共查询到20条相似文献,搜索用时 15 毫秒
1.
Bai JZ Bardon O Becker-Szendy RA Burnett TH Campbell JS Chen SJ Chen SM Chen YQ Cheng ZD Coller JA Cowan RF Cui HC Cui XZ Ding HL Du ZZ Dunwoodie W Fang C Fero MJ Gao ML Gao SQ Gao WX Gao YN Gu JH Gu SD Gu WX Guo YN Guo YY Han Y Hatanaka M He J Hitlin DG Hu GY Hu T Huang DQ Huang YZ Izen JM Jia QP Jiang CH Jiang ZJ Johnson AS Jones LA Kelsey MH Lai YF Lang PF Lankford A Li F Li J Li PQ Li QM Li RB Li W Li WD Li WG Li YS Lin SZ Liu HM Liu Q Liu RG Liu Y Lowery B Lu JG Ma DH Ma EC Ma JM 《Physical review letters》1992,69(21):3021-3024
2.
Belous K Shapkin M Sokolov A Abe K Abe K Adachi I Aihara H Anipko D Arinstein K Aulchenko V Aushev T Bakich AM Barberio E Bay A Bedny I Bitenc U Bizjak I Blyth S Bondar A Bozek A Bracko M Browder TE Chang MC Chen A Chen KF Chen WT Cheon BG Chistov R Choi Y Choi YK Cole S Dalseno J Drutskoy A Eidelman S Epifanov D Fratina S Fujikawa M Gabyshev N Gershon T Gokhroo G Golob B Ha H Haba J Hasegawa Y Hayasaka K Hayashii H Hazumi M Heffernan D Hokuue T Hoshi Y Hou S Hou WS Iijima T Ikado K Imoto A 《Physical review letters》2007,99(1):011801
The mass of the tau lepton has been measured in the decay mode tau-->3pinutau using a pseudomass technique. The result obtained from 414 fb-1 of data collected with the Belle detector is Mtau=[1776.61+/-0.13(stat)+/-0.35(sys)] MeV/c2. The upper limit on the relative mass difference between positive and negative tau leptons is |Mtau+-Mtau-|/Mtau<2.8 x 10-4 at 90% confidence level. 相似文献
3.
Battle M Ernst J Kwon Y Roberts S Thorndike EH Wang CH Dominick J Lambrecht M Sanghera S Shelkov V Skwarnicki T Stroynowski R Volobouev I Wei G Zadorozhny P Artuso M Goldberg M He D Horwitz N Kennett R Mountain R Moneti GC Muheim F Mukhin Y Playfer S Rozen Y Stone S Thulasidas M Vasseur G Zhu G Bartelt J Csorna SE Egyed Z Jain V Kinoshita K Edwards KW Ogg M Britton DI Hyatt ER MacFarlane DB Patel PM Akerib DS Barish B Chadha M Chan S Cowen DF Eigen G Miller JS O'Grady C Urheim J Weinstein AJ 《Physical review letters》1994,73(8):1079-1083
4.
Akerib DS Barish B Chadha M Cowen DF Eigen G Miller JS Urheim J Weinstein AJ Acosta D Masek G Ong B Paar H Sivertz M Bean A Gronberg J Kutschke R Menary S Morrison RJ Nelson HN Richman JD Tajima H Schmidt D Sperka D Witherell MS Procario M Yang S Daoudi M Ford WT Johnson DR Lingel K Lohner M Rankin P Smith JG Alexander JP Bebek C Berkelman K Besson D Browder TE Cassel DG Coffman DM Drell PS Ehrlich R Galik RS Garcia-Sciveres M Geiser B Gittelman B Gray SW Hartill DL Heltsley BK Honscheid K 《Physical review letters》1992,69(25):3610-3614
5.
Balest R Daoudi M Ford WT Johnson DR Lingel K Lohner M Rankin P Smith JG Alexander JP Bebek C Berkelman K Besson D Browder TE Cassel DG Cho HA Coffman DM Drell PS Ehrlich R Galik RS Garcia-Sciveres M Geiser B Gittelman B Gray SW Hartill DL Heltsley BK Honscheid K Jones CD Kandaswamy J Katayama N Kim PC Kreinick DL Ludwig GS Masui J Mevissen J Mistry NB Ng CR Nordberg E Ogg M O'Grady C Patterson JR Peterson D Riley D Sapper M Selen M Worden H Worris M Würthwein F Avery P Freyberger A Rodriguez J 《Physical review D: Particles and fields》1993,47(9):R3671-R3675
6.
7.
Savage MJ 《Physical review D: Particles and fields》1989,40(9):3116-3117
8.
《JETP Letters》2007,85(8):347-352
A precise τ lepton mass measurement performed at the VEPP-4M collider with the KEDR detector is reported. The mass value is
evaluated from the τ+τ− cross section behavior around the production threshold. The result based on 6.7 pb−1 of data is m
τ = 1776.81
−0.23
+0.25
± 0.15 MeV. Using 0.8 pb−1 of data collected at the ψ′ peak, we have also determined that Γ
ee
B
ττ(ψ′) = 9.0 ± 2.6 eV.
The text was submitted by the authors in English. 相似文献
9.
10.
