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    Article

    Possibility of extracting the weak phase 7 from Λb→ Λ0 decays

    We explore the possibility of extracting the weak phase γ from pure tree decays Λb→ Λ(ie687_01) in a model independent way. We find the CP violating phase γ can be determined cleanly without any hadronic uncertai...

    A. K. Giri, R. Mohanta, M. P. Khanna in Pramana (2004)

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    Article

    Analysis of directCP violation in \(B^- \to D^0 D_s^-, D^0 D^-\) decays

    We investigate the possibility of observing direct CP violation in the decay modes \(B^- \to D^0 D_s^- \) and \(D^0 D^-\) within the standard m...

    A.K. Giri, R. Mohanta in The European Physical Journal C - Particles and Fields (2001)

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    Article

    An analysis of Cabibbo-favored two-body decays of charmed mesons withη orη′ in the final state

    We have carried out a study of Cabbibbo-favored two-body decays ofD 0 andD s + involving η and η′ in the final state, ...

    R. C. Verma, A. N. Kamal, M. P. Khanna in Zeitschrift für Physik C Particles and Fields (1995)

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    Article

    The strong and radiative decays ofD *-mesons

    M. P. Khanna, M. K. Volkov in Theoretical and Mathematical Physics (1995)

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    Article

    Flavour-spin symmetry and weak decays of heavy hadrons

    Recent developments in the theory of heavy quarks have increased the prospects for the study of non-perturbative QCD in the weak decays of heavy mesons and baryons and for the reliable determination of some of...

    M P Khanna in Pramana (1993)

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    Article

    Sum rules for the pseudoscalar BBP couplings

    In the ‘tadpole’ type mechanism of Coleman and Glashow, where all the summetry breaking effects are generated through symmetry breaking terms belonging to the same regular representation (octet in the case of ...

    M. P. Khanna, R. C. Verma in Zeitschrift für Physik C Particles and Fields (1990)

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    Article

    Ground state baryon magnetic moments and nucleon axial vector coupling

    Ground-state baryon magnetic moments and nucleon axial vector coupling are calculated usingqcd inspired configuration mixing and relativistic corrections. Unlike earlier attempts, we incorporate a natural mass sc...

    Pashupati N Pandit, M P Khanna in Pramana (1985)

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    Article

    Nonleptonic decay matrix elements in the variable pressure bag model

    The consequences of the variable pressure bag model for the nonleptonic decays of hyperons and Ω are investigated. Though the order of magnitude and the relative sign for the various decay amplitudes are correct...

    P K Chatley, M P Khanna in Pramana (1984)

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    Article

    Baryon magnetic moments in quark-diquark model

    The baryon magnetic moments in quark-diquark model are studied and it is found that the diquark (spin 1 and 0) mixing which may arise as a result of quarkgluon interaction inside a hadron, leads to a good agre...

    M P Khanna, R C Verma in Pramana (1983)

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    Article

    Effects of gluon exchange on baryon magnetic moments

    R. C. Verma, M. P. Khanna in Lettere al Nuovo Cimento (1971-1985) (1981)

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    Article

    Masses of charmed andb-quark hadrons in quasinuclear coloured quark model

    Employing non-relativistic quasinuclear coloured quark model, which provides a unified description of mesons and baryons, masses of charmed andb-quark hadrons are studied. Various mass splittings are estimated, a...

    C P Singh, Avinash Sharma, M P Khanna in Pramana (1981)

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    Article

    Symmetry breaking for theBBP-couplings

    Using the consistency requirements arising from the Coleman-Glashow null result for ‘tadpole’-type symmetry-breaking, we obtain a simple method of accounting for the SU(3) symmetry-breaking at theBBP-vertex, with...

    Jatinder K Bajaj, M P Khanna, K Prema in Pramana (1981)

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    Article

    Masses of heavy hadrons in quark model

    C. P. Singh, M. P. Khanna in Lettere al Nuovo Cimento (1971-1985) (1981)

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    Article

    Quark model predictions on the masses of heavier vector mesons

    We use the quark model considerations of Federman, Rubinstein and Talmi and the relation (m ψ/m ϕ)≃(m ϒ/m ψ)≃(m ϒ/m

    C P Singh, Satish Kanwar, M P Khanna in Pramana (1980)

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    Article

    Baryon mass relations in the internalSU 6 symmetry

    M. P. Khanna in Lettere al Nuovo Cimento (1971-1985) (1980)

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    Article

    Magnetic moments of baryons in broken SU(4)

    Assuming that the anomalous magnetic moment interaction has the formaT 1 1 +bT 2 ...

    C P Singh, Ramesh C Verma, M P Khanna in Pramana (1979)

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    Article

    Charm changing weak decays 1/2+ → 3/2+ + 0/γ in SU(4) and SU(8) w

    Weak decay modes (1/2+ → 3/2+ + 0/γ) of charmed baryons are studied. Relations among the various decay amplitudes are derived in isospin, SU(3), SU(4) and SU(8) w symmetries. S...

    Ramesh C Verma, M P Khanna in Pramana (1978)

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    Article

    Adjoint representation admixture to weak nonleptonic decays in SU(4) and SU(8)

    In order to remove some of the unsatisfactory features of the GIM model, we consider15-admixture in SU(4). ΔC=±ΔS decays remain unaffected. Lee-Sugawara sum-rule is obtained.15-admixture is extended then to63-adm...

    Ramesh C Verma, M P Khanna in Pramana (1977)

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    Article

    SU (8) mass relations amongJ P=1/2+ and 3/2+ baryons

    Mass relations among charmed and uncharmed baryons belonging to20 and20′ multiplets of SU(4) are derived in the framework of SU(8) symmetry, Spin singlet mass breaking interaction is found to give unsatisfactory ...

    Ramesh C Verma, M P Khanna in Pramana (1977)

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    Article

    Magnetic moments of baryons in higher symmetry schemes including charm

    Relations among the magnetic moments of charmed and uncharmed baryons are derived in the framework of SU(4) and SU(8) symmetries. The SU(3) resultμ (Σ o)=−μ(Λ) is not present in SU(4), but is obta...

    Ramesh C Verma, M P Khanna in Pramana (1977)

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