全文获取类型
收费全文 | 2223篇 |
免费 | 83篇 |
国内免费 | 15篇 |
专业分类
化学 | 1399篇 |
晶体学 | 21篇 |
力学 | 111篇 |
数学 | 205篇 |
物理学 | 585篇 |
出版年
2023年 | 17篇 |
2022年 | 24篇 |
2021年 | 33篇 |
2020年 | 29篇 |
2019年 | 26篇 |
2018年 | 33篇 |
2017年 | 28篇 |
2016年 | 53篇 |
2015年 | 64篇 |
2014年 | 89篇 |
2013年 | 101篇 |
2012年 | 170篇 |
2011年 | 196篇 |
2010年 | 123篇 |
2009年 | 125篇 |
2008年 | 132篇 |
2007年 | 125篇 |
2006年 | 122篇 |
2005年 | 102篇 |
2004年 | 74篇 |
2003年 | 77篇 |
2002年 | 48篇 |
2001年 | 47篇 |
2000年 | 45篇 |
1999年 | 28篇 |
1998年 | 25篇 |
1997年 | 22篇 |
1996年 | 29篇 |
1995年 | 31篇 |
1994年 | 16篇 |
1993年 | 26篇 |
1992年 | 29篇 |
1991年 | 24篇 |
1990年 | 15篇 |
1989年 | 23篇 |
1988年 | 23篇 |
1987年 | 11篇 |
1986年 | 8篇 |
1985年 | 13篇 |
1984年 | 10篇 |
1983年 | 13篇 |
1982年 | 8篇 |
1981年 | 11篇 |
1980年 | 6篇 |
1979年 | 5篇 |
1978年 | 10篇 |
1976年 | 8篇 |
1975年 | 10篇 |
1974年 | 11篇 |
1973年 | 10篇 |
排序方式: 共有2321条查询结果,搜索用时 15 毫秒
11.
Chuan-Pin Lee Ching-Yuan Liu Ming-Chee Wu Chun-Hua Pan Tsuey-Lin Tsai Hwa-Jou Wei Lee-Chung Men 《Journal of Radioanalytical and Nuclear Chemistry》2013,296(2):1119-1125
The sorption capacity of cesium (Cs) and selenium (Se) in crushed mudrock was demonstrated in this study through a 2-site Langmuir model. To employ such a numerical analysis, batch tests were applied in this study in synthetic seawater and groundwater with sorption/desorption kinetic experiments (time-dependent) and different concentrations (10?2–10?7 M). The 2-site sorption models, which correspond to two rate constants (λ 1 and λ 2), might be more adequate than 1-site sorption models in characterizing Cs and Se sorption/desorption according to the least square errors between the numerical analysis and the results of the batch tests. The fitting results showed that a 2-site Langmuir model is capable of appropriately describing Cs and Se sorption in mudrock. Consequently, the sorption capacity was calculated at about 0.06 mol/kg for Cs and at 0.015 mol/kg for Se. 相似文献
12.
Rung-Ywan Tsai Chung-Ta Cheng Chin-Tien Yang Shuen-Chen Chen Chun-Chieh Huang Shih-Wei Chen Wen-Haw Lu 《Optical Review》2013,20(2):185-188
The application of blue laser lithography for creating antireflective submicron structures on a crystalline silicon substrate was evaluated. The assembled blue laser lithography system was obtained by modifying a commercial blue laser optical pickup head and consisting of a 405-nm-wavelength blue laser and a 0.85-numerical-aperture objective lens. Si substrates were patterned with submicron column patterns of various periods and aspect ratios by blue laser lithography using a sputtered Ge-Sb-Sn-O layer as a resist. The reflectance of the patterned Si substrate decreased to 3% on average in the 300–1000 nm wavelength range, with a low sensitivity to the angle of incident light. Such patterned substrates showed potential for application in crystalline Si solar cells. 相似文献
13.
The synthesis and characterization of [Dy4(dhampH3)4(NO3)2](NO3)2 (1), a new tetranuclear dysprosium (III) complex, is described. The compound was characterized by its X-ray structure, magnetic properties as well as the luminescent spectra. The compound crystallizes in a P1? space group with a zig-zag linear form of geometry. The ac magnetic susceptibilities of the molecule indicate that it is a magnetic molecule with a slow magnetization relaxation. The molecule also exhibits an emission spectrum that was confirmed to be ligand based. These results indicate that this molecule has both a slow magnetization relaxation (that could be potentially a SMM) and luminescent properties. 相似文献
14.
15.
16.
17.
