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Study of the inducement of PTFE electret on apoptosis of MKN tumor cell@

1999

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Four Lie algebras associated with R6 and their applications

Journal of mathematical physics, 2010-09, Vol.51 (9)

2010

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Quasars, Blazars, and Gamma Rays

Science (American Association for the Advancement of Science), 1992-09, Vol.257 (5077), p.1642-1647

1992

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Finite‐dimensional representations of the special linear Lie superalgebra sl(1,n). I. Typical representations

Journal of mathematical physics, 1987-10, Vol.28 (10), p.2280-2303

Palev, Tchavdar D.

1987

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Quasiparticle and thermodynamic mass in the heavy-fermion system CeB6

Journal of physics. Condensed matter, 1993-10, Vol.5 (40), p.7435-7450

1993

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Constituent quark model and a possible JP=0-, T=0 dibaryon

Journal of physics. G, Nuclear and particle physics, 1994-05, Vol.20 (5), p.L49-L56

1994

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Conservation laws in electrically polarizable spatially dispersive media. II. Additional boundary condition

Journal of physics. Condensed matter, 1991-04, Vol.3 (15), p.2561-2575, Article 2561

1991

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Acoustic axes in orthorhombic media

Proceedings of the Royal Society of London. Series A, Mathematical and physical sciences, 1985-09, Vol.401 (1820), p.131-143

1985

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The analytically continued S matrix for potentials defined as a sum of exponentials. II. The multichannel problem

Journal of physics. B, Atomic and molecular physics, 1983-08, Vol.16 (15), p.2785-2800

Meyer, H D

1983

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Study of the inducement of PTFE electret on apoptosis of MKN tumor cell@

Four Lie algebras associated with R6 and their applications

Quasars, Blazars, and Gamma Rays

Finite‐dimensional representations of the special linear Lie superalgebra sl(1,n). I. Typical representations

Quasiparticle and thermodynamic mass in the heavy-fermion system CeB6

Constituent quark model and a possible JP=0-, T=0 dibaryon

Conservation laws in electrically polarizable spatially dispersive media. II. Additional boundary condition

Acoustic axes in orthorhombic media

The analytically continued S matrix for potentials defined as a sum of exponentials. II. The multichannel problem

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