全文获取类型
收费全文 | 36614篇 |
免费 | 6781篇 |
国内免费 | 5796篇 |
专业分类
化学 | 27047篇 |
晶体学 | 580篇 |
力学 | 2348篇 |
综合类 | 403篇 |
数学 | 4037篇 |
物理学 | 14776篇 |
出版年
2024年 | 109篇 |
2023年 | 660篇 |
2022年 | 1318篇 |
2021年 | 1437篇 |
2020年 | 1482篇 |
2019年 | 1535篇 |
2018年 | 1327篇 |
2017年 | 1364篇 |
2016年 | 1796篇 |
2015年 | 1988篇 |
2014年 | 2404篇 |
2013年 | 2995篇 |
2012年 | 3492篇 |
2011年 | 3536篇 |
2010年 | 2621篇 |
2009年 | 2693篇 |
2008年 | 2910篇 |
2007年 | 2411篇 |
2006年 | 2238篇 |
2005年 | 1805篇 |
2004年 | 1351篇 |
2003年 | 1136篇 |
2002年 | 1149篇 |
2001年 | 934篇 |
2000年 | 751篇 |
1999年 | 627篇 |
1998年 | 454篇 |
1997年 | 410篇 |
1996年 | 362篇 |
1995年 | 297篇 |
1994年 | 295篇 |
1993年 | 236篇 |
1992年 | 182篇 |
1991年 | 150篇 |
1990年 | 141篇 |
1989年 | 90篇 |
1988年 | 81篇 |
1987年 | 61篇 |
1986年 | 71篇 |
1985年 | 47篇 |
1984年 | 24篇 |
1983年 | 30篇 |
1982年 | 13篇 |
1981年 | 14篇 |
1980年 | 9篇 |
1979年 | 19篇 |
1978年 | 7篇 |
1977年 | 11篇 |
1957年 | 8篇 |
1925年 | 10篇 |
排序方式: 共有10000条查询结果,搜索用时 15 毫秒
151.
采用基于第一性原理的密度泛函理论研究了四角晶相二氧化铪(t-HfO2)体相及 其(001)表面的原子几何与电子结构.理论计算结果表明,t-HfO2(001)表面不会 产生重构现象.与体相电子结构相比, t-HfO2(001)表面态密度明显高于体相态 密度.其次,表面原子的态密度更靠近费米能级(EF),价带往低能量处移动,并 有表面态产生.计算结果表明了t-HfO2表面禁带宽度明显低于体相的禁带宽度. t-HfO2(001)的表面态产生以及表面禁带宽度减小是由于Hf原子与O原子的配位 数减少,表面原子周围的环境发生变化而引起的.
关键词:
密度泛函理论
2(001)')" href="#">t-HfO2(001)
表面电子结构 相似文献
152.
153.
We report the demonstration of passively continuous-wave mode-locking(CWML) of diode-pumped Tm,Ho:YV04 laser using an InGaAs/GaAs multiple quantum-well(MQW) structure semiconductor as the saturable absorber.Stable mode-locking pulses at the central wavelength of 2 041 nm are obtained. The maximum output power is 151 mW.The pulse duration is 10.5 ps at the repetition rate of 64.3 MHz. 相似文献
154.
155.
156.
Weijun Liu Guihua Chen Guanghong He Wei Zhang 《Journal of nanoparticle research》2011,13(7):2705-2713
In this study, single-crystalline starfish-like cuprous oxide (Cu2O) nanocrystals with the backbones lengths in the range of 660 nm~16 ??m are successfully prepared through ??-irradiation, the cetyltrimethylammonium bromide (CTAB) is used as a capping material or soft colloidal templates. Without the addition of CTAB in the reaction system, irregular Cu2O nanoclusters were obtained and their diameter is about 200 nm~1 ??m. Controlling the concentration ratio of CTAB to the copper ions, starfish-like morphology of Cu2O can be obtained in high yield. Their structures are characterized by X-ray diffraction, scanning electron microscopy, and high-resolution transmission electron microscopy. The possible growth mechanism of the starfish structure is discussed in the text. For potential application in lithium-ion batteries, an electrode made of the starfish-like Cu2O shows excellent electrochemical cycling performance and high-rate capability. Compared with the Cu2O nanoclusters, the starfish-like Cu2O exhibits an improved electrochemical cycling stability. The capacity of the starfish-like Cu2O can maintain 340 and 215 mAh g?1 after 50 cycles at the rate of 0.1 C and 5 C, respectively. The reversible capacity holds 60% as the discharge?Ccharge rate even increases by 50 times. 相似文献
157.
