Muzaffar Irshad

Muzaffar Irshad


Research Focus & Metrics

Academic Career Length

7Years (2020-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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20 May 2022 in Physics Letters B
Verified
Journal Article
Open access
MAM. Ablikim
M. Ablikim
MAM.N. Achasov
M.N. Achasov
PAP. Adlarson
P. Adlarson
SAS. Ahmed
S. Ahmed
MAM. Albrecht
M. Albrecht
JZJ.H. Zou
J.H. Zou

4 January 2022 in Symmetry
Verified
Journal Article
Open access
PDF file
MIMuzaffar Irshad
Muzaffar Irshad
DLDong Liu
Dong Liu
XZXiaorong Zhou
Xiaorong Zhou
GHGuangshun Huang
Guangshun Huang
Electromagnetic form factors (EMFFs) are fundamental observable of baryons that intimately related to their internal structure and dynamics, where the EMFFs of hyperons provide valuable insight into the behavior of the strangeness. The EMFFs of hyperons can also help to understand those of nucleons as they are connected with the flavor SU(3) symmetry. The EMFFs of nucleons can be measured in both spacelike and timelike regions. However, it is difficult to probe the EMFFs of hyperons in spacelike region due to the unstable nature of hyperons. By means of electron-positron annihilation, the EMFFs of hyperons in timelike region is accessible via the production of hyperon-antihyperon pair. The timelike EMFFs of the isospin triplet Σ hyperons measured at Babar, CLEO-c and BESIII experiments are reviewed in this paper. Besides, the relevant theoretical discussion based on the experimental results are also presented.

5 May 2020 in Physical Review D
Verified
Journal Article
Open access
PDF file
MAM. Ablikim
M. Ablikim
MAM. N. Achasov
M. N. Achasov
PAP. Adlarson
P. Adlarson
SAS. Ahmed
S. Ahmed
MAM. Albrecht
M. Albrecht
BCBESIII Collaboration
BESIII Collaboration
We measured the branching fractions of the decays χcJ→Σ−Σ¯+ for the first time using the final states nn¯π+π−. The data sample exploited here is 448.1×106  ψ(3686) events collected with BESIII. We find B(χcJ→Σ−Σ¯+)=(51.3±2.4±4.1)×10−5,(5.7±1.4±0.6)×10−5, and (4.4±1.7±0.5)×10−5, for J=0, 1, 2, respectively, where the first uncertainties are statistical and the second systematic.