Electronic structure of praseodymium monopnictides and monochalcogenides under pressure
暂无分享,去创建一个
[1] T. Kikegawa,et al. X-ray study with synchrotron radiation of cerium and praseodymium monopnictides with the NaCl-type structure at high pressures , 2003 .
[2] S. K. De,et al. Magneto-optical Kerr effect in Pr monopnictides , 2003 .
[3] M. Rajagopalan,et al. Theoretical studies on the high pressure phases of Lanthanum monochalcogenides , 2003 .
[4] M. Rajagopalan,et al. Theoretical study of LaP and LaAs at high pressures , 2002 .
[5] M. Rajagopalan,et al. Electronic and structural properties of LaSb and LaBi , 2002 .
[6] P. Söderlind. Delocalization and phase transitions in Pr: Theory , 2002 .
[7] A. Steckl,et al. Rare earth doped semiconductors III , 2001 .
[8] Z. Szotek,et al. Self-interaction-corrected description of the electronic properties of americium monochalcogenides and monopnictides , 2001 .
[9] T. Kikegawa,et al. Phase transitions of LnAs (Ln = Pr, Nd, Sm, Gd, Dy and Ho) with NaCl-type structure at high pressures , 2001 .
[10] T. Kikegawa,et al. Phase transitions of LnSb (Ln=lanthanide) with NaCl-type structure at high pressures , 2000 .
[11] O. Eriksson,et al. Spin-orbit coupling in the actinide elements : A critical evaluation of theoretical equilibrium volumes , 1999, cond-mat/9908344.
[12] P. Strange,et al. Understanding the valency of rare earths from first-principles theory , 1999, Nature.
[13] Z. Szotek,et al. THEORY OF PRESSURE-INDUCED PHASE TRANSITIONS IN CERIUM CHALCOGENIDES , 1999 .
[14] O. Shimomura,et al. Phase transitions of lanthanide monophosphides with NaCl-type structure at high pressures , 1998 .
[15] Z. Szotek,et al. Electronic structure of cerium monopnictides under pressure , 1998 .
[16] Segall,et al. Electronic structure of rare-earth pnictides. , 1996, Physical review. B, Condensed matter.
[17] Lemos. Singularities in a scalar field quantum cosmology. , 1995, Physical review. D, Particles and fields.
[18] Svane. Electronic structure of cerium in the self-interaction corrected local spin density approximation. , 1994, Physical review letters.
[19] O. Gunnarsson,et al. Transition-metal oxides in the self-interaction-corrected density-functional formalism. , 1990, Physical review letters.
[20] M. Methfessel,et al. Elastic constants and phonon frequencies of Si calculated by a fast full-potential linear-muffin-tin-orbital method. , 1988, Physical review. B, Condensed matter.
[21] Norman,et al. Supercell calculations of the valence photoemission spectra of CeSb, PrSb, and NdSb. , 1985, Physical review. B, Condensed matter.
[22] A. Zunger,et al. Self-interaction correction to density-functional approximations for many-electron systems , 1981 .
[23] B. Segall,et al. Self-consistent electronic structure of Si, Ge and diamond by the LMTO-ASA method , 1980 .
[24] B. Morosin,et al. Remarks on the compressibilities of cubic materials and measurements on Pr chalcogenides , 1979 .
[25] F. Hulliger. Chapter 33 Rare earth pnictides , 1979 .
[26] V. Pecharsky,et al. Handbook on the physics and chemistry of rare earths , 1979 .
[27] O. K. Andersen,et al. Linear methods in band theory , 1975 .
[28] A. Jayaraman,et al. Pressure-Induced Electronic Collapse and Structural Changes in Rare-Earth Monochalcogenides , 1972 .
[29] K. Andres,et al. Hyperfine Enhanced Nuclear Magnetic Cooling in Van Vleck Paramagnetic Intermetallic Compounds , 1971 .