Ammar R Baringer P Coppage D Davis R Kelly M Kwak N Lam H Ro S Kubota Y Lattery M Nelson JK Perticone D Poling R Schrenk S Wang R Alam MS Kim IJ Nemati B Romero V Sun CR Wang P Zoeller MM Crawford G Fulton R Gan KK Kagan H Kass R Lee J Malchow R Morrow F Sung MK Whitmore J Wilson P Butler F Fu X Kalbfleisch G Lambrecht M Skubic P Snow J Bortoletto D Brown DN Dominick J McIlwain RL Miller DH Modesitt M Shibata EI Schaffner SF Shipsey IP Battle M Ernst J Kroha H Roberts S Sparks K Thorndike EH 《Physical review D: Particles and fields》1992,45(11):3976-3985
11.
Bartelt J Csorna SE Egyed Z Jain V Kinoshita K Barish B Chadha M Chan S Cowen DF Eigen G Miller JS O'Grady C Urheim J Weinstein AJ Acosta D Athanas M Masek G Paar HP Sivertz M Gronberg J Kutschke R Menary S Morrison RJ Nakanishi S Nelson HN Nelson TK Qiao C Richman JD Ryd A Tajima H Sperka D Witherell MS Procario M Balest R Cho K Daoudi M Ford WT Johnson DR Lingel K Lohner M Rankin P Smith JG Alexander JP Bebek C Berkelman K Bloom K Browder TE Cassel DG Cho HA Coffman DM Crowcroft DS Drell PS 《Physical review letters》1994,73(14):1890-1894
12.
Bowcock T Kinoshita K Pipkin FM Procario M Wilson R Wolinski J Xiao D Ammar R Baringer P Coppage D Haas P Lam H Jawahery A Park CH Kubota Y Nelson JK Perticone D Poling R Chen W Dominick J McIlwain RL Miller DH Ng CR Schaffner SF Shibata EI Yao W Sparks K Thorndike EH Alam MS Kim IJ Li WC Lou XC Sun CR Fulton R Hempstead M Jensen T Johnson DR Kagan H Kass R Morrow F Whitmore J Bortoletto D Goldberg M Horwitz N Mestayer MD Moneti GC Sharma V Shipsey IP Skwarnicki T Csorna SE Letson T Alexander J 《Physical review D: Particles and fields》1990,41(3):805-808
13.
M.Bischofberger 《中国物理C(英文版)》2010,34(6):902-906
We report recent results of searches for lepton flavor violation and second class current in decays of τ leptons using the data sample collected in the Belle experiment at the KEKB electron-positron asymmetric-energy collider. 相似文献
14.
Gibaut D Kinoshita K Barish B Chadha M Chan S Cowen DF Eigen G Miller JS O'Grady C Urheim J Weinstein AJ Acosta D Athanas M Masek G Paar HP Gronberg J Kutschke R Menary S Morrison RJ Nakanishi S Nelson HN Nelson TK Qiao C Richman JD Ryd A Tajima H Sperka D Witherell MS Procario M Balest R Cho K Daoudi M Ford WT Johnson DR Lingel K Lohner M Rankin P Smith JG Alexander JP Bebek C Berkelman K Bloom K Browder TE Cassel DG Cho HA Coffman DM Crowcroft DS Drell PS Ehrlich R Gaidarev P Galik RS 《Physical review letters》1994,73(7):934-938
15.
M. Bischofberger 《中国物理 C》2010,34(6):902-906
We report recent results of searches for lepton flavor violation and second class current in decays of τ leptons using the data sample collected in the Belle experiment at the KEKB electron-positron asymmetricenergy collider. 相似文献
16.
17.
Viehhauser G Wang JC Wolf A Wu J Csorna SE McLean KW Marka S Xu Z Godang R Kinoshita K Lai IC Schrenk S Bonvicini G Cinabro D Greene R Perera LP Zhou GJ Chan S Eigen G Lipeles E Schmidtler M Shapiro A Sun WM Urheim J Weinstein AJ Wurthwein F 《Physical review letters》2000,84(5):830-834
Using 4.68 fb(-1) of e(+)e(-) annihilation data collected with the CLEO II detector at the Cornell Electron Storage Ring, we have studied tau radiative decays tau(-)-->nu(tau)&mgr;(-)nu;(&mgr;)gamma and tau(-)-->nu(tau)e(-)nu;(e)gamma. For a 10 MeV minimum photon energy in the tau rest frame, the branching fraction for radiative tau decay to a muon or electron is measured to be (3.61+/-0.16+/-0. 35)x10(-3) or (1.75+/-0.06+/-0.17)x10(-2), respectively. The branching fractions are in agreement with standard model theoretical predictions. 相似文献
18.
Braaten E 《Physical review letters》1988,60(16):1606-1609
19.
We present a method for obtaining bounds on the magnetic moment of the lepton. In order to do this, we study the radiative decayW as a function of the anomalous magnetic moment of the ,a
. One can obtain bounds as good asa
< 4.05×10–2, 2.25×10–2, 4.5×10–3, and 2.5×10–3 at the present Fermilab, future Fermilab, SSC, and LHC, respectively. 相似文献
20.
《Nuclear Physics B》1998,523(3):439-449
We calculate the squared matrix element for the process e+e− → τ+τ−γ allowing for anomalous magnetic and electric dipole moments at the ττγ vertex. No interferences are neglected and no approximations of light fermion masses are made. We show that anomalous moments affect not only the cross section, but also the shape of the photon energy and angular distributions. We also demonstrate that in the case of the anomalous magnetic dipole moment, the contribution from interference involving Standard Model and anomalous amplitudes is significant compared to the contribution from anomalous amplitudes alone. A program to perform the calculation is available and it may be employed as a Monte Carlo generator. 相似文献