Recently added

Collected Works of Prof. Rajasekaran: Recent submissions

  • Rajasekaran G. (2011)
    [No abstract available]
  • Rajasekaran G. (2012)
    Commentary
  • Indumathi D.; Kaul R.K.; Murthy M.V.N.; Rajasekaran G. (2012)
    We follow up on the analysis of Mecozzi and Bellini (arXiv:1110.1253v1) where they showed, in principle, the possibility of superluminal propagation of neutrinos, as indicated by the recent OPERA result. We refine the ...
  • Rajasekaran G. (Indian Academy of Sciences, Bangalore, 2016)
    After a brief history, we focus on the present status of HEP and its possible future. Ideas to ensure a healthy growth of HEP in India are discussed. This involves a few major experimental projects in fundamental physics. ...
  • Rajasekaran G. (Indian Academy of Sciences, Bangalore, 2016)
    This paper is based on a paper written byMV NMurthy and G Rajasekaran, Pramana- J. Phys. 82, L609 (2014); arXiv:1305.2715. The possibility of the unexplained Kolar events, recorded in the 1970s and 1980s, being due to the ...
  • Abbas G.; Abyaneh M.Z.; Biswas A.; Gupta S.; Patra M.; Rajasekaran G.; Srivastava R. (World Scientific Publishing Co. Pte Ltd, 2016)
    The origin of small mixing among the quarks and a large mixing among the neutrinos has been an open question in particle physics. In order to answer this question, we postulate general relations among the quarks and the ...
  • Choubey S.; Indumathi D.; Agarwalla S.; Bandyopadhyay A.; Bhattacharyya G.; Chun E.J.; Dasgupta B.; Dighe A.; Ghoshal P.; Giri A.K.; Goswami S.; Hirsch M.; Kajita T.; Kaplinghat M.; Mani H.S.; Mohanta R.; Murthy M.V.N.; Pakvasa S.; Parida M.K.; Rajasekaran G.; Ray S.; Rodejohann W.; Roy P.; Umasankar S.; Schwetz T.; Sinha N. (Indian Academy of Sciences, Bangalore, 2009)
    This is the report of the neutrino physics working group at WHEPP-X. We summarize the problems selected and discussed at the workshop and the papers which have resulted subsequently. © Indian Academy of Sciences.
  • Murthy M.V.N.; Rajasekaran G. (Indian Academy of Sciences, Bangalore, 2014)
    The possibility of the unexplained Kolar events, recorded in the 1970s and 1980s, being due to the decays of dark matter particles of mass in the range of 510 GeV, is pointed out. © Indian Academy of Sciences.
  • Agarwalla S.K.; Parida M.K.; Mohapatra R.N.; Rajasekaran G. (2007)
    The high scale mixing unification hypothesis recently proposed by three of us (R.N.M., M.K.P. and G.R.) states that if at the seesaw scale the quark and lepton mixing matrices are equal, then for quasidegenerate neutrinos ...
  • Rajasekaran G. (Indian Academy of Sciences, Bangalore, 2019)
    Murray Gell-Mann, who passed away at the age of 90 years was a giant of modern particle physics. His most well-known contribution is the proposal that protons and neutrons are not indivisible but are made up of smaller ...
  • Rajasekaran G. (2012)
    [No abstract available]
  • Rajasekaran G. (Indian Academy of Sciences, Bangalore, 2016)
    [No abstract available]
  • Acharya B.S.; Agarwalla S.K.; Behera P.K.; Bhasin A.; Chattopadhyay S.; Choubey S.; Datar V.; Gandhi R.; Gangopadhyay G.; Goswami S.; Hasan R.; Indumathi D.; Mondal N.K.; Murthy M.V.N.; Naimuddin M.D.; Rajasekaran G.; Ranganathaiah C.; Raychaudhuri A.; Singh V.; Sinha N.; Vinodkumar A.M.; Viyogi Y.P. (2013)
