全文获取类型
收费全文 | 5199篇 |
免费 | 1262篇 |
国内免费 | 2453篇 |
专业分类
化学 | 4430篇 |
晶体学 | 241篇 |
力学 | 378篇 |
综合类 | 300篇 |
数学 | 739篇 |
物理学 | 2826篇 |
出版年
2024年 | 10篇 |
2023年 | 51篇 |
2022年 | 165篇 |
2021年 | 149篇 |
2020年 | 159篇 |
2019年 | 153篇 |
2018年 | 138篇 |
2017年 | 248篇 |
2016年 | 150篇 |
2015年 | 266篇 |
2014年 | 284篇 |
2013年 | 405篇 |
2012年 | 404篇 |
2011年 | 418篇 |
2010年 | 444篇 |
2009年 | 486篇 |
2008年 | 563篇 |
2007年 | 475篇 |
2006年 | 515篇 |
2005年 | 495篇 |
2004年 | 347篇 |
2003年 | 293篇 |
2002年 | 272篇 |
2001年 | 309篇 |
2000年 | 333篇 |
1999年 | 179篇 |
1998年 | 117篇 |
1997年 | 111篇 |
1996年 | 91篇 |
1995年 | 86篇 |
1994年 | 101篇 |
1993年 | 105篇 |
1992年 | 80篇 |
1991年 | 69篇 |
1990年 | 64篇 |
1989年 | 60篇 |
1988年 | 54篇 |
1987年 | 41篇 |
1986年 | 52篇 |
1985年 | 36篇 |
1984年 | 36篇 |
1983年 | 21篇 |
1982年 | 19篇 |
1981年 | 15篇 |
1980年 | 5篇 |
1979年 | 9篇 |
1978年 | 8篇 |
1977年 | 4篇 |
1971年 | 3篇 |
1965年 | 5篇 |
排序方式: 共有8914条查询结果,搜索用时 813 毫秒
901.
ZOU Wen-Hua TIAN Yuan SHEN Shui-Fa GU Jian-Zhong PENG Bang-Bao ZHANG Di-Da MA Zhong-Yu 《中国物理C(英文版)》2010,34(1)
Recent years have witnessed intense activity concerning the study of nuclei with equal numbers of neutrons and protons (N = Z). Exotic properties have been exhibited in the N = Z nuclei, especially in those with atomic masses around 80. In the present paper, the projected shell model(PSM)together with a relativistic Hartree-Bogoliubov (RHB) theory is used to study the nuclear structure near the N = Z line in the mass A ≈ 80 region. For three Zr isotopes 80,82,84Zr, the projected potential energy surfaces and ground state bands are calculated. It is shown that shape coexistence occurs in all of these nuclei. Moreover, we find that the residual neutron-proton interaction strongly affects the ground state band of 80Zr; however, it slightly modifies those of 82Zr and 84Zr. 相似文献
902.
目标表面发射率对红外热像仪测温精度的影响 总被引:2,自引:0,他引:2
介绍了红外热像仪测温原理,分析了影响红外热像仪测温精度的因素,计算了不同表面发射率下红外热像仪的测温误差曲线。理论分析表明,目标表面发射率越高,红外热像仪测温精度越高。实验改变表面发射率的设置,计算了不同表面发射率对应的总辐射亮度,得到TP8型长波红外热像仪能够精确测温时,目标表面发射率必须大于0.5的结果。最后,对表面发射率分别为0.96、0.93和0.3的3种材料进行实际测温,结果表明,材料表面发射率较高时,红外热像仪具有较好的测温精度。 相似文献
903.
DONG GuoXiang YU ShaoYing LIU YanXin SHEN CaiWan & DONG YongSheng I School of Science Huzhou Teachers College Huzhou China School of Science Information Engineering Zhejiang Normal University Jinhua 《中国科学:物理学 力学 天文学(英文版)》2010,(1)
Theoretical calculations of the energy bands in nucleus 102 Zr are carried out by taking the projected shell model approach, which has reproduced the experimental data. In addition, by analyzing band-head energies, corresponding configurations of yrast band, quasi-particle rotational bands and side bands, we have worked out the microscopic formation mechanism of axially symmetric deformation bands: The low-excitation deformation bands are attributed to the high-j intruder states 1g 7/2 and 1h 11/2 in the N=... 相似文献
904.
