首页 | 本学科首页   官方微博 | 高级检索  
文章检索
  按 检索   检索词:      
出版年份:   被引次数:   他引次数: 提示:输入*表示无穷大
  收费全文   693篇
  免费   19篇
  国内免费   1篇
化学   324篇
晶体学   4篇
力学   19篇
数学   55篇
物理学   311篇
  2021年   9篇
  2020年   5篇
  2019年   7篇
  2018年   3篇
  2017年   8篇
  2016年   17篇
  2015年   12篇
  2014年   10篇
  2013年   22篇
  2012年   32篇
  2011年   49篇
  2010年   24篇
  2009年   21篇
  2008年   28篇
  2007年   41篇
  2006年   23篇
  2005年   23篇
  2004年   35篇
  2003年   27篇
  2002年   39篇
  2001年   12篇
  2000年   15篇
  1999年   10篇
  1998年   10篇
  1997年   5篇
  1996年   7篇
  1995年   12篇
  1994年   12篇
  1993年   6篇
  1992年   17篇
  1991年   11篇
  1990年   13篇
  1989年   16篇
  1988年   8篇
  1987年   13篇
  1986年   4篇
  1985年   12篇
  1984年   6篇
  1983年   6篇
  1982年   5篇
  1981年   10篇
  1980年   9篇
  1979年   4篇
  1978年   5篇
  1977年   3篇
  1976年   5篇
  1975年   10篇
  1974年   4篇
  1973年   5篇
  1969年   3篇
排序方式: 共有713条查询结果,搜索用时 15 毫秒
101.
102.
103.
104.
105.
Specific heat measurements of a single crystal of the organic metal (BEDT-TTF)2KHg(SCN)4 have been carried out at low temperatures and under a magnetic field of up to 14 T. A jump in the specific heat of about 0.1 J/mol·K, which corresponds to the antiferromagnetic phase transition, has been observed. The magnetic field is found to decrease the transition temperature at any field orientation. The strongest effect was found to take place in the field direction along the highly conducting ac plane. Zh. éksp. Teor. Fiz. 113, 1058–1063 (March 1998) Published in English in the original Russian journal. Reproduced here with stylistic changes by the Translation Editor.  相似文献   
106.
A single sideband (SSB) receiver has been developed and implemented for use with a submillimeter sideband generator. While the sideband generator emits both an upper and lower sideband, and even some unshifted laser radiation, the receiver responds to only one sideband. The operator of the system can choose which sideband to receive. Rejection of the undesired signal is accomplished through selective frequency shifting coupled with the use of a commercially available single-sideband microwave mixer.  相似文献   
107.
108.
We have measured the electronic lifetimes of the systems Mo(W), Mo(Ru), Mo(Fe) and Mo(U). The concentrations were ≈ 370PPM, 70PPM, 20PPM, and 50PPM respectively. For the first three systems, only the hole octahedron centered atH was investigated thoroughly for all angles and the data inverted to get point lifetimes. For Mo(U) the investigation was done over the entire Fermi surface with the aid of an on-line PDP 11/20 mini-computer. Only selective points were used on other pieces of the Fermi surface in order to avoid problems with degenerate frequencies. A careful determination of the effective masses was also made at all angles under investigation. The masses were found to be in disagreement with those of Leaver and Meyers (these masses were used in our orginal investigation) by as much as 20% in some orientations. The electronic lifetimes were nearly isotropic on the hole octahedron in all the alloy systems investigated. In Mo(U) the isotropy was found to extend to all thed-like surfaces. Only thes-p-like hole ellipsoids centered atN possibly have a substantially different lifetime, but its measurement is inaccurate due to beats from degenerate and many close-lying frequencies.  相似文献   
109.
The utility of theta function-modulated plane wave bases — the modulation is essentially by site-centered Gaussians — in the band problem is shown. The Kronig-Penney model is used as a test system.  相似文献   
110.
Positron lifetimes have been measured as a function of temperature in 4-butyloxybenzal-4′-ethylaniline (BEA). BEA has been previously reported to have two liquidcrystalline phases (smectic and nematic) with transition temperatures as follows: solid → smectic, 40.5° C; smectic → nematic, 51.0° C; and nematic → isotropic liquid, 65.5° C. Positron life time spectra were resolved into two components, with the shorter component τ1 remaining approximately constant in all phases, and τ2 exhibiting reversible changes at all of the above transitions. In addition, an irreversible discontinuity in the τ2 lifetime was observed in the vicinity of 28° C, indicating the presence of a new phase (phase X) of BEA. The τ2 andI 2 values obtained for the various phases of BEA are: solid (1.25 nsec, 7.1%), phase X (1.97 nsec, 26.2%), smectic (2.36 nsec, 23.6%), nematic (2.72 nsec, 28.3%), and isotropic liquid (2.69 nsec, 29.8%).  相似文献   
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号