Discrimination of basal cell carcinoma from normal dermal stroma by quantitative multiphoton imaging
Lin SJ Jee SH Kuo CJ Wu RJ Lin WC Chen JS Liao YH Hsu CJ Tsai TF Chen YF Dong CY 《Optics letters》2006,31(18):2756-2758
We performed multiphoton fluorescence (MF) and second-harmonic generation (SHG) imaging on human basal cell carcinoma samples. In the dermis, basal cell carcinomas can be identified by masses of autofluorescent cells with relatively large nuclei and marked peripheral palisading. In the normal dermis, SHG from dermal collagen contributes largely to the multiphoton signal. However, within the cancer stroma, SHG signals diminish and are replaced by autofluorescent signals, indicating that normal collagen structures responsible for SHG have been altered. To better delineate the cancer cells and cancer stroma from the normal dermis, a quantitative MF to SHG index is developed. We demonstrate that this index can be used to differentiate cancer cells and adjacent cancer stroma from the normal dermis. Our work shows that MF and SHG imaging can be an alternative for Mohs' surgery in the real-time guidance of the secure removal of basal cell carcinoma. 相似文献
18.
Prominin‐1‐Specific Binding Peptide‐Modified Apoferritin Nanoparticle Carrying Irinotecan as a Novel Radiosensitizer for Colorectal Cancer Stem‐Like Cells 下载免费PDF全文
Jenny Ling‐Yu Chen Yuan‐Chun Tsai Ming‐Hsien Tsai Shin‐Yu Lee Ming‐Feng Wei Sung‐Hsin Kuo Ming‐Jium Shieh 《Particle & Particle Systems Characterization》2017,34(5)
Resistance of cancer stem cells to radiotherapy remains a major obstacle to successful cancer management. Prominin‐1 (PROM1) is a cancer stem cell marker. Nanoparticle (NP) chemotherapeutics preferentially accumulate in tumors and are able to target cancer and cancer stem‐like cells through cancer cell‐specific ligands, making them uniquely suited as radiosensitizers for chemoradiation therapy. Using a biocompatible apoferritin NP, a PROM1‐targeted NP carrying irinotecan (PROM1‐NP) is engineered. The synergistic effect of the NP and irradiation is evaluated in PROM1‐overexpressing HCT‐116 colorectal cancer cell lines in vitro and in vivo. PROM1‐NP has a size of 17.2 ± 0.2 nm and surface charge of ?13.5 ± 0.2 mV. It demonstrates higher intracellular uptake than nontargeted NP or irinotecan alone. Treatment with PROM1‐NPs decreases HCT‐116 cell proliferation in a dose‐ and time‐dependent manner. In vitro radiosensitization reveals that PROM1‐NP is significantly more effective as a radiosensitizer than nontargeted NP or irinotecan. HCT‐116 tumor xenograft growth is markedly slower following treatment with PROM1‐NP plus irradiation, suggesting that PROM1‐NP is more effective as a radiosensitizer than irinotecan and nontargeted NP in vivo. This study provides the first preclinical evidence of the effectiveness of PROM1‐targeted NP formulation of irinotecan as a radiosensitizer. 相似文献
19.
Jürg Fröhlich Tai-Peng Tsai Horng-Tzer Yau 《Communications in Mathematical Physics》2002,225(2):223-274
We consider the nonlinear Hartree equation describing the dynamics of weakly interacting non-relativistic Bosons. We show
that a nonlinear M?ller wave operator describing the scattering of a soliton and a wave can be defined. We also consider the dynamics of a
soliton in a slowly varying background potential W(ɛx). We prove that the soliton decomposes into a soliton plus a scattering wave (radiation) up to times of order ɛ−1. To leading order, the center of the soliton follows the trajectory of a classical particle in the potential W(ɛx).
Received: 30 June 2000 / Accepted: 25 June 2001 相似文献
20.
Jong-Shenq Guo Hirokazu Ninomiya Je-Chiang Tsai 《Physica D: Nonlinear Phenomena》2010,239(3-4):230-239
Recent experimental studies of photosensitive Belousov–Zhabotinskii reaction have revealed the existence of propagating wave segments. The propagating wave segments are unstable, but can be stabilized by using a feedback control to continually adjust the excitability of the medium. Experimental studies also indicate that the locus of the size of a stabilized wave segment as a function of the excitability of the medium gives the excitability boundary for the existence of 2D wave patterns with free ends in excitable media. To study the properties of this boundary curve, we use the wave front interaction model proposed by Zykov and Showalter. This is equivalent to study a first order system of three ordinary differential equations which includes a singular nonlinearity. Using two different reduced first order systems of two ordinary differential equations, we first show the existence of wave segments for any given propagating velocity. Then the wave profiles can be classified into two types, namely, convex and non-convex types. More precisely, when the normalized propagating velocity is small, we show that the wave profile is of convex type, while the wave profile is of non-convex type when the normalized velocity is close to 1. 相似文献