MO Xiao-Hu E.V.Abakumova M.N.Achasov V.E.Blinov CHU Yuan-Ping DONG Hai-Yi FU Cheng-Dong F.A.Harris V.V.Kaminskiy A.A.Krasnov LI Xiao-Nan LIU Qian N.Yu.Muchnoi I.B.Nikolaev E.E.Pyata QU Hua-Min QIN Qing A.G.Shamov SHEN Cheng-Ping G.S.Varner WANG Yi-Fang XU Jin-Qiang ZHANG Jian-Yong ZHANG Qing-Jiang ZHANG Yin-Hong ZHANG Tian-Bao V.N.Zhilich ZHAO Zhuo A.A.Zhukov 《中国物理C(英文版)》2010,34(6)
The beam energy measurement system at BEPCII is composed of there parts: laser source and optics system,laser-electron interaction system and High Purity Germanium(HPGe)detector system.The special components and construction of each part are introduced,especially about radiation background mea-surement in the storage ring,which is of great importance for the safe commissioning of HPGe detector. 相似文献
905.
为了改善腔增强吸收光谱的探测灵敏度和光谱分辨率,通过将激光光束离轴注入光学谐振腔中,减小了谐振腔内振荡,提高了模式密度,使得谐振腔被近似看作为“怀特池”。采用记录波长在扫描过程中实际变化的方法,对光谱数据进行了非线性校正,省去了参考光路的布置,简化了实验光路。对二氧化碳在1.572μm处的一条弱吸收谱线进行了测量,得到了大小为1.98×10^-7cm^-1的最小探测灵敏度。实验结果表明同等实验条件下,光束离轴入射时比正轴入射时的腔增强吸收光谱具有更高的信噪比和光谱分辨率。 相似文献
906.
907.
The rare isotope ^236U has a half-life of 2.342(3)×107 years, and is produced principally by thermal neutron capture on ^235U. The isotopic atom ratio of ^236U/^238U depends on the integral thermal neutron flux received by the material of interest. ^236U is potentially useful as a "fingerprint" for indicating the presence of neutron-irradiated uranium usually originating from nuclear activity. By extracting negative molecular ion UO^- from the uranium oxide target, simulating the ^236U^16O^- beam transport with ^238U^16O^- and ^208Pb2^16O^- pilot molecular ion beam, transporting the ^236U-containing ion beam with a high resolution injection magnet analyzer and electrostatic analyzer system, and finally identifying and detecting ^236U with a time-of-flight detector (TOF), a method for AMS (Accelerator Mass Spectrometry) measurement of ^236U was established on the HI-13 Accelerator AMS system at China Institute of Atomic Energy. 相似文献
908.
XYZ particles at Belle 总被引:1,自引:0,他引:1
In this paper, I review recent progress in the study of the XYZ particles at Belle. I only focus on studies with charmonium and one or more light mesons in the final states. This covers the X(3872), X(3915), Y(4140), X(4350), and the charged Z states. 相似文献
909.
The rare isotope 236U has a half-life of 2.342(3)×107 years,and is produced principally by thermal neutron capture on 235U.The isotopic atom ratio of 236U/238U depends on the integral thermal neutron flux received by the material of interest.236U is potentially useful as a fingerprint for indicating the presence of neutron-irradiated uranium usually originating from nuclear activity.By extracting negative molecular ion UO- from the uranium oxide target,simulating the 236U16O- beam transport with 238U16O- an... 相似文献
910.
A K-N2 mixture is irradiated in a glass fluorescence cell with pulses of 710hm radiation from an OPO laser, populated K2 (^1∧g) state by two-photon absorption. The cross section for ^1∧g →^3∧g transfer in K2 is determined using molecular fluorescence spectrometry. The cell temperature is kept constant at 553K. The N2 pressure is varied between 40 Pa and 400 Pa. The effects of K2-K collisions could not be neglected. These effects are subtracted out by using the results of the pure K experiment. The cross sections are (3.8 ± 1.5) ×10^-15 cm^2 for K2 (^1∧g) + N2 → K2(^3∧g) +N2 and (8.9 ± 3.5) × 10^-15 cm^2 for K2 (^3∧g) collisions with N2. 相似文献