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31.
We report measurements of the circular polarization correlation parameterP 3 for the excitation of the 4s′[1/2] j=1 state in Ar by 40 eV electrons and for the excitation of the Kr 5s[3/2] J=1 state by 30 eV electrons at electron scattering angles up to 50°. The measured Ar data are compared to predictions of a distorted wave Born approximation (DWBA). The agreement is in general not very good with theory predictingP 3 values considerably larger than the measured values in the regime of small scattering angles. In Kr, where the measured data are compared to theoretical predictions from a DWBA, a first-order many-body theory (FOMBT) and a relativistic distorted wave theory (RDW), the level of agreement between experiment and theory is somewhat better. The measuredP 3 parameters in conjunction with the previously measured linear coherence parametersP 1 undP 2 under the same scattering conditions yield the total polarizationP tot + which is a measure for the level of coherence in the excitation process. In both cases studied here, we found values of eliminateP tot + that were consistent with a fully coherent excitation process.  相似文献   
32.
The high pressure behaviour of InI is studied by DFT‐calculations and compared with experimental data. The existence of a 5s2 electron pair in In+ represents an unfavourable bonding situation for high symmetry structures because of effective closed shell repulsion. Since cations with a ns2 electron pair are highly polarizable and the electronic situation is more favourable in the low symmetry structure InI prefers a TlI‐type structure at ambient pressure. A pressure induced transition to the more densely packed high symmetry CsCl‐type structure takes place at about 19 GPa according to our calculations. At ambient pressure the interactions are predominantly ionic. However with increasing pressure the distances between In+ cations in the TlI‐type structure diminish drastically, mainly due to the changing space requirement of the lone electron pair. Apart from ionic interactions further bonding interactions between the In+ cations occur. At elevated pressure the electron localization function (ELF) as well as the band structure diagrams suggest metallic bonding between the In+ within the zigzag chain, i. e. increasing bonding interactions between the In+ cations due to the electron pair and its s‐p‐mixing. At ambient pressure In‐In interactions are rather weak and the space requirement of the lone electron pair mainly determines the characteristic arrangement of the ions. At elevated pressure the In‐In interactions become stronger and stabilise themselves additionally the specific structural arrangement.  相似文献   
33.
Zusammenfassung Es wurde eine direkte Bestimmung des 3,4-Benzpyrens in wä\riger Lösung beschrieben, die auf der Löslichkeitserhöhung beruht, die das in Wasser schwer lösliche 3,4-Benzpyren durch Coffein erfährt. Es können so noch 4 ng/ml bei der angegebenen Standardisierung bestimmt werden. Bei der Direktbestimmung des 3,4-Benzpyrens im System Coffein-Wasser ist ein pH >6,0 einzuhalten, da bei höheren Wasserstoffionenkonzentrationen die Fluorescenzintensität stark abnimmt.
Direct fluorimetric determination of benzo(a)pyrene in aqueous medium
A method for the direct determination of benzo(a)pyrene in aqueous solution is based on the increase of its solubility by coffeine. 4 ng of benzo(a)pyrene/ml can be determined by the procedure described. In this direct determination in the system coffeine-water the pH has to be adjusted to >6.0, as the fluorescence intensity considerably decreases with higher H+ concentrations.


Eine ausführliche Darstellung findet sich in der Dissertation von G. Becker, Univ. Karlsruhe 1968.

Die Messungen zu dieser Arbeit -wurden an dem Chemischen Untersuchungsamt für das Saarland, Saarbrücken, mit einem Spektralphotometer der Deutschen Forschungsgemeinschaft ausgeführt. Beiden Institutionen sind wir zu Dank verpflichtet.  相似文献   
34.
The Gas Complex MnAlF5 and its Influence on the Purification of AlF3 by Sublimation The gas complex MnAlF5 has been determined mass spectroscopically by the ions MnAlF5+ and MnAlF4+. The gas complex MnAlF5 is formed above 973 K by heating up mixtures of AlF3/MnF2 or AlF3 · 3 H2O endowed with Mn2+ or by heating up solid MnAlF5 too. At 1 008 K the enthalpie of dissociation is 197 kJ/mole. The equilibrium structures of the high spin molecule MnAlF5 (S = 5/2) were examined with ab initio calculations at the HF-level by comlete gradient optimizing. Two minimum structures were found on the potential energy surface. A bidentate fluorine bridged structure was found to be the most stable at the HF-level. Vibrational frequencies and thermodynamic functions of complex formation were estimated for both minimum structures. The importance of the formation of the gas complex for the separation of MnF2 and AlF3 by sublimation is discussed.  相似文献   
35.
Acyl- and Alkylidenephosphines. XXIII. Synthesis and Structure of [Bis(trimethylsilylsulfano)methylidene]phosphines Analogous to the phenyl derivative 1a [2] tert-butyl- 1b , mesityl- 1c and methylbis-(trimethylsilyl)phosphine 1 d react with carbon disulfide to give the corresponding [bis(trimethylsilylsulfano)methylidene]phosphines 4 . Only in case of the mesitylphosphine 1 c the intermediate compounds 2 and 3 could be detected by n.m.r. spectroscopic methods; thermally unstable [bis(trimethylsilylsulfano)methylidene]methylphosphine 4 d dimerizes rapidly [1]. [Bis(trimethylsilylsulfano)methylidene]phenylphosphine 4 a crystallizes in the monoclinic centrosymmetric space group P21/c with following dimensions of the unit cell determined at ?95 ± 3°C: a = 1386.4(8); b = 1036.0(7); c = 1281.7(8) pm; ß = 101.23(4)°; Z = 4. An X-ray structure determination (R = 0.032) proves the constitution of this compound as already derived from its nmr spectra. Characteristic bond lengths and angles are: P?C 170; P? C(phenyl) 183; C? S 176; S? Si 219 pm; C? P?C 107; P?C? S 124 and 120; S? C? S 116 and C? S? Si 111°.  相似文献   
36.
