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41.
Minkin V. I. Gribanova T. N. Starikov A. G. Minyaev R. M. 《Russian Chemical Bulletin》2003,52(3):519-525
The electronic and molecular structure of planar (cyclic and linear) tetra- and hexaatomic clusters (XY)
n
(XY = CC, BN, BeO, LiF; n = 2, 3) was studied using the ab initio CCD(full)/6-311+G** method and density functional approach (B3LYP/6-311+G**). The stability of cyclic clusters C6, B3N3, and Be3O3 with D3h
symmetry is mainly determined by the aromaticity of their -electron systems. 相似文献
42.
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45.
A novel copper molybdate with mixed ligands, [{(Cu·phen)2(tp)}{(Cu·phen·H2O)2(tp)}{Mo4O14}] (phen=1,10-phenanthroline, tp=terephthalate) 1, has been hydrothermally synthesized and structurally characterized. The crystal belongs to monoclinic system, space group P21/c with a=13.1711(7), b=19.6132(10), c=13.6910(7) (A), β=117.6870(10)°, V=3131.8(3)(A)3, Z=2, C64H44Cu4Mo4N8O24, Mr=1946.99, Dc=2.065 g/cm3, F(000)=1920, μ(MoKα) (A) 2.198 mm-1, R=0.0810 and wR=0.2012 for 4233 observed reflections (Ⅰ > 2σ(Ⅰ)). The structural analysis indicates that the title compound contains a discrete tetramolybdate cluster decorated with copper complex fragments and tp ligands bridging the clusters into a wave-like layer. The hydrogen bonding between adjacent layers further extends the compound into a 3-D framework. 相似文献
46.
Yong Li Xiao-Bing Cui Ji-Qing Xu Ke-Chang Li Guang-Hua Li Qing-Xin Yang 《Journal of solid state chemistry》2005,178(1):363-369
Both the homometal cluster [P(ph4)]2[Mo2O2(μ-S)2(S2)2] (1) and [Mo2O2(μ-S)2(Et2dtc)2] (2) (Et2dtc=diethyl-dithiocarbamate) were successfully synthesized by low-temperature solid-state reactions. X-ray single-crystal diffraction studies suggest that compound (1) is a dinuclear anion cluster, and compound (2) is a dinuclear neutral cluster. The two compounds were characterized by elemental analyses, IR spectra and UV-Vis spectra. The third-order non-linear optical (NLO) properties of the clusters were also investigated and all exhibited nice non-linear absorption and self-defocusing performance with moduli of the hyperpolarizabilities 5.145×10−30 esu for (1) and 5.428×10−30 esu for (2). 相似文献
47.
Ulrich Schubert 《Journal of Sol-Gel Science and Technology》2003,26(1-3):47-55
Organically substituted metal alkoxides can be prepared by reaction of the parent alkoxides with complexing organic compounds. The chemical and structural consequences of such substitutions are discussed in this article. Examples are given showing how functional organic moieties, such as polymerizable groups, can be incorporated into sol-gel materials via the complexing ligands. Major structural differences between silica-based and metal-based hybrid materials originate from the different charge/coordination number ratios of silicon and most metals. This results in a high tendency for the molecular building blocks to aggregate. In many cases, metal oxide clusters are formed which are capped by the organic ligands. Such surface-modified clusters are themselves very valuable condensed matter units for materials syntheses. 相似文献
48.
铂锡双金属催化剂上丙烷脱氢反应研究 总被引:2,自引:0,他引:2
对比研究了Sn/Pt比为1;1,2,:1和5:1的原子簇担载于γ-Al2O3上制成的Pt=Sn原子簇催化剂,和用SnCl2和H2PtCl6浸渍制备的相应Sn/Pt比的催化剂对丙烷脱氢生成丙烯的催化性能。 相似文献
49.
利用IR,EXAFS, ~(13)CO同位素交换反应及与NO作用等手段研究了Pt羰基簇合物[Pt_3(CO)_6]~(2-)_n(n=3,4)在NaY分子筛超笼内的合成机理.在氧化样品Pt~(2+)/NaY上300-373 K的还愿羰基化过程中,首先Pt~(2+)与CO反应生成PtO(CO)物种(波数σ_(CO)=2110 cm~(-1)),然后聚集成“Pt_3(CO)_6”(σ_(CO)=2112,1896和1841 cm~(-1)),最后生成深绿色的Pt羰基簇合物Pt_(12)(CO)_(24)]~(2-)/NaY(σ_(CO)=2080,1824 cm~(-1)).“Pt_3(CO)_6”的羰基在室温下能迅速地与~(13)CO发生交换,而[Pt_3(CO)_6]~(2-)_n(n=3,4)的羰基与~(13)CO的同位素交换即使在343 K也进行得很慢,室温下,NO能逐步破坏Pt羰基簇合物的层间和层内Pt-Pt键,得到中间物种“Pt_3(CO)_6”和PtO(CO),同时在气相产生CO_2和N_2O.而由上述两中间物种出发,300-353 K温度下,在CO气氛中的还原羰基化又能可逆地得到原羰基簇合物. 相似文献
50.
The geometries of the most stable isomers of gold telluride systems AuTe, Au2Te, and AuTe2 are determined using the MP2 method. The aspect of gold—telluride interaction, the electron correlation, and relativistic
effects on geometry and stability are investigated at the MP2 and CCSD(T) theoretical levels. The results show that the electron
correlation and relativistic effects are responsible not only for gold—gold attraction but also for additional gold—telluride
interaction. The gold—telluride interaction is strong enough to modify the known pattern of bare gold clusters. Both effects
are essential for determining the geometry and relative stability of this type of systems. 相似文献