收费全文 | 2841篇 |
免费 | 739篇 |
国内免费 | 115篇 |
化学 | 568篇 |
晶体学 | 6篇 |
力学 | 304篇 |
综合类 | 66篇 |
数学 | 242篇 |
物理学 | 2509篇 |
2024年 | 11篇 |
2023年 | 47篇 |
2022年 | 72篇 |
2021年 | 122篇 |
2020年 | 100篇 |
2019年 | 64篇 |
2018年 | 92篇 |
2017年 | 132篇 |
2016年 | 158篇 |
2015年 | 158篇 |
2014年 | 278篇 |
2013年 | 178篇 |
2012年 | 184篇 |
2011年 | 235篇 |
2010年 | 181篇 |
2009年 | 176篇 |
2008年 | 198篇 |
2007年 | 147篇 |
2006年 | 146篇 |
2005年 | 153篇 |
2004年 | 126篇 |
2003年 | 134篇 |
2002年 | 85篇 |
2001年 | 92篇 |
2000年 | 71篇 |
1999年 | 47篇 |
1998年 | 52篇 |
1997年 | 38篇 |
1996年 | 40篇 |
1995年 | 31篇 |
1994年 | 21篇 |
1993年 | 20篇 |
1992年 | 16篇 |
1991年 | 10篇 |
1990年 | 12篇 |
1989年 | 9篇 |
1988年 | 12篇 |
1987年 | 10篇 |
1986年 | 4篇 |
1985年 | 7篇 |
1984年 | 7篇 |
1983年 | 4篇 |
1982年 | 6篇 |
1977年 | 1篇 |
1976年 | 1篇 |
1974年 | 1篇 |
1973年 | 2篇 |
1971年 | 1篇 |
1970年 | 1篇 |
1969年 | 1篇 |
The dispersion function depends on transport time in the centre of the transport tube, as related to carrier gas flow rate and tube volume and on the relation between carrier gas flow rate and ablation chamber volume. The equations describing the signal shape standardize signals from different systems and allow quantitative optimization of the ablation chamber, the transport tube and the detector.
Application of the model to ICP-MS shows that only a part of the area filled by the transported vaporization product and thus only a part of the transported vaporization product can be observed at the detector. The model is able to quantify both fractions.
As was calculated, the observed fraction of analyte is always higher than the observed fraction of the sample containing cross section and depends on the chosen transport parameters characterising the dispersion function. Thus, the determination of the signal integrals in the usual way can lead to systematic errors if the parameters influencing the dispersion function are variable.
Therefore, a different method of analysis based on signal equations is proposed and demonstrated. By this method of data treatment, all important system parameters influencing the dispersion function could be calculated and matched with theoretical ones. Furthermore, a complete integral of the transient signal including its statistical variation can be generated from a limited number of measurement points. For example, this can be applied to signals detected incompletely because of detector saturation and enables the use of high-abundance elements as internal standards.
Furthermore, the method can be used to monitor system performance, to identify the flow regime inside the ablation chamber, to take into account the sample volume for quantitative analysis and finally, to detect anomalous signal distributions that would lead to systematic errors. The prospects and limitations of the model are discussed for LA-ICP-MS in single shot mode. 相似文献