    [No abstract available]
  • Kumar A.; Kumar A.M.V.; Jash A.; Mohanty A.K.; Chacko A.; Ajmi A.; Ghosal A.; Khatun A.; Raychaudhuri A.; Dighe A.; Chatterjee A.; Gaur A.; Ghosh A.; Kumar A.; Redij A.; Satyanarayana B.; Acharya B.S.; Choudhary B.C.; Ranganathaiah C.; Ravikumar C.D.; Gupta C.; Indumathi D.; Kaur D.; Majumdar D.; Samuel D.; Tiwari D.; Rajasekaran G.; Gangopadhyay G.; Majumder G.; Ravikumar H.B.; Singh J.B.; Shahi J.S.; Libby J.; Singh J.; Raveendrababu K.; Meghna K.K.; Rebin K.R.; Kar K.; Bhattacharya K.; Pant L.M.; Athar M.S.; Murthy M.V.N.; Malik M.A.; Naimuddin M.D.; Salim M.; Ghosh M.; Devi M.M.; Mondal N.K.; Majumdar N.; Sinha N.; Dash N.; Ghoshal P.; Mehta P.; Behera P.; Kanishka R.; Gandhi R.; Ganai R.; Hasan R.; Krishnaveni S.; Lakshmi S.M.; Singh S.K.; Inbanathan S.S.R.; Sankar S.U.; Jafer S.; Biswas S.; Kumar S.; Agarwalla S.K.; Choubey S.; Saha S.; Ahmed S.; Behera S.P.; Goswami S.; Chattopadhyay S.; Bhattacharya S.; Banerjee S.; Dasgupta S.; Pal S.; Mukhopadhyay S.; Raut S.; Bose S.; Mahapatra S.; Ghosh T.; Thakore T.; Kashyap V.K.S.; Subrahmanyam V.S.; Singh V.; Chandratre V.B.; Bhatnagar V.; Datar V.M.; Bari W.; Viyogi Y.P. (Indian Academy of Sciences, Bangalore, 2017)
    The upcoming 50 kt magnetized iron calorimeter (ICAL) detector at the India-based Neutrino Observatory (INO) is designed to study the atmospheric neutrinos and antineutrinos separately over a wide range of energies and ...
  • Garg S.K.; Shreecharan T.; Das P.K.; Deshpande N.G.; Rajasekaran G. (Springer Verlag, 2011)
    We analyze e+e- → γγ, e -γ →γγ → e+e- processes within the Seiberg-Witten expanded noncommutative scenario using polarized beams. With unpolarized beams the leading order effects of non commutativity starts from second ...
  • Rajasekaran G. (Indian Academy of Sciences, Bangalore, 2014)
    The history of weak interactions starting with Fermi's creation of the beta decay theory and culminating in its modern avatar in the form of the electroweak gauge theory is described. Discoveries of parity violation, ...
  • Abbas G.; Gupta S.; Rajasekaran G.; Srivastava R. (American Physical Society, 2015)
    Starting with the high scale mixing unification hypothesis, we investigate the renormalization-group evolution of mixing parameters and masses for Dirac-type neutrinos. Following this hypothesis, the Pontecorvo-Maki-Naka ...
  • Abbas G.; Gupta S.; Rajasekaran G.; Srivastava R. (American Physical Society, 2014)
    We investigate the renormalization group evolution of masses and mixing angles of Majorana neutrinos under the "high scale mixing unification" hypothesis. Assuming the unification of quark-lepton mixing angles at a high ...
  • Cao Q.-H.; Ma E.; Rajasekaran G. (2007)
    If the standard model of particle interactions is extended to include a second scalar doublet [H+,(H0+iA0)/2], which is odd under an unbroken Z2 discrete symmetry, it may be called the dark scalar doublet, because its ...
  • Ma E.; Rajasekaran G. (Institute of Physics Publishing, 2017)
    It has recently been shown that the phenomenologically successful pattern of cobimaximal neutrino mixing (θ13 ≠ 0, θ23 = π/4, and δCP = ±π/2) may be achieved in the context of the non-Abelian discrete symmetry A4, if the ...

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