Recently added

Collected Works of Prof. Rajasekaran: Recent submissions

  • Rajasekaran G. (Indian Association for the Cultivation of Science (IACS), 1986)
  • Rajasekaran G. (arXiv, 2019)
    Starting with the Wolfenstein form for the leptonic mixing matrix we show that renormaliztion group evolution brings that to the observed large mixing at low energies.
  • Mishra A.K.; Rajasekaran G. (American Institute of Physics, 2000)
    The recent discoveries of new forms of quantum statistics require a close look at the under-lying Fock space structure. This exercise becomes all the more important in order to provide a general classification scheme for ...
  • Mishra A.K.; Rajasekaran G. (American Institute of Physics, 2000)
    We construct the quantum field theory of particles obeying new kinds of quantum statistics, called orthofermi and orthobose statistics. For the orthofermions (orthobosons), the wave function is antisymmetric (symmetric) ...
  • Rajasekaran G. (arXiv, 2006)
    The inward bound path of discovery unravelling the mysteries of matter and the forces that hold it together has culminated at the end of the twentieth century,in a theory of the Fundamental Forces of Nature based on ...
  • Rathin Adhikari.; Rajasekaran G. (arXiv, 2001)
    We consider L-violating Supersymmetric Models to explain the recent muon gμ−2 deviation from the Standard Model. The order of trilinear L-violating couplings which we require also generate neutrino mass which is somewhat ...
  • Rajasekaran G. (arXiv, 2008)
    This is an elementary account of neutrinos as Majarona particles and the search for neutrinoless double beta decays. It also includes some more ideas about neutrinos.
  • Malik R.P.; Mishra A.K.; Rajasekaran G. (arXiv, 1999)
    We develop a GL_{qp}(2) invariant differential calculus on a two-dimensional noncommutative quantum space. Here the co-ordinate space for the exterior quantum plane is spanned by the differentials that are commutative ...
  • Rajasekaran G. (arXiv, 2011)
    We consider the possibility of the existence of a stable massive charged particle by a minimal extension of the standard model particle content. Absolute stability in the case of singly charged particle is not possible if ...
  • Rajasekaran G. (1967)
    Models which regard the decimet B* as a composite of the octet baryons and octet pseudoscalar mesons usually give excessively large SU(3) violations for the B* because of the large mass differences within the baryon octet ...
  • Rajasekaran G. (1967)
    It is shown that Gupta's commutator theory of CP violation violates the CPT theorem and that the anticommutator form for the current-current interaction is necessitated by CPT invariance alone, irrespective of whether CP ...
  • Rajasekaran G.; Biswas S.N. (1961)
    The characteristics of the Λ-N interaction at low energy have been obtained assuming that the Λ-N potential is nonlocal but separable and similar to that suggested by Yamaguchi in the case of N-N potential. The unknown ...
  • Rajasekaran G. (1965)
    It is shown that in order that symmetry considerations be applicable to resonances occurring between the thresholds connected by the symmetry principle, the modulus of the momentum in any channel should be smaller or at ...
  • Dalitz R.H.; Rajasekaran G. (1964)
    The binding energy of the systems ΛΛBe10 and ΛΛHe6, considered as three-particle systems (Λ-Λ-nucleus), are calculated as function of the Λ-Λ potential strength by a variational procedure using a trial function of the form ...
  • Dalitz R.H.; Rajasekaran G. (1963)
    [No abstract available]
  • Rajasekaran G. (Società Italiana di Fisica, 1964)
    [No abstract available]
  • Pandit L.K.; Rajasekaran G. (1969)
    The first-order SU(3) symmetry breaking in semi-leptonic decays is studied by use of the techniques of equal time commutators. The correction for the baryon axial-vector decay constants is related to that for the strong ...
  • Gupta V.; Rajasekaran G. (1969)
    We consider the commutation relations of the vector and axial-vector current densities. Assuming that the commutators of the time components are given (with no Schwinger terms) we derive conditions imposed by covariance ...
  • Dalitz R.H.; Wong T.C.; Rajasekaran G. (1967)
    The Y0*(1405) resonance state is considered in terms of a multichannel potential arising from vector meson (V) exchange between the baryon octet (B) and the pseudoscalar meson octet (P). The interactions are assumed to ...
  • Divakaran P.P.; Gupta V.; Rajasekaran G. (1968)
    The possibility that the electromagnetic current may have a part transforming like I=2, with C=-1, in addition to the usual I=0 and I=1 parts is considered. It is argued that there is no evidence at present to exclude such ...

Search DSpace


Advanced Search

Browse

My Account