A. Narayan
Mississippi State University
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by A. Narayan.
Physical Review Letters | 2013
D. Androic; A. Asaturyan; T. Averett; J. Balewski; J. Beaufait; J. Benesch; F. Benmokhtar; J. Birchall; R. Carlini; S. Covrig; W. Deconinck; J. Diefenbach; D. Dutta; M. Elaasar; D. Gaskell; J. Grames; K. Grimm; F. Guo; K. Johnston; D. Jones; M. K. Jones; R. Jones; E. Korkmaz; S. Kowalski; J. Leacock; J. Leckey; L. Lee; S. MacEwan; D. Mack; R. Mahurin
The Q(weak) experiment has measured the parity-violating asymmetry in ep elastic scattering at Q(2)=0.025(GeV/c)(2), employing 145 μA of 89% longitudinally polarized electrons on a 34.4 cm long liquid hydrogen target at Jefferson Lab. The results of the experiments commissioning run, constituting approximately 4% of the data collected in the experiment, are reported here. From these initial results, the measured asymmetry is A(ep)=-279±35 (stat) ± 31 (syst) ppb, which is the smallest and most precise asymmetry ever measured in ep scattering. The small Q(2) of this experiment has made possible the first determination of the weak charge of the proton Q(W)(p) by incorporating earlier parity-violating electron scattering (PVES) data at higher Q(2) to constrain hadronic corrections. The value of Q(W)(p) obtained in this way is Q(W)(p)(PVES)=0.064±0.012, which is in good agreement with the standard model prediction of Q(W)(p)(SM)=0.0710±0.0007. When this result is further combined with the Cs atomic parity violation (APV) measurement, significant constraints on the weak charges of the up and down quarks can also be extracted. That PVES+APV analysis reveals the neutrons weak charge to be Q(W)(n)(PVES+APV)=-0.975±0.010.
Physical Review C | 2016
T. Gogami; Chen Chen; D. Kawama; P. Achenbach; A. Ahmidouch; I. Albayrak; D. Androic; A. Asaturyan; R. Asaturyan; O. Ates; P. Baturin; R. Badui; W. Boeglin; J. Bono; E. Brash; P. Carter; A. Chiba; E. Christy; S. Danagoulian; R. De Leo; D. Doi; M. Elaasar; R. Ent; Y. Fujii; M. Fujita; M. Furic; M. Y. Gabrielyan; L. Gan; F. Garibaldi; D. Gaskell
Spectroscopy of a
Physics Letters B | 2017
J. A. Magee; A. Narayan; D. Jones; R.S. Beminiwattha; J. C. Cornejo; M. M. Dalton; W. Deconinck; D. Dutta; D. Gaskell; J. W. Martin; Kent Paschke; Vladas Tvaskis; A. Asaturyan; J. Benesch; G. D. Cates; B. S. Cavness; L. A. Dillon-Townes; G. Hays; J.R. Hoskins; E. Ihloff; R. Jones; P. M. King; S. Kowalski; L. Kurchaninov; L. Lee; A. McCreary; M. McDonald; A. Micherdzinska; A. Mkrtchyan; H. Mkrtchyan
^{10}_{\Lambda}
arXiv: Nuclear Experiment | 2015
A. Narayan; D. Jones; J. C. Cornejo; M. M. Dalton; W. Deconinck; D. Dutta; D. Gaskell; J. W. Martin; Kent Paschke; V. Tvaskis; A. Asaturyan; J. Benesch; G. D. Cates; B. S. Cavness; L. A. Dillon-Townes; G. Hays; E. Ihloff; R. Jones; S. Kowalski; L. Kurchaninov; L. Lee; A. McCreary; M. McDonald; A. Micherdzinska; A. Mkrtchyan; H. Mkrtchyan; V. Nelyubin; S. Page; W. D. Ramsay; P. Solvignon
