Semileptonic transition of B in noncommutative space- time

In this paper, we study the noncommutative effect on the semileptonic transition of B Ò Dlv . We replace the weak interaction vertex in the ordinary space with its counterpart in the noncommutative space. It is shown that, more new form factors are needded to describe the hadronic part of the transi...

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Main Authors: M Gholami, M Haghighat, GH Khosravi
Format: Article
Language:English
Published: Isfahan University of Technology 2013-09-01
Series:Iranian Journal of Physics Research
Subjects:
Online Access:http://ijpr.iut.ac.ir/browse.php?a_code=A-10-1-628&slc_lang=en&sid=1
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author M Gholami
M Haghighat
GH Khosravi
author_facet M Gholami
M Haghighat
GH Khosravi
author_sort M Gholami
collection DOAJ
description In this paper, we study the noncommutative effect on the semileptonic transition of B Ò Dlv . We replace the weak interaction vertex in the ordinary space with its counterpart in the noncommutative space. It is shown that, more new form factors are needded to describe the hadronic part of the transition amplitude. All the form factors are obtained at the lowest order of three point QCD sum rule. Consequently, the decay rate of B Ò Dlv is calculated and a bound of the order of 4 GeV on is given for B Ò Dlv=(5.5 ± 0.5) × 10-2.
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spelling doaj.art-7fd93b5200ef44a7b6d9a0777c4f3ac12022-12-22T03:18:17ZengIsfahan University of TechnologyIranian Journal of Physics Research1682-69572013-09-01132149161Semileptonic transition of B in noncommutative space- timeM GholamiM HaghighatGH KhosraviIn this paper, we study the noncommutative effect on the semileptonic transition of B Ò Dlv . We replace the weak interaction vertex in the ordinary space with its counterpart in the noncommutative space. It is shown that, more new form factors are needded to describe the hadronic part of the transition amplitude. All the form factors are obtained at the lowest order of three point QCD sum rule. Consequently, the decay rate of B Ò Dlv is calculated and a bound of the order of 4 GeV on is given for B Ò Dlv=(5.5 ± 0.5) × 10-2.http://ijpr.iut.ac.ir/browse.php?a_code=A-10-1-628&slc_lang=en&sid=1semileptonic transitionnoncommutative spaceform factordecay rate
spellingShingle M Gholami
M Haghighat
GH Khosravi
Semileptonic transition of B in noncommutative space- time
Iranian Journal of Physics Research
semileptonic transition
noncommutative space
form factor
decay rate
title Semileptonic transition of B in noncommutative space- time
title_full Semileptonic transition of B in noncommutative space- time
title_fullStr Semileptonic transition of B in noncommutative space- time
title_full_unstemmed Semileptonic transition of B in noncommutative space- time
title_short Semileptonic transition of B in noncommutative space- time
title_sort semileptonic transition of b in noncommutative space time
topic semileptonic transition
noncommutative space
form factor
decay rate
url http://ijpr.iut.ac.ir/browse.php?a_code=A-10-1-628&slc_lang=en&sid=1
work_keys_str_mv AT mgholami semileptonictransitionofbinnoncommutativespacetime
AT mhaghighat semileptonictransitionofbinnoncommutativespacetime
AT ghkhosravi semileptonictransitionofbinnoncommutativespacetime