Dayashankar Kulshreshtha | University of Delhi (original) (raw)
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Papers by Dayashankar Kulshreshtha
Physics Letters B, 1991
The quark loop diagram for f;P for a heavy-light (Qq) meson is employed within a Lorentz-invarian... more The quark loop diagram for f;P for a heavy-light (Qq) meson is employed within a Lorentz-invariant framework for addressing a two-fold issue: (i) finite corrections to the asymptotic scaling law (f;P~mQ-1/2) of shifman, Voloshin, Politzer and Wise; (ii) 1/MQ corrections to the static approximation for the heavy-quark propagator in lattice calculations. The loop diagram yields a general two-component structure f;P=f;0+deltaf;
Journal of Modern Physics, Jan 1, 2012
Recently we have studied the instant-form quantization (IFQ) and the light-front quantization (LF... more Recently we have studied the instant-form quantization (IFQ) and the light-front quantization (LFQ) of the conformally gauge-fixed Polyakov D1 brane action using the Hamiltonian and path integral formulations. The IFQ is studied in the equal world-sheet time framework on the hyperplanes defined by the world-sheet time σ 0 = τ = constant and the LFQ in the equal light-cone world-sheet time framework, on the hyperplanes of the light-front defined by the light-cone world-sheet time . The light-front theory is seen to be a constrained system in the sense of Dirac in contrast to the instant-form theory. However, owing to the gauge anomalous nature of these theories, both of these theories are seen to lack the usual string gauge symmetries defined by the world-sheet reparametrization invariance (WSRI) and the Weyl invariance (WI). In the present work we show that these theories when considered in the presence of background gauge fields such as the NSNS 2-form gauge field
Il Nuovo Cimento A (1971-1996), Jan 1, 1985
... 87A, N. 1 1 Maggie 1985 ... IIALLING, DL ]cIA:RTILL, S. IIOLZNER, M. ITO, J. KANDAS-WAMY, DL ... more ... 87A, N. 1 1 Maggie 1985 ... IIALLING, DL ]cIA:RTILL, S. IIOLZNER, M. ITO, J. KANDAS-WAMY, DL KREINICK, Y. KUBOTA, NB MISTRY, F. MO:RROW, E. NO:RDBE:RG, M. 0GG, A. SILVER:MAN, I ). C. STEIN, S. STONE, I). WEBE:R, R. ~VILCKE, AJ SADDOFF, R. GILES, J. IIASSA ...
Lettere Al Nuovo Cimento (19711985), Jan 1, 1985
Summary We investigate the spectroscopy of the charmonium (cc) and bottomonium (bb) bound states ... more Summary We investigate the spectroscopy of the charmonium (cc) and bottomonium (bb) bound states in a static flavour-independent nonrelativistic quark-antiquark (qq) two-step potential model proposed earlier. Our predictions are in good agreement with ...
Journal of Modern Physics, Jan 1, 2011
Journal of Modern Physics, Jan 1, 2010
Physics Letters B, 1991
The quark loop diagram for f;P for a heavy-light (Qq) meson is employed within a Lorentz-invarian... more The quark loop diagram for f;P for a heavy-light (Qq) meson is employed within a Lorentz-invariant framework for addressing a two-fold issue: (i) finite corrections to the asymptotic scaling law (f;P~mQ-1/2) of shifman, Voloshin, Politzer and Wise; (ii) 1/MQ corrections to the static approximation for the heavy-quark propagator in lattice calculations. The loop diagram yields a general two-component structure f;P=f;0+deltaf;
Journal of Modern Physics, Jan 1, 2012
Recently we have studied the instant-form quantization (IFQ) and the light-front quantization (LF... more Recently we have studied the instant-form quantization (IFQ) and the light-front quantization (LFQ) of the conformally gauge-fixed Polyakov D1 brane action using the Hamiltonian and path integral formulations. The IFQ is studied in the equal world-sheet time framework on the hyperplanes defined by the world-sheet time σ 0 = τ = constant and the LFQ in the equal light-cone world-sheet time framework, on the hyperplanes of the light-front defined by the light-cone world-sheet time . The light-front theory is seen to be a constrained system in the sense of Dirac in contrast to the instant-form theory. However, owing to the gauge anomalous nature of these theories, both of these theories are seen to lack the usual string gauge symmetries defined by the world-sheet reparametrization invariance (WSRI) and the Weyl invariance (WI). In the present work we show that these theories when considered in the presence of background gauge fields such as the NSNS 2-form gauge field
Il Nuovo Cimento A (1971-1996), Jan 1, 1985
... 87A, N. 1 1 Maggie 1985 ... IIALLING, DL ]cIA:RTILL, S. IIOLZNER, M. ITO, J. KANDAS-WAMY, DL ... more ... 87A, N. 1 1 Maggie 1985 ... IIALLING, DL ]cIA:RTILL, S. IIOLZNER, M. ITO, J. KANDAS-WAMY, DL KREINICK, Y. KUBOTA, NB MISTRY, F. MO:RROW, E. NO:RDBE:RG, M. 0GG, A. SILVER:MAN, I ). C. STEIN, S. STONE, I). WEBE:R, R. ~VILCKE, AJ SADDOFF, R. GILES, J. IIASSA ...
Lettere Al Nuovo Cimento (19711985), Jan 1, 1985
Summary We investigate the spectroscopy of the charmonium (cc) and bottomonium (bb) bound states ... more Summary We investigate the spectroscopy of the charmonium (cc) and bottomonium (bb) bound states in a static flavour-independent nonrelativistic quark-antiquark (qq) two-step potential model proposed earlier. Our predictions are in good agreement with ...
Journal of Modern Physics, Jan 1, 2011
Journal of Modern Physics, Jan 1, 2010