresponding to an integrated luminosity of 791 fb1^{-1} collected with the Belle detector. No evidence of significant CP violation is observed. We report the most precise CP asymmetry measurement in the decay D0KS0π0D^0\rightarrow K^0_S\pi^0 to date: ACPD0KS0π0=(0.28±0.19±0.10)A_{CP}^{D^0\rightarrow K^0_S\pi^0}=(-0.28\pm0.19\pm0.10)%. We also report the first measurements of CP asymmetries in the decays D0KS0ηD^0\rightarrow K^0_S\eta and D0KS0ηD^0\rightarrow K^0_S\eta': ACPD0KS0η=(+0.54±0.51±0.16)A_{CP}^{D^0\rightarrow K^0_S\eta}=(+0.54\pm0.51\pm0.16)% and ACPD0KS0η=(+0.98±0.67±0.14)A_{CP}^{D^0\rightarrow K^0_S\eta'}=(+0.98\pm0.67\pm0.14)%, respectively

    Search for the Lepton-Flavor-Violating Decay τμη\tau^- \to \mu^- \eta at Belle

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    We have searched for the Lepton Flavor Violating decay τμη\tau^- \to \mu^- \eta using a data sample of 84.3 fb1^{-1} accumulated with the Belle detector at KEK. The η\eta-meson was detected through the decay modes: ηγγ\eta \to \gamma\gamma and π+ππ0\pi^+\pi^-\pi^0. No signal candidates are found, and we obtain an upper limit for the branching fraction B(τμη)<3.4×107{\cal B}(\tau^- \to \mu^- \eta)<3.4\times 10^{-7} at the 90% confidence level.Comment: Submitted to Phys.Rev.Let

    Observation of Bs0J/ψf0(980)B_s^0\to J/\psi f_0(980) and Evidence for Bs0J/ψf0(1370)B_s^0\to J/\psi f_0(1370)

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    We report the first observation of Bs0J/ψf0(980)B_s^0\to J/\psi f_0(980) and first evidence for Bs0J/ψf0(1370)B_s^0\to J/\psi f_0(1370), which are CP eigenstate decay modes. These results are obtained from 121.4  fb1121.4\;\mathrm{fb}^{-1} of data collected at the Υ(5S)\Upsilon(5S) resonance with the Belle detector at the KEKB e+ee^+e^- collider. We measure the branching fractions B(Bs0J/ψf0(980);f0(980)π+π)=(1.160.19+0.31(stat.)0.17+0.15(syst.)0.18+0.26(NBs()Bˉs()))×104\mathcal{B}(B_s^0\to J/\psi f_0(980);f_0(980)\to\pi^+\pi^-)=(1.16^{+0.31}_{-0.19}(\mathrm{stat.})^{+0.15}_{-0.17}(\mathrm{syst.})^{+0.26}_{-0.18}(N_{B_s^{(*)}\bar B_s^{(*)}})) \times 10^{-4} with a significance of 8.4σ8.4\sigma, and B(Bs0J/ψf0(1370);f0(1370)π+π)=(0.340.14+0.11(stat.)0.02+0.03(syst.)0.05+0.08(NBs()Bˉs()))×104\mathcal{B}(B_s^0\to J/\psi f_0(1370);f_0(1370)\to\pi^+\pi^-)=(0.34^{+0.11}_{-0.14}(\mathrm{stat.})^{+0.03}_{-0.02}(\mathrm{syst.})^{+0.08}_{-0.05}(N_{B_s^{(*)}\bar B_s^{(*)}})) \times 10^{-4} with a significance of 4.2σ4.2\sigma. The last error listed is due to uncertainty in the number of produced Bs()Bˉs()B_s^{(*)}\bar B_s^{(*)} pairs.Comment: 5 pages, 2 figures, 2 tables, published in PR

    Search for the X(1812) in B±K±ωϕB^{\pm} \to K^{\pm} \omega \phi

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    We report on a search for the X(1812) state in the decay B±K±ωϕB^{\pm} \to K^{\pm} \omega \phi with a data sample of 657×106657\times10^6 BBˉB\bar{B} pairs collected with the Belle detector at the KEKB e+ee^+e^- collider. No significant signal is observed. An upper limit B(B±K±X(1812),X(1812)ωϕ)<3.2×107{\cal B}(B^{\pm} \to K^{\pm} X(1812),X(1812) \to \omega \phi)<3.2\times 10^{-7} (90% C.L.) is determined. We also constrain the three-body decay branching fraction to be B(B±K±ωϕ){\cal B}(B^{\pm} \to K^{\pm} \omega \phi) << 1.9 ×106\times 10^{-6} (90% C.L.).Comment: 5pages,2 figures(3 figure files). submitted to PRD(RC

    Measurement of Inclusive Radiative B-meson Decays with a Photon Energy Threshold of 1.7 GeV

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    Using 605/fb of data collected at the Upsilon(4S) resonance we present a measurement of the inclusive radiative B-meson decay channel, B to X_s gamma. For the lower photon energy thresholds of 1.7, 1.8, 1.9 and 2.0GeV, as defined in the rest frame of the B-meson, we measure the partial branching fraction and the mean and variance of the photon energy spectrum. At the 1.7GeV threshold we obtain the partial branching fraction BF(B to X_s gamma) = (3.45 +/- 0.15 +/- 0.40) x 10^-4, where the errors are statistical and systematic.Comment: 9 pages, 3 figures, 2 table
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