Photon transitions in Upsilon(2S) and Upsilon(3S) decays.

نویسندگان

  • M Artuso
  • C Boulahouache
  • S Blusk
  • J Butt
  • E Dambasuren
  • O Dorjkhaidav
  • J Li
  • N Menaa
  • R Mountain
  • H Muramatsu
  • R Nandakumar
  • R Redjimi
  • R Sia
  • T Skwarnicki
  • S Stone
  • J C Wang
  • K Zhang
  • S E Csorna
  • G Bonvicini
  • D Cinabro
  • M Dubrovin
  • A Bornheim
  • S P Pappas
  • A J Weinstein
  • J L Rosner
  • R A Briere
  • G P Chen
  • T Ferguson
  • G Tatishvili
  • H Vogel
  • M E Watkins
  • N E Adam
  • J P Alexander
  • K Berkelman
  • D G Cassel
  • V Crede
  • J E Duboscq
  • K M Ecklund
  • R Ehrlich
  • L Fields
  • R S Galik
  • L Gibbons
  • B Gittelman
  • R Gray
  • S W Gray
  • D L Hartill
  • B K Heltsley
  • D Hertz
  • L Hsu
  • C D Jones
  • J Kandaswamy
  • D L Kreinick
  • V E Kuznetsov
  • H Mahlke-Krüger
  • T O Meyer
  • P U E Onyisi
  • J R Patterson
  • D Peterson
  • J Pivarski
  • D Riley
  • A Ryd
  • A J Sadoff
  • H Schwarthoff
  • M R Shepherd
  • S Stroiney
  • W M Sun
  • J G Thayer
  • D Urner
  • T Wilksen
  • M Weinberger
  • S B Athar
  • P Avery
  • L Breva-Newell
  • R Patel
  • V Potlia
  • H Stoeck
  • J Yelton
  • P Rubin
  • C Cawlfield
  • B I Eisenstein
  • G D Gollin
  • I Karliner
  • D Kim
  • N Lowrey
  • P Naik
  • C Sedlack
  • M Selen
  • J J Thaler
  • J Williams
  • J Wiss
  • K W Edwards
  • D Besson
  • T K Pedlar
  • D Cronin-Hennessy
  • K Y Gao
  • D T Gong
  • Y Kubota
  • B W Lang
  • S Z Li
  • R Poling
  • A W Scott
  • A Smith
  • C J Stepaniak
  • S Dobbs
  • Z Metreveli
  • K K Seth
  • A Tomaradze
  • P Zweber
  • J Ernst
  • A H Mahmood
  • K Arms
  • K K Gan
  • H Severini
  • D M Asner
  • S A Dytman
  • W Love
  • S Mehrabyan
  • J A Mueller
  • V Savinov
  • Z Li
  • A Lopez
  • H Mendez
  • J Ramirez
  • G S Huang
  • D H Miller
  • V Pavlunin
  • B Sanghi
  • E I Shibata
  • I P J Shipsey
  • G S Adams
  • M Chasse
  • M Cravey
  • J P Cummings
  • I Danko
  • J Napolitano
  • C S Park
  • W Park
  • J B Thayer
  • E H Thorndike
  • T E Coan
  • Y S Gao
  • F Liu
  • R Stroynowski
چکیده

We have studied the inclusive photon spectra in Upsilon(2S) and Upsilon(3S) decays using a large statistics data sample obtained with the CLEO III detector. We present the most precise measurements of electric dipole (E1) photon transition rates and photon energies for Upsilon(2S) --> gammachi(bJ)(1P) and Upsilon(3S) --> gammachi(bJ)(2P) (J = 0, 1, 2). We measure the rate for a rare E1 transition Upsilon(3S) --> gammachi(b0)(1P) for the first time. We also set upper limits on the rates for the hindered magnetic dipole (M1) transitions to the eta(b)(1S) and eta(b)(2S) states.

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Proposal for Testing Lepton Univerality in Upsilon Decays at a B Factory Running at Υ(3s) *

A proposal is presented for detecting new physics at a B factory running at the Υ(3S) resonance by testing lepton universality to the few percent level in the leptonic decays of the Υ(1S) and Υ(2S) resonances tagged by the dipion in the chain decay: Υ(3S) → π + π

متن کامل

Observation of Upsilon(2S)-->etaUpsilon(1S) and search for related transitions.

We report the first observation of Upsilon(2S)-->etaUpsilon(1S), with a branching fraction B=(2.1(-0.6)+0.7(stat)+/-0.3(syst)) x 10(-4) and a statistical significance 5.3sigma. Data were acquired with the CLEO III detector at the CESR e+e(-) symmetric collider. This is the first process observed involving a b-quark spin flip. For related transitions, 90% confidence limits in units of 10(-4) are...

متن کامل

Observation of the Hadronic transitions chi(b1,2)(2P)-->omegaUpsilon(1S).

The CLEO Collaboration has made the first observations of hadronic transitions among bottomonium (bbmacr;) states other than the dipion transitions among Upsilon(nS) states. In our study of Upsilon(3S) decays, we find a significant signal for Upsilon(3S)-->gammaomegaUpsilon(1S) that is consistent with radiative decays Upsilon(3S)-->gammachi(b1,2)(2P), followed by chi(b1,2)(2P)-->omegaUpsilon(1S...

متن کامل

Production of the Η B (ns) States

The rates for magnetic dipole (M1) transitions Υ(nS) → ηb(n S) + γ, n ≤ n, are compared. The photon energies for allowed (n = n) M1 transitions are very small, so hindered (n < n) transitions could be more favorable for discovering the ηb(1S, 2S). The question then arises whether Υ(2S) or Υ(3S) is a better source of ηb(1S). Whereas one nonrelativistic model favors ηb(1S) production from Υ(2S), ...

متن کامل

Measurement of the muonic branching fractions of the narrow upsilon resonances.

The decay branching fractions of the three narrow Upsilon resonances to mu(+)mu(-) have been measured by analyzing about 4.3 fb(-1) e(+)e(-) data collected with the CLEO III detector. The branching fraction B(Upsilon(1S)-->mu(+)mu(-))=(2.49+/-0.02+/-0.07)% is consistent with the current world average, but B(Upsilon(2S)-->mu(+)mu(-))=(2.03+/-0.03+/-0.08)% and B(Upsilon(3S)-->mu(+)mu(-))=(2.39+/-...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

عنوان ژورنال:
  • Physical review letters

دوره 94 3  شماره 

صفحات  -

تاریخ انتشار 2005