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81.
龚春慧 FatemiSetareh ProttiNicoletta PostumaIan BortolussiSilva 耿长冉 汤晓斌 AltieriSaverio 《强激光与粒子束》2017,29(12):126004
针对坐落于意大利帕维亚大学的TRIGA Mark II反应堆热柱结构进行优化设计,从而满足面向硼中子俘获治疗(BNCT)的单光子发射计算机断层成像(SPECT)研究要求。为提高计算效率并减小统计误差,对比分析使用SSW/SSR方法与直接使用反应堆为源项时热柱内照射位置处中子能谱,其结果基本一致,从而验证了SSW/SSR方法的可靠性。为在该反应堆开展BNCT中SPECT实验,热柱中子束需准直为笔形束。对比分析四种热柱优化方案下束流口处及探测器处热中子和光子通量:40 cm长石墨(射束口5 cm3 cm);0.5 cm厚硼包裹40 cm长石墨(射束口5 cm3 cm);30 cm长天然锂聚乙烯(射束口直径4 cm);30 cm长天然锂聚乙烯(20 cm长射束口直径5 cm,5 cm长射束口直径4 cm,5 cm长射束口直径2 cm)。结果显示,射束口处热中子通量分别为1.05108,2.52107,6.08107和5.10 107 #/(cm2s)。综合考虑中子准直效果及光子污染,方案三具有最优性能。为后续进行BNCT-SPECT理论和实验研究提供了基础,从而有效促进BNCT剂量准确评估方法的研究进程。 相似文献
82.
A new Mn(II) coordination polymer, [Mn (L1)2(NCS)2]n (1) [L1 = 3,4-bis(4-pyridyl)-5-(2-pyridyl)-1,2,4-triazole] was synthesized by the reaction of ligand L1 and mixtures of manganese(II) acetate and potassium thiocyanate using the heat gradient method. Compound 1 has been characterized by IR spectroscopy, elemental analyses and X-ray crystallography. The crystal structure of compound 1 was determined by single-crystal X-ray diffraction and shows a new interesting one-dimensional coordination polymer. Nanostructures of compound 1 have been synthesized by sonochemical method. The products were characterized by X-ray powder diffraction, scanning electron microscopy (SEM), and IR spectroscopy. The thermal stability of nano particles of compound 1 was studied by thermal gravimetric and differential thermal analyses. 相似文献
83.
利用直流磁控溅射技术在玻璃衬底上沉积了TiO2薄膜,并对其进行了Co离子注入,最后在真空中500 ℃退火50 min,得到系列薄膜样品. 利用剥离-分散方法制备了薄膜的透射电镜样品,并用扫描电镜(SEM)、X射线能量散射谱(EDX)和高分辨透射电镜(HRTEM)对样品做了近似原位观察,研究了薄膜样品中不同Co离子注入深度的成分分布和显微结构. 结果表明,薄膜呈锐钛矿结构,Co元素主要分布在薄膜表层,Co离子的注入使TiO2薄膜的晶粒被部分破坏,并形成CoO,而5
关键词:
2薄膜')" href="#">Co注入TiO2薄膜
电镜原位观察
室温铁磁性 相似文献
84.
F. Gühne 《Isotopes in environmental and health studies》2013,49(6):201-207
Zur Prüfung von Kontaminationsmeβgeräten und zur Beglaubigung von Flächenstrahlungsquellen als Normale wurden im Deutscheti Amt für Meβwesen und Warenprüfung zwei Sälze von Flächenstrahlungsquellen mil den Betastrahlen 90Sr/90Y, 201Tl und 60Co angefertigt. Durch das dabei verwendete Herstellungsverfahren, bei dem je ein Tropfen rudioakliver Lösung in ein Feld eines vorgegebenen Rasters gebracht wurde, konnte eine sehr gleichmäβige Verteilung der akliven Substanz über die Quellenfläche erreicht und eine unmiltelbare Bestimmung der Flächenaktivitätswerte ermöglicht werden. Der besondere Aufbau der Flächenstrahlungsquellen geslatlet es, auf einfache Weise Meβfehler bei Kontaminationsme βgeräten, die durch das Material der Unterlage, auf dem sich die aktive Substanz befindet, und durch die Dicke der akliven Schicht hervorgerufen tcerden, zu erfassen oder zu eliminieren. 相似文献
85.
Mehmet Yaman 《光谱学与光谱分析》2013,32(5):1331-1337
The aim of this study is to examine seasonal changes in Cu and Co concentrations of three plant species for monitoring the effects of pollution in Elazig,Turkey.For this purpose,the leaves of the Pinus nigra L.,Cedrus libani and Cupressus arizonica together with soil samples were collected from different points depending on traffic intensity,nearness the city center and cement factory as well as control location during different months of the year.Flame atomic absorption spectrophotometer(FAAS) was used for measurement of the metals in clear digests after the dry ashing method.Copper and Co concentrations were in the ranges from 1.3to 2.6mg.kg-1 and相似文献
86.
