全文获取类型
收费全文 | 3975篇 |
免费 | 847篇 |
国内免费 | 339篇 |
专业分类
化学 | 1685篇 |
晶体学 | 47篇 |
力学 | 287篇 |
综合类 | 73篇 |
数学 | 885篇 |
物理学 | 2184篇 |
出版年
2024年 | 7篇 |
2023年 | 42篇 |
2022年 | 91篇 |
2021年 | 110篇 |
2020年 | 129篇 |
2019年 | 153篇 |
2018年 | 115篇 |
2017年 | 201篇 |
2016年 | 221篇 |
2015年 | 192篇 |
2014年 | 277篇 |
2013年 | 278篇 |
2012年 | 230篇 |
2011年 | 252篇 |
2010年 | 236篇 |
2009年 | 269篇 |
2008年 | 263篇 |
2007年 | 257篇 |
2006年 | 238篇 |
2005年 | 227篇 |
2004年 | 205篇 |
2003年 | 168篇 |
2002年 | 137篇 |
2001年 | 133篇 |
2000年 | 114篇 |
1999年 | 85篇 |
1998年 | 87篇 |
1997年 | 78篇 |
1996年 | 57篇 |
1995年 | 54篇 |
1994年 | 36篇 |
1993年 | 38篇 |
1992年 | 42篇 |
1991年 | 26篇 |
1990年 | 15篇 |
1989年 | 13篇 |
1988年 | 19篇 |
1987年 | 11篇 |
1986年 | 8篇 |
1985年 | 5篇 |
1984年 | 14篇 |
1982年 | 7篇 |
1981年 | 4篇 |
1980年 | 4篇 |
1979年 | 5篇 |
1977年 | 1篇 |
1975年 | 1篇 |
1973年 | 2篇 |
1967年 | 1篇 |
1957年 | 1篇 |
排序方式: 共有5161条查询结果,搜索用时 234 毫秒
921.
922.
流动诱导残余应力是塑料制品产生应力开裂以及翘曲变形等现象的重要原因,对成型过程中流动诱导残余应力研究具有重要意义.推导了基于黏弹性eXtended Pom-Pom本构关系的能量方程,进而建立了描述黏弹性流体非等温充模流动的气-液两相模型.用同位网格有限体积法进行了求解,得到了凝固层和剪切速率分布,给出了充填结束时影响制件力学性能的流动诱导残余应力.结果表明,型腔中凝固层的厚度与注射速率有关,注射速率越大,充模时间越短,凝固层越薄.在制品表层紧邻模壁的地方,剪切速率和残余应力几乎为零;在制品次表层的位置,制件内剪切速率和流动残余应力也较高;而在远离模壁的地方,剪切速率和流动残余应力也较小. 相似文献
923.
在波荡器和扭摆器的研制过程中,为提高磁块的测量效率和精度,提出了2维全自动亥姆霍兹线圈磁块测量方法。通过理论推导得到仅采用2维全自动旋转而不需要3维旋转就可以实现磁块的全自动测量,降低了磁块全自动测量的实现难度。根据该方法的理论,已成功研制出一台2维全自动亥姆霍兹线圈测量装备,并在上海光源的磁块测量中使用。系统地给出2维全自动亥姆霍兹线圈磁块的测量理论和方法,并对测量误差进行了分析,该系统实现了磁块剩磁测量的高效率、高精度和高重复性,可以在30 s内完成单磁块的测量,重复性和精度均好于510-4。 相似文献
924.
当前土壤中的重金属污染日益严重,研究开发便携式土壤重金属快速、现场检测技术设备能为土壤重金属污染状况普查提供快速、有效的技术手段。系统中发射光路采用透镜对激光光束会聚并作用到样品;收集光路采用抛物面镜组对等离子体光信号收集并耦合至光纤。分析了激光光束经透镜汇聚后作用到样品时的功率密度,给出了等离子体光信号耦合至光纤端面的光斑大小,并得到整个光学系统的大小尺寸。结果表明,整个光学系统结构紧凑、体积小、光信号耦合效率高,非常适用于便携式土壤重金属快速、现场的探测系统应用。 相似文献
925.
We experimentally study the generation and storage of double slow light pulses in a Pr3+:Y2SiO5 crystal. Under electromagnetically induced transparency, a single signal pulse is stored in the spin coherence of the crystal. By simultaneously switching on two control fields to recall the stored information, the spin coherence is converted into two slow light pulses with distinct frequencies. Furthermore, the storage and controlled retrieval of double slow light pulses are obtained by manipulating the control fields. This study of double slow light pulses may have practical applications in information processing and all-optical networks. vspace2mm 相似文献
926.
