ar X iv : h ep - l at / 0 01 10 08 v 2 1 3 N ov 2 00 0 1 Differential decay rate for B →

نویسندگان

  • S. Aoki
  • R. Burkhalter
  • M. Fukugita
  • S. Hashimoto
  • K - I. Ishikawa
  • N. Ishizuka
  • Y. Iwasaki
  • K. Kanaya
  • T. Kaneko
  • Y. Kuramashi
  • M. Okawa
  • T. Onogi
  • S. Tominaga
  • N. Tsutsui
  • A. Ukawa
  • N. Yamada
  • T. Yoshi
چکیده

We present our study on B → πlν semileptonic decay form factors using NRQCD action for heavy quark. In the analysis, we use the form factors f1(v · kπ) and f2(v · kπ) defined in the context of heavy quark effective theory by Burdman et al.. Since the NRQCD action for heavy quark respects the heavy quark symmetry, our results are described by the HQET form factors most naturally. From a quenched lattice QCD simulation at β=5.9 on a 16 3 × 48 lattice, we obtain the form factors f1(v · kπ) and f2(v · kπ), and find that their 1/mB correction is small. The limit of physical heavy and light quark masses can be reached without introducing any model function, and we obtain a prediction for the differential decay rate dΓ/dq 2. We also discuss the soft pion limit of the form factors.

برای دانلود رایگان 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

ar X iv : h ep - l at / 0 01 10 08 v 1 1 N ov 2 00 0 1 Differential decay rate for B → πlν semileptonic decays ∗

We present our study on B → πlν semileptonic decay form factors using NRQCD action for heavy quark. In the analysis, we use the form factors f1(v · kπ) and f2(v · kπ) defined in the context of heavy quark effective theory by Burdman et al.. Since the NRQCD action for heavy quark respects the heavy quark symmetry, our results are described by the HQET form factors most naturally. From a quenched...

متن کامل

ar X iv : h ep - l at / 0 01 10 26 v 2 1 3 N ov 2 00 0 1 QCD vacuum structure

Several issues related to the structure of the QCD vacuum are reviewed. We concentrate mostly on results concerning instantons and center vortices.

متن کامل

ar X iv : h ep - l at / 0 01 10 26 v 1 3 N ov 2 00 0 1 QCD vacuum structure

Several issues related to the structure of the QCD vacuum are reviewed. We concentrate mostly on results concerning instantons and center vortices.

متن کامل

ar X iv : h ep - l at / 0 01 10 90 v 1 3 0 N ov 2 00 0 PARALLEL COMPUTING FOR QCD ON A PENTIUM CLUSTER

Motivated by the computational demands of our research and budgetary constraints which are common to many research institutions, we built a " poor man's supercomputer " , a cluster of PC nodes which together can perform parallel calculations at a fraction of the price of a commercial supercomputer. We describe the construction, cost, and performance of our cluster.

متن کامل

ar X iv : h ep - l at / 0 01 10 13 v 3 8 N ov 2 00 0 1 Chemical potential response of meson masses at finite temperature

We study the response of meson masses to the chemical potential (∂m/∂µ) at high temperature and at zero chemical potential on N f = 2 lattice with staggered fermions. Preliminary results for the meson composed of different quarks show that ∂m/∂µ|µ=0 is negative in the confinement phase and positive in the deconfinement phase.

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

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 2000