The constants of binding dye molecules with the micelles of sodium dodecyl sulfate are determined using quenching of delayed fluorescence of acridine dyes by sodium iodide in aqueous–micellar solutions. Kinetic equations have been composed that describe the processes of deactivation of the excited states of dyes. By solving these equations at the concentration of the quencher sodium iodide corresponding to the minimum lifetime of triplet states and at the concentration of micelles corresponding to the least value of the delayed fluorescence quenching rate constants, we obtained the constants of binding dyes with micelles equal to 1.3·107, 2.9·107, and 3.1·107 M–1 for trypaflavine, acridine orange, and acridine yellow, respectively. We calculated the rate constants of quenching of the triplet states of the molecules of dyes by iodide ions (I
–) that decreased in transition from trypaflavine to acridine orange and acridine yellow. 相似文献
87.
本文利用激光透镜效应在激光束腰前后的反对称效应,以双样品池差分法对Co进行定量测定。单样品池和双样品池的最低可测浓度分别为5ng/ml和2ng/ml。分析灵敏度高于常规的分光光度计法10倍。He-Ne激光束功率为2mw。 相似文献
88.
Theoretical studies of cobalt(I)‐catalyzed hydroacylation of vinylsilanes and alkyl aldehydes 下载免费PDF全文
Density functional theory (DFT) was used to investigate computationally cobalt(I)‐catalyzed hydroacylation of vinylsilanes and alkyl aldehydes to give ketones. Calculation indicated that cobalt(I)‐catalyzed hydroacylation had eight possible reaction pathways. In the cobalt‐hydride complexes IM2a and IM2b, the hydrogen migration occurred prior to the carbon–carbon bond‐forming reaction. In the complexes IM3a1 and IM3b1, the carbonyl elimination reaction occurred prior to the direct reductive elimination reaction. In the cobalt–carbonyl complexes IM4a and IM4b, the carbonyl insertion reaction was much easier to achieve than the decarbonylation reaction. The dominant reaction pathway was the reaction channel IM1a → TS1a → IM2a → TS2a1 → IM3a1 → TS4a → IM4a → TS5a → IM5a → TS6a → IM6a, and the reductive elimination reaction was the rate‐determining step for this channel, so the dominant product predicted theoretically was the linear ketone. Furthermore, the solvation effect was remarkable, and it decreased generally the free energies of the species. Copyright © 2015 John Wiley & Sons, Ltd. 相似文献
89.
以高锰酸钾降解薛氏钠盐(6-羟基-β-萘磺酸钠)合成4-磺基邻苯二甲酸,并以此为原料“固相熔融法”合成了四磺基酞菁钴(CoPcS4)。CoPcS4在DMSO中发生解聚,随着pH值的升高,解聚增加。CoPcS4以二聚体形式与牛血清白蛋白(BSA)结合后具有更强的光敏活性。分别采用紫外和荧光光谱分析方法准确测定了四磺基酞菁钴与BSA的结合位置数和结合常数。两种方法的结果基本一致,数量级皆为105 L·mol-1。CoPcS4与BSA的首要结合位置为SiteⅠ和SiteⅡ,两种结合位置的结合能力差别不大。结果表明,CoPcS4可与牛血清白蛋白很好地结合,白蛋白起到存储与转运作用。 相似文献
90.
Sølvi Storsæter 《Surface science》2006,600(10):2051-2063
The heats of adsorption of different C1 and C2 molecules assumed to be present during the initial steps of the Fischer-Tropsch synthesis and activation energies for elementary steps envisioned to occur in the synthesis are calculated for Co by using the unity bond index-quadratic exponential potential (UBI-QEP) method. The preexponential factors for the elementary steps are calculated from transition-state theory, and the rate constants are calculated according to the Arrhenius equation. The activation barrier for hydrogenation of CO is found to be lower compared to hydrogen assisted dissociation of CO, which has a smaller activation barrier than direct dissociation of CO. The reaction steps with high activation barriers are eliminated. Based on this elimination two sets of elementary steps for formation of C1 and C2 alkenes and alkanes in the Fischer-Tropsch synthesis are established: one based on hydrogen assisted CO dissociation (carbide mechanism) and one based on CO hydrogenation (CO insertion mechanism). In addition, one mechanism of producing CO2 from the water-gas shift reaction is proposed. The resulting mechanisms are combined and used in the microkinetic model, which are fitted to experimental results at methanation conditions (T = 483 K or 493 K, p = 1.85 bar and H2/CO = 10) over a Co/Al2O3 Fischer-Tropsch catalyst. A good tuning is obtained by adjusting the C-Co and H-Co binding strengths. The microkinetic modelling based on these assumptions indicates that CO is mainly converted through hydrogenation of CO and that C2 compounds are mainly produced by insertion of CO into a metal-methyl bond. Thus, from the surface coverages and reaction rates predicted by the microkinetic modelling the mechanism can be further reduced to only include the CO insertion mechanism. Hydrogenation of CHO to CH2O is found to be the rate determining initiation step, and insertion of CO into a metal-methyl bond is found to be the rate determining step for chain growth. By using the UBI-QEP method for calculation of activation energies, the activation barriers for dissociation of CO and hydrogenation of surface carbon are found to be too large for the carbide mechanisms to occur. However, experimental data or another theoretical method is necessary in order to support or disprove the calculated activation energies in this work. 相似文献