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341.
以生成I(L)拓扑空间为基础,首先引入了Ω_L,I_L等算子及I(L)-fuzzy拓扑空间的概念,其次研究了该拓扑空间的基本性质及算子的相应运算规则,最后讨论了此拓扑空间与I(L)-fuzzy拓扑空间的关系.得到了生成I(L)-fuzzy拓扑空军的相应性质. 相似文献
342.
定向诱导基因组局部突变技术(Targeting Induced Local Lesions IN Genomes, 简称TILLINC)是一种全新的、高通量和低成本反向遗传学研究方法。近年来, 随着突变筛选技术的革新, TILLING技术平台日趋多元化, 使得TILLING技术的操作更为简单﹑快速, 并广泛应用于作物育种研究领域。简要介绍了TILLING技术平台的最新发展动态, 并初步探讨了将辐射诱变处理与TILLING高通量筛选相结合在诱变育种中的应用前景。To investigate the M1 biological effects of heavy ions irradiation on Lycopersicon esculentum Mill., its seeds were irradiated by 12C6+heavy ions (80 MeV/u) with the dosages of 30, 60, 90, 120 and 160 Gy respectively . The results showed that with doses increased gradually, germination rate and seedling rate of Lycopersicon esculentum Mill. were decreased, and the latter was lower than the former, mainly due to the inhibition of root growth. The irradiation increased the content of MDA and proline evidently, showing irradiation could damage biomembrane, and also decreased the activities of POD and SOD with distinct inhibition pattern. However, the low dose and high dose irradiation promoted APX activity, illustrating APX was induced to protect irradiation injury. In brief, exposure to 12C6+ heavy ions had obvious injury effects on the seeds of Lycopersicon esculentum Mill.. Heavy ions irradiation damaged biomembrane, inhibited activities of enzymes, and finally inhibited the growth of the first generation of these seeds. 相似文献
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MesomorphicCharacteristicsofInducedChiralNematicPhaseof[SmecticLCP,PS(4BC/DM)/NematicLC,E7/ChiralDopant,CB┐15]┐TernaryComposi... 相似文献
346.
目前选煤厂煤质检测过程自动化程度低,采样与制样技术需要大量的人工参与。检测技术的落后直接影响数据的准确性从而对整个选煤厂生产过程控制与产品质量控制产生重要影响,直接关系选煤厂的经济效益。面对产业升级的需要,将先进的自动采制样技术引进煤炭生产经营企业是当务之急。机器人采制样系统包含:机械化采样与初制样技术、机器人精细化制样技术、煤炭快速检测技术、自动快速浮沉技术,为选煤厂提供了一种全自动采制检的新技术方案。 相似文献
347.
水体中溶解有机物的荧光光谱特性分析 总被引:2,自引:0,他引:2
以355 nm激光为激发光源,在实验室中利用激光诱导荧光(LIF)方法对不同水体中溶解有机物(DOM)的荧光光谱进行了测量,并以最小二乘法-高斯拟合对水体荧光光谱进行了拟合,解卷积得出了水喇曼散射谱及DOM的荧光光谱.在改变激发光脉冲强度的条件下,以一定浓度腐殖酸溶液为测量样品分析了DOM的荧光饱和特性.结果表明,随着激发光功率密度的增加,水喇曼散射强度线性增加,而DOM的荧光强度随着激发光功率密度的增加先是线性增加,此时归一化荧光强度为一恒定值.当激发光功率密度大于55 mW/cm2时, 荧光强度增加缓慢,归一化荧光强度则逐渐降低.研究发现,在有机物浓度较高时,出现了激发态分子间的单重态-单重态猝灭,并且在低浓度情况下,随着有机物浓度的增加,出现了有机物荧光峰值强度位置的红移并伴有波形的展宽. 相似文献
348.
Kenny Lee Nathaniel Corrigan Cyrille Boyer 《Angewandte Chemie (International ed. in English)》2023,62(44):e202307329
Polymerization induced microphase separation (PIMS) is a strategy used to develop unique nanostructures with highly useful morphologies through the microphase separation of emergent block copolymers during polymerization. In this process, nanostructures are formed with at least two chemically independent domains, where at least one domain is composed of a robust crosslinked polymer. Crucially, this synthetically simple method is readily used to develop nanostructured materials with the highly coveted co-continuous morphology, which can also be converted into mesoporous materials by selective etching of one domain. As PIMS exploits a block copolymer microphase separation mechanism, the size of each domain can be tightly controlled by modifying the size of block copolymer precursors, thus providing unparalleled control over nanostructure and resultant mesopore sizes. Since its inception 11 years ago, PIMS has been used to develop a vast inventory of advanced materials for an extensive range of applications including biomedical devices, ion exchange membranes, lithium-ion batteries, catalysis, 3D printing, and fluorescence-based sensors, among many others. In this review, we provide a comprehensive overview of the PIMS process, summarize latest developments in PIMS chemistry, and discuss its utility in a wide variety of relevant applications. 相似文献
349.
Laser-induced thermal effects on the hexagonal MoO3 nanorods at different power density levels were studied using Raman spectroscopy and scanning electron microscopy techniques. The structural features of the nanorods were accompanied by varying the incident laser power from 8.0 to 600 mW by using a gradual increasing rate and a sudden increasing incident laser power. It was shown that the photoeffects observed on the MoO3 nanorods critically depends on the exposure rate. By gradually increasing the incident laser power up to 600 mW, morphology of the nanorods were completely preserved, and the observed thermal behavior was discussed on the basis of thermal contact at nanoscale. However, when the irradiation intensity was suddenly increased, it was observed that overheating of h-MoO3 nanorods at relatively lower laser powers (80 mW) sublimate the nanorods around the laser spot region. The MoO3 molecules on vapor-phase at high temperatures condense and crystallize next to the laser spot on the orthorhombic (α-MoO3) and monoclinic (β-MoO3) phases. Furthermore, the nanorods closest to the laser spot region undergo a structural phase (and morphological) transition from h-MoO3 phase to α-MoO3 phase. 相似文献