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排序方式: 共有219条查询结果,搜索用时 15 毫秒
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Brick DH Widgoff M Beilliere P Lutz P Narjoux JL Gelfand N Alyea ED Bloomer M Bober J Busza W Cole B Frank TA Fuess TA Grodzins L Hafen ES Haridas P Huang D Huang HZ Hulsizer R Kistiakowsky V Ledoux RJ Milstene C Noguchi S Oh SH Pless IA Steadman S Stoughton TB Suchorebrow V Tether S Trepagnier PC Wadsworth BF Wu Y Yamamoto RK Cohn HO Calligarich E Castoldi C Dolfini R Introzzi G Ratti S Badiak M DiMarco R Jacques PF Kalelkar M Plano RJ Stamer PE Brucker EB Koller EL Alexander G Grunhaus J 《Physical review D: Particles and fields》1990,41(3):765-773
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Synthesis and X-Ray Structure Analysis of the 8π-Electron-Ring-System S4N4O2Sn2(CH3)6 and the Magnetic Properties of S4N4O2 and S8N8O4 S4N4O2 reacts with N[Sn(CH3)3]3 in a molar ratio of 1:1 to an eight-membered trimethyltin-substituted 8π-electron skeleton, S4N4O2Sn2(CH3)6. In contrast to known 6π-electronsystems this compound has tin atoms which are tetracoordinated. This was demonstrated on the basis of an x-ray analysis. S4N4O2Sn2(CH3)6 · 1/2 C6H6 crystallizes in the space group P21/c with a = 1396.0(4), b = 1190.3(4), c = 1256.7(3) pm, and β = 103.46(2)°. It was shown that the ability of coordination at the tin atom depends on the electron density. The magnetic properties of S4N4O2 and S8N8O4 were investigated by the Faraday method. The high diamagnetism in these ring compounds is caused by the π-electrons. 相似文献
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The crystal structure of La3ReO8, prepared at 1425°C, is reported to be different from a previous result on a preparation at 900°C (BAUD et al., 1979). The high temperature modification crystallizes in the monoclinic space group P21/m with a = 7.757(1), b = 7.777(1), c = 5.928(1) Å, γ = 111.1°, Z = 2. The structure was solved by Patterson and Fourier methods from single crystal diffractometer data and refined to final R(F) = 0,073. The structure consists of isolated, distorted ReO6 octahedra and double chains of edge-shared La4O tetrahedra. 相似文献
5.
Boca R Gembický M Herchel R Haase W Jäger L Wagner C Ehrenberg H Fuess H 《Inorganic chemistry》2003,42(22):6965-6967
Triethylenetetramine (L(4)) was used as a tetradentate blocking ligand that, after complexation with Ni(II), leaves two sites ready for ligation with tricyanomethanide. The formed binuclear complex [L(4)Ni(NCC(CN)CN)(2)NiL(4)](ClO(4))(2) exhibits a ferromagnetic coupling with J/hc = +0.15 cm(-1) and g(Ni) = 2.126; below 16 K, a ferromagnetic ordering is evidenced by ac magnetic susceptibility (both in-phase and out-of-phase), magnetization, field-cooled magnetization, and zero-field-cooled magnetization measurements. 相似文献
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Structure and Properties of Double Halogenides of Substituted Ammonium and Mercury(II). VI. Crystal Structure of (CH3NH3)2HgBr4 and (CH3NH3)2HgI4 The compounds (CH3NH3)2HgBr4 and (CH3NH3)2HgI4 were prepared from stoichiometric mixtures of the methylammonium halogenides and the mercury(II) halogenides in methanol by evaporation. X-ray structure determination revealed for (CH3NH3)2HgBr4 monoclinic symmetry, space group P21/c and orthorhombic symmetry, space group Pbca for (CH3NH3)2HgI4. Both compounds are built from isolated, slightly deformed tetrahedra. The Hg? Br distances range from 2.586(3) Å to 2.598(2) Å, the Br? Hg? Br angles from 105.36(8)° to 112.26(8)°. The observed distances in the HgI4 tetrahedra are in the range 2.751(1) and 2.803(1) Å, the I? Hg? I angles between 106.25(3)° and 115.68(4)°. The tetrahedra are linked together by hydrogen bonds between the methylammonium group and the halogen atoms. 相似文献
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The new complex indium rhenium and scandium rhenium oxides, In6ReO12 and Sc6ReO12, have been synthesized as single phases in sealed silica tubes and by high-pressure high-temperature syntheses, and their crystal structures have been determined by single crystal X-ray diffraction.The compounds crystallize in a rhombohedral structure related to the distorted fluorite structure like Ln6ReO12 for some rare earth elements, S. G.: R-3, Z=3, aH= 9.248(2) Å, cH=8.720(2) Å for Sc6ReO12 and aH=9.492(1) Å, cH=8.933(1) Å for In6ReO12. A maximum in magnetization is observed for Sc6ReO12 at T(Mmax)=1.89(2) K, whereas ferromagnetic ordering is found for In6ReO12 by a pronounced increase in the temperature dependence of magnetization at TC=7.5(5) K. The magnetic moment per rhenium ion in In6ReO12 and Sc6ReO12 is 0.84(1) and 0.65(1) μB, respectively, derived from the paramagnetic regions. 相似文献
10.
Bogert D Burnstein R Fisk R Fuess S Morfin J Ohska Stutte L Walker JK Bofill J Busza W Eldridge T Friedman JI Goodman MC Kendall HW Kostoulas IG Lyons T Magahiz R Mattison T Mukherjee A Osborne L Pitt R Rosenson L Sandacz A Tartaglia M Taylor FE Verdier R Whitaker S Yeh GP Abolins M Brock R Cohen A Ernwein J Owen D Slate J Weerts H 《Physical review letters》1985,55(6):574-577