Within the framework of effective-mass approximation, the effects of a laser field on the ground-state donor binding energy in zinc-blende (ZB) GaN/AlGaN quantum well (QW) have been investigated variationally. Numerical results show that the donor binding energy is highly dependent on QW structure parameters and Al composition in ZB GaN/AlGaN QW. The laser field effects are more noticeable on the donor binding energy of an impurity localized inside the QW with small well width and low Al composition. However, for the impurity located in the vicinity of the well edge of the QW, the donor binding energy is insensible to the variation of Al composition, well width and laser field intensity in ZB GaN/AlGaN QW. In particular, the competition effects between laser field and quantum confinement on impurity states have also been investigated in this paper. 相似文献
158.
We study constraints on neutrino properties for a class of bi-large mixing See-Saw mass matrices with texture zeros and with the related Dirac neutrino mass matrix to be proportional to a diagonal matrix of the form diag(ε,1,1). Texture zeros
may occur in the light (class a) or in the heavy (class b) neutrino mass matrices. Each of these two classes has 5 different forms which can produce non-trivial three generation mixing with
at least one texture zero. We find that two types of texture zero mass matrices in both class a and class b can be consistent with present data on neutrino masses and mixing. None of the neutrinos can have zero masses and the lightest of the light neutrinos has a
mass larger than about 0.046 eV for class a and 0.0027 eV for class b. In these models although the CKM CP violating phase vanishes, the non-zero Majorana phases can exist and can play an important role in producing the observed baryon asymmetry in our
universe through leptogenesis mechanism. The requirement of
producing the observed baryon asymmetry can further distinguish
different models and also restrict the See-Saw scale to be in the
range of 1012~1015 GeV. We also discuss RG effects on V13. 相似文献
159.
Based on the effective-field theory with self-spin correlations and the differential operator technique,physical properties of the spin-2 system with biaxial crystal field on the simple cubic, body-centered cubic, as well as faced-centered lattice have been studied. The influences of the external longitudinal magnetic field on the magnetization,internal energy, specific heat, and susceptibility have been discussed in detail. The phenomenon that the magnetization in the ground state shows quantum effects produced by the biaxial transverse crystal field has been found. 相似文献
160.
XiGuang Cao Xun Chen YunHua Chen XiangYi Cui DeQing Fang ChangBo Fu Karl L. Giboni HaoWei Gong GuoDong Guo Ming He Jie Hu XingTao Huang XiangDong Ji YongLin Ju ShaoLi Li Qing Lin HuaXuan Liu JiangLai Liu Xiang Liu Wolfgang Lorenzon YuGang Ma YaJun Mao KaiXuan Ni Kirill Pushkin XiangXiang Ren Michael Schubnell ManBing Shen YuJie Shi Scott Stephenson AnDi Tan Greg Tarlé HongWei Wang JiMing Wang Meng Wang XuMing Wang Zhou Wang YueHuan Wei ShiYong Wu MengJiao Xiao Xiang Xiao PengWei Xie Tao Ye YingHui You XiongHui Zen Hua Zhang Tao Zhang HaiYing Zhao Li Zhao XiaoPeng Zhou ZhongHua Zhu 《中国科学:物理学 力学 天文学(英文版)》2014,57(8):1476-1494