Be hypernucleus was carried out at JLab Hall C using the
Nature | 2018
D. Androic; M. Shabestari; B. Sawatzky; K. Bartlett; J.F. Dowd; L. Lee; S. Zhamkochyan; D. Gaskell; T. Averett; V. Tvaskis; B. Waidyawansa; M. Poelker; D. Dutta; V.M. Gray; A. Micherdzinska; A. Asaturyan; Nuruzzaman; J. Grames; J. Leacock; N. Simicevic; P. Wang; J. Leckey; Jae Hyuk Lee; J. Dunne; P. Solvignon; J. Benesch; R. Suleiman; A. Mkrtchyan; Kent Paschke; M. M. Dalton
(e,e^{\prime}K^{+})
Physical Review Letters | 2016
A. Narayan; D. Jones; J. C. Cornejo; M. M. Dalton; Wouter Deconinck; D. Dutta; D. Gaskell; J. W. Martin; Kent Paschke; V. Tvaskis; A. Asaturyan; J. Benesch; G. D. Cates; B. S. Cavness; L. A. Dillon-Townes; G. Hays; R. Jones; P. King; L. Kurchaninov; L. Lee; M. McDonald; A. Micherdzinska; A. Mkrtchyan; H. Mkrtchyan; V. Nelyubin; S. Page; W. D. Ramsay; P. Solvignon; D. Storey; A. Tobias
reaction. A new magnetic spectrometer system (SPL+HES+HKS), specifically designed for high resolution hypernuclear spectroscopy, was used to obtain an energy spectrum with a resolution of 0.78 MeV (FWHM). The well-calibrated spectrometer system of the present experiment using the
Physical Review C | 2015
T. Gogami; M. Furic; R. Badui; R. De Leo; A. Matsumura; T. Horn; P. Markowitz; H. Mkrtchyan; T. Maruta; M. I. Niculescu; E. Christy; S. A. Wood; H. Kanda; D. Doi; J. Pochodzalla; Y. Okayasu; A. Gasparian; S. Zhamkochyan; F. R. Wesselmann; D. Gaskell; L. Gan; A. Narayan; V. Maxwell; R. Ent; K. Yokota; M. Elaasar; J. Bono; K. Tsukada; V. Tadevosyan; D. Androic
p(e,e^{\prime}K^{+})\Lambda,\Sigma^{0}
EPJ Web of Conferences | 2014
D. Androic; D.S. Armstrong; A. Asaturyan; T. Averett; J. Balewski; J. Beaufait; R.S. Beminiwattha; J. Benesch; F. Benmokhtar; J. Birchall; R. Carlini; G. D. Cates; J.C. Cornejo; S. Covrig; M. M. Dalton; C.A. Davis; W. Deconinck; J. Diefenbach; J.F. Dowd; J. Dunne; D. Dutta; W.S. Duvall; M. Elaasar; W.R. Falk; J. M. Finn; T. Forest; D. Gaskell; M. T. Gericke; J. Grames; V.M. Gray
reactions allowed us to determine the energy levels, and the binding energy of the ground state peak (mixture of 1
Physical Review X | 2016
A. Narayan; D. Jones; J. C. Cornejo; M. M. Dalton; W. Deconinck; D. Dutta; D. Gaskell; J. W. Martin; Kent Paschke; V. Tvaskis; A. Asaturyan; J. Benesch; G. D. Cates; B. S. Cavness; L. A. Dillon-Townes; G. Hays; E. Ihloff; R. Jones; P. King; S. Kowalski; L. Kurchaninov; L. Lee; M. McDonald; A. Micherdzinska; A. Mkrtchyan; H. Mkrtchyan; V. Nelyubin; S. Page; W. D. Ramsay; P. Solvignon
^{-}
Physical Review C | 2016
T. Gogami; Chen Chen; D. Kawama; P. Achenbach; A. Ahmidouch; I. Albayrak; D. Androic; A. Asaturyan; R. Asaturyan; O. Ates; P. Baturin; R. Badui; W. Boeglin; J. Bono; E. Brash; P. Carter; A. Chiba; E. Christy; S. Danagoulian; R. De Leo; D. Doi; M. Elaasar; R. Ent; Y. Fujii; M. Fujita; M. Furic; M. Y. Gabrielyan; L. Gan; F. Garibaldi; D. Gaskell
and 2