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951.
In a spin‐polarized electron gas, Coulomb interaction couples the spin and motion degrees of freedom to build propagating spin waves. The spin wave stiffness Ssw quantifies the energy cost to trigger such excitation by perturbing the kinetic energy of the electron gas (i.e. putting it in motion). Here we introduce the concept of spin–orbit stiffness, Sso, as the energy necessary to excite a spin wave with a spin polarization induced by spin–orbit coupling. This quantity governs the Coulombic enhancement of the spin–orbit field acting of the spin wave. First‐principles calculations and electronic Raman scattering experiments carried out on a model spin‐polarized electron gas, embedded in a CdMnTe quantum well, demonstrate that Sso = Ssw. Through optical gating of the structure, we demonstrate the reproducible tuning of Sso by a factor of 3, highlighting the great potential of spin–orbit control of spin waves in view of spintronics applications. (© 2016 WILEY‐VCH Verlag GmbH &Co. KGaA, Weinheim) 相似文献
952.
We evaluate the spin polarization (Edelstein or inverse spin galvanic effect) and the spin Hall current induced by an applied electric field by including the weak localization corrections for a two-dimensional electron gas. We show that the weak localization effects yield logarithmic corrections to both the spin polarization conductivity relating the spin polarization and the electric field and to the spin Hall angle relating the spin and charge currents. The renormalization of both the spin polarization conductivity and the spin Hall angle combine to produce a zero correction to the total spin Hall conductivity as required by an exact identity. Suggestions for the experimental observation of the effect are given. 相似文献
953.
The reaction of oximes with dichloromethane was carried out in 71–98% yields at 20–30 °C for 2–3.5 h in the presence of sodium hydroxide by combination of benzyldimethyltetradecylammonium chloride and ultrasonication. The main advantage of the present procedure is that the reaction time is much shorter than classical methods. 相似文献
954.
N.V. Rama Rao R. Gopalan M. Manivel Raja V. Chandrasekaran D. Chakravarty R. Sundaresan R. Ranganathan K. Hono 《Journal of magnetism and magnetic materials》2007
SmCo5+x wt% Fe (x=0, 5 and 10) nanocomposite powders were synthesized by mechanical milling and were consolidated into bulk shape by spark plasma sintering (SPS) technique. The evolution of structure and magnetic properties were systematically investigated in milled powders as well as in SPS samples. A maximum coercivity of 8.9 kOe was achieved in spark plasma sintered SmCo5+5 wt% Fe sample. The exchange spring interaction between the hard and soft magnetic phases was evaluated using δM–H measurements and the analysis revealed that the SPS sample containing 5 wt% Fe had a stronger exchange coupling between the magnetic phases than that of the sample with10 wt% Fe. 相似文献
955.
A novel water-soluble solvatochromic molecule, 7-(dimethylamino)-2-fluorenesulfonate (2,7-DAFS), was prepared by a three-step
reaction from 2-nitrofluorene in good overall yield. The pH and solvent effects on the UV-VIS absorption and fluorescence
spectra of 2,7-DAFS have been studied. Protonation of the dimethylamino group switches the absorption from intramolecular
charge-transfer (ICT) to π → π* transition. The ground state pKa value of 2,7-DAFS was determined as 4.51. The fluorescence spectrum of the excited basic form, *(DAFS), shows a structureless
single band with a large Stokes shift, whereas that of the acidic form, *(+HDAFS), exhibits a structured band with a small Stokes shift. The emission intensities of the basic and acidic forms versus
pH/Ho plots show stretched sigmoidal curves and indicate that (1) the rate of deprotonation of *(+HDAFS) is comparable to the fluorescence decay of the species, and (2) the efficient proton-induced quenching of *(DAFS) fluorescence
occurs. The pKa* was estimated as −1.7 from the fluorescence titration curve. The fluorescence maximum of *(DAFS) is blue-shifted as the
polarity of solvent decreases. However, no clear dependency of the emission intensity and spectral half width, and thus fluorescence
quantum yield, on the solvent polarity was revealed. It appears that the fluorescence sensitivity of 2,7-DAFS is 15 ∼ 25 times
greater than the sensitivity of a widely utilized fluorescent probe, 5-(dimethylamino)-1-naphthalenesulfonate. This higher
sensitivity, together with the ease of derivatization, would provide the fluorene-based fluorescent molecules significant
advantages for a variety of applications. 相似文献
956.