Silver epoxy was selected to bond transducer plates on glass substrates. The properties and thickness of the bonding medium affect the electrical input impedance of the transducer. Thus, the thickness of the silver epoxy bonding layer was used as a design parameter to optimize the structure for the transducer input impedance to match the 50 Ω output impedance of most radio frequency (RF) generators. Simulation and experimental results show that nearly perfect matching is achieved without using any matching circuit. At the matching condition, the transducer operates at a frequency band a little bit below the half-wavelength resonant frequency of the piezoelectric plate. In experiments, lead titanate (PT) piezoelectric plates were employed. Both full-size, 11.5 mm × 2 mm × 0.4 mm, and half-size, 5.75 mm × 2 mm × 0.4 mm, can be well matched using optimal silver epoxy thickness. The transducer assemblies demonstrate high efficiency. The conversion loss from electrical power to acoustic power in soda-lime glass is 4.3 dB. This loss is low considering the fact that the transducers operate at off-resonance by 12%. With proper choice of silver epoxy thickness, the transducer can be matched at the fundamental, the 3rd and 5th harmonic frequencies. This leads to the possible realization of triple-band transducers. Reliability was assessed with thermal cycling test according to Telcordia GR-468-Core recommendation. Of the 30 transducer assemblies tested, none broke until 2900 cycles and 27 have sustained beyond 4050 cycles. 相似文献
927.
The effect of the relative phase (?) between the probe and driving fields on the gain without inversion (GWI) in a Doppler broadened open quasi Λ-type four level atomic system with vacuum induced coherence (VIC) for both co- and counter-propagating probe and driving fields cases is studied. It is shown that: (1) GWI and the probe detuning region in which GWI exists are very sensitive to variation of the relative phase; when values of the other parameters keep unvarying, by adjusting value of ?, the largest GWI can be obtained. (2) The Doppler width (D) also has dramatically modulation role on the phase-dependent GWI. When value of D is smaller, the value of ? which corresponds to the largest value of GWI is about π, when value of D is large enough, it is about π/2. (3) GWI varies periodically with ? varying, the period is 2π, but the concrete variation rule is closely related to value of D. (4) In the co-propagating case we can obtain much larger GWI than that in the counter-propagating case. 相似文献
928.
Nanostructural modifications in a double-graded Pt/Ni/C multi-trilayer, due to irradiation by an energetic ion-beam, have been analyzed using X-ray reflectivity (XRR), X-ray standing wave (XSW) and cross-sectional transmission electron microscopy (X-TEM) techniques. 2 MeV Au2+ ions were rastered on Pt/Ni/C multi-trilayer samples producing a uniformly irradiated area at ion-fluences ranging from 1 × 1014 ions/cm2 to 2 × 1015 ions/cm2. Ion irradiation induced modifications of microstructural parameters, e.g., layer thicknesses and electron densities of individual layers and interface roughnesses have been obtained from XRR analysis. Pt- and Ni-fluorescence yield from the as-deposited sample under the XSW condition show the distinct existence of Pt and Ni layers. The almost indistinguishable Pt- and Ni-fluorescence data over the first order Bragg peak from the sample irradiated at the highest ion-fluence, suggest complete mixing of Pt and Ni. Strong mixing between Pt and Ni in the ion irradiated samples is also corroborated by XRR results. X-TEM studies reveal the individual layer structure in the as-deposited sample. This layer structure is lost in the sample irradiated at the highest ion fluence indicating a complete mixing between Pt and Ni layers and nanoscale grain growth of Pt-Ni alloys. Additionally, formation of Pt-Ni alloy nano-clusters in the C-layers is observed. The results are understood in the light of the positive heat of mixing between Pt and C, and Ni and C and the negative heat of mixing between Pt and Ni. The effect of heat of mixing becomes dominant at high fluence irradiation. 相似文献
929.
930.
激光诱导击穿光谱(LIBS)谱线具有很窄的展宽,且光谱仪因外界温度条件的变化存在波长漂移,光谱数据为离散数字信号,受噪声、谱线重叠及连续背景的影响,信号存在失真和变形。而目前光谱仪自带谱线识别分析软件主要以"就近原则"为主,错误率较高,必须依赖于人眼的观察对比。针对这个问题,在研究LIBS光谱特性的基础上,提出了一种窗口可变滑动相关分析方法(CAASW),用于激光诱导击穿光谱谱线自动识别。以土壤标准物质为样品,对该方法进行了实验分析和评价,与光谱仪自带分析识别软件相比,CAASW明显提高了识别准确率和识别速度,最终实现了谱线的自动识别。 相似文献