Acyl- and Alkylidenephosphines. XVIII. Monoacetyl- and Diacetylphosphine When triacetylphosphine 3a is treated with methanol 4 or benzyl alcohol 6 P? C(O) bonds are cleaved and a mixture of diacetyl- 2a and monoacetylphosphine 1a is formed. The thermally labile phosphine 1a decomposes completely within a few hours at +20°C; but 2a also reacts slowly within days to give triacetylphosphine 3a and further unknown compounds. As it is found by nmr-spectroscopic studies the acidic hydrogen atoms of monoacetylphosphine 1a are both bound to phosphorus. In liquid diacetylphosphine 2a or in solutions of this compound, However, there exists an equilibrium between the keto tautomer K- 2a with a PH and the enol tautomer E- 2a with an O? H? O group; compared with pentane-2,4-dione 8a the keto tautomerpredo minates in 2a . As in 1,3-diketones a low temperature and a small dielectric constant of the solvent increase the amount of enol tautomer E- 2a present. The 1H-nmr resonance of the enolic hydrogen atom is observed at very low field (δ = 18,3 ppm).  相似文献   
37.
Acyl- and Alkylidenephosphines. XXII. Synthesis and Structure of 1, 3-Dimethyl-2,2,4,4-tetrakis(trimethylsilylsulfano)-1,3-diphosphetane At ?30°C methylbis(trimethylsilyl)phosphine reacts with carbon disulfide to give a red adduct first which rearranges to [bis(trimethylsilylsulfano)methylidene]methylphosphine 1a . In contrast to the thermally stable phenyl derivative 1b [2], this compound with its insufficiently shielded P?C group dimerizes fast with increasing temperature. 1,3-Dimethyl-2,2,4,4-tetrakis(trimethylsilylsulfano)-1,3-diphosphetane 2a formed by this reaction, crystallizes in the triclinic space group P1 with following dimensions of the unit cell, determined at a temperature of measurement of ?80 ± 3°C: a = 1024.7(3); b = 1360.2(5); c = 1326.3(6)pm; α = 117.85(4); ß = 111.05(3); γ = 72.09(3)°; Z = 2. Due to ring folding at the P1? P2 axis of 149.1°, the molecule shows pseudosymmetry Cs. Characteristic averaged bond lengths and angles obtained at an Rw-value of 0.030, are: P? C(endocyclic) 188 and 191; P? CH3 184; C? S 183; S? Si 216 pm; C? P? CH3 105; P? C? S 113; S? C? S 114; C? S? Si 108; P? C? P 90 and C? P? C 86°.  相似文献   
38.
Molecular and Crystal Structure of 1,4-Bis[tris(tetrahydrofuran)lithium]-octaphenyltetrasilane 1,4-Dilithium-octaphenyltetrasilane prepared from octaphenyl-cyclo-tetrasilane and lithium in tetrahydrofuran (THF) [4], can be isolated from tetrahydrofuran/n-pentane as an adduct with six molecules of tetrahydrofuran per formula unit. The orange-red compound crystallizes in the triclinic space group P1 {a = 1159.6(3); b = 1268.4(2); c = 1367.8(3) pm; α = 92,23(2)° β = 113.79(2)° γ = 111.62(2)° at ?5 ± 3°C; Z = 1}. An x-ray structure determination (Rw = 0.046) shows the existence of a centrosymmetric molecule with an extended planar Li? Si4? Li unit; either lithium atom is bound to silicon and to the oxygen atoms of three molecules of tetrahydrofuran. Characteristic bond lengths and angles are: Li? Si 271; Si? Si 241 and 243; Si? C 190 to 192 pm; Li? Si? Si 126°; Si? Si? Si 127°. 29Si and 7Li n.m.r. measurements at low temperatures indicate the presence of three different adducts.  相似文献   
39.
Mono-, di- and tri-alkyl-substituted allenes were potentiostatically oxidized in methanol at graphite and Pt anodes. At the former electrode, α-methoxylated ketones (due to 4F/mole electricity consumption) and esters (6F/mole) were the major products. At a Pt anode, intermediate products such as vinyl-ether derivatives (2F/mole) were characterised too. Unlike the anodic oxidation of alkenes and alkynes previously reproted in the literature, dimerisation is not a typical process in the allenes' oxidation, since of all the products obtained only a sole dimer has been observed. The mechanism for the formation of most products is discussed.  相似文献   
40.
Preparation and Properties of Formed Aluminium Oxide. I. Influence of the Precipitation Conditions of the Boehmite Hydrogel on the Pore Structure of Formed Aluminium Oxide A report is given on the influence of the precipitation conditions of boehmite (pH value, temperature, concentration and residence time in the precipitation suspension) on the cavity structure of aluminium oxide spheres, made by coagulation of boehmite hydrosol in ammonia liquor and subsequent thermal treatment at 110 and 600°C. The boehmite hydrogel was obtained at continuous precipitation conditions by neutralisation of sodium aluminate solution with nitric acid. It is shown that the difference in the pore structure of the formed aluminium oxide obtained by varying the precipitation conditions were caused by the special morphological features of the boehmite crystallization in the precipitation process.  相似文献   
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