A new anthracene-based fluorescent PET sensor 1 with a tridentate ionophore of amide/β-amino alcohol displays very good selectivity and sensitivity for Fe3+ (K
a = 1.6 × 103 M−1) and Hg2+ (K
a = 2.1 × 103 M−1) in CH3CN–H2O (3:7, v/v) with detection limit of 1 μM. More fluorescence enhancement was observed when 1 selectively detected Fe3+ or Hg2+ in CH3CN and its detection limit was up to 0.03 μM. 相似文献
957.
利用一个同型二聚体模型,甲酰胺二聚体,模拟一对肽基团.用量子化学从头计算考察了二聚体中酰胺-I带振动模式之间的振动耦合及其在空间的行为. 研究发现C=O伸缩振动耦合以静电作用为主,耦合有效距离能超过10 oA. 一维和二维红外光谱的激子模拟计算表明,耦合常数的空间依赖性能够清楚地表现在光谱特征中. 这些结果意味着多肽中C=O伸缩振动模式能够在很远的距离相互耦合并产生振动态的离域化. 相似文献
958.
In this work, we devote to explore excited‐state intramolecular proton transfer (ESIPT) behavior for a novel fluorescent molecule naphthalimide‐based 2‐(2‐hydroxyphenyl)‐benzothiazole (HNIBT) [New J. Chem. 2019, 43, 9152.] in toluene and methanol (MeOH) solvents. Exploring weak interactions, stable HNIBT‐enol, and HNIBT‐MeOH‐enol complex can be found in S0 state via TDDFT/B3LYP/6‐311+G(d,p) level. Given photoexcitation, intramolecular hydrogen bond O1? H2···N3 of HNIBT‐enol and HNIBT‐MeOH‐enol is dramatically enhanced, which offers impetus for facilitates ESIPT reaction. After repeated comparisons, we verify the unavailability of intermolecular hydrogen bonding effects between HNIBT‐enol and MeOH molecules. In view of excitation, HOMO (π) → LUMO (π*) transition and the changes of electronical densities indeed impulse ESIPT tendency. Via constructing potential energy curves (PECs), for both HNIBT‐enol and HNIBT‐MeOH‐enol complex, the ESIPT could only occur along with intramolecular hydrogen bond O1? H2···N3. Through comparison, the potential barrier falls from 4.124 kcal/mol (HNIBT‐enol) to 2.132 kcal/mol (HNIBT‐MeOH‐enol). Therefore, we confirm that the ESIPT of the HNIBT system happens more easily in the MeOH solvent compared with the toluene solvent. 相似文献
959.
《印度化学会志》2021,98(10):100150
The traditional methods of synthesis of biguanide drugs generally result in the formation of high levels of waste. In this study, we have developed a simple and green route for the synthesis of olanexidine, the novel antimicrobial compound developed by Otsuka Pharmaceutical Factory Inc. This molecule has been clinically explored in Japan for pre-operative skin preparations. The proposed synthesis scheme is beneficial as it has obviated the use of harmful sodium dicyanamide and has employed the readily available dicyandiamide to facilitate cyanoguanidylation of 3,4-dichlorobenzylamine into 3,4-dichlorobenzylbiguanide. This intermediate was further condensed with 1-bromooctane, using tetrabutyl ammonium bromide as the phase transfer catalyst, in a biphasic solvent system comprising of water and ethyl acetate. The developed method resulted in an overall yield of 76% of olanexidine. 相似文献
960.
氧空位是材料缺陷工程的重要组成. 基于光生氧空位的直接热利用, 实现纯水分解制氢的光热耦合实验, 被认为是太阳能综合利用的有效途径. 以多种制备方法合成的TiO2纳米材料为基础, 研究了多种形貌纳米TiO2及其Fe掺杂改性材料的光热耦合反应能力. 通过高分辨透射电子显微镜(HRTEM)、 X射线衍射(XRD)和电子顺磁共振(EPR)对晶体特征进行表征, 利用漫反射光谱(DRS)、 光致发光(PL)和三电极测试法表征了材料的性能, 并结合密度泛函理论(DFT)计算了产氢反应路径. 研究结果表明, 溶胶-凝胶法制备的纳米颗粒相比水热法制备的纳米片及纳米线, 体相内缺陷较多, 载流子强度高, 光热耦合产氢效果较差. Fe掺杂改性扩展了光响应, 增强了载流子分离和寿命, 降低了电子传输阻抗, 利于光反应过程中光生氧空位的形成, 克服了制氢反应中的关键能垒. 同时, 纳米材料中的缺陷促进了Fe离子的有效掺杂, Fe掺杂TiO2纳米颗粒的光热耦合平均产氢量为9.73 μmol/g, 性能提升达13倍. 相似文献