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71.
Barabas B Caglioti L Zucchi C Maioli M Gal E Micskei K Pályi G 《The journal of physical chemistry. B》2007,111(39):11506-11510
Enantiomeric excesses obtained in absolute enantioselective synthesis by chiral autocatalysis (Soai-reaction) were statistically analyzed. Two sets of parallel experiments, which were performed under chemically different conditions, are available. One group contains 37, while the other contains 84 preparative results. The former group shows some interesting tendencies but does not give conclusive statistical results. The sample of 84 parallel experiments, providing 39 R- and 45 S-excesses have shown that these data represent two distinct, non-symmetric sets with different non-Gaussian distributions. Clear S preference was found. 相似文献
72.
Thomas Jordan Mark Pollicott Károly Simon 《Communications in Mathematical Physics》2007,270(2):519-544
In this paper we shall consider a self-affine iterated function system in , d ≥ 2, where we allow a small random translation at each application of the contractions. We compute the dimension of a typical
attractor of the resulting random iterated function system, complementing a famous deterministic result of Falconer, which
necessarily requires restrictions on the norms of the contraction. However, our result has the advantage that we do not need
to impose any additional assumptions on the norms. This is of benefit in practical applications, where such perturbations
would correspond to the effect of random noise. We also give analogous results for the dimension of ergodic measures (in terms
of their Lyapunov dimension). Finally, we apply our method to a problem originating in the theory of fractal image compression.
Research of Jordan and Pollicott was supported by the EPSRC and the research of Simon was supported by an EU-Marie Curie grant
and the OTKA Foundation #T42496. 相似文献
73.
László Drahos Károly Vékey 《Journal of the American Society for Mass Spectrometry》1999,10(4):323-328
The mean thermal energy and its distribution has been calculated for various peptides. The table, figures, and analytical expressions provided in the paper can be used to determine the mean thermal energy and its distribution in peptides in a very simple way, without having to use complex mathematics. Accuracy is ∼±6%. The same expressions can be used for most organic compounds with an estimated accuracy of ∼±10%. Data for W(CO)6, the “thermometer molecule,” are also given. 相似文献
74.
75.
76.
Károly Lázár Andjelka Toma?evi? Goran Bo?kovi? Ern? Kiss 《Hyperfine Interactions》2009,192(1-3):23-29
Catalytic performances of Fe-AlPILC (14 wt.% Fe) and Fe-ZSM-5 (5 wt.% Fe) catalysts are compared in the wet oxidative degradation of methomyl. Fe-ZSM-5 exhibits outstanding whereas Fe-AlPILC shows only mediocre activity. Positions of iron are analysed in the two catalysts by Mössbauer spectroscopy. Iron is in highly dispersed state in Fe-AlPILC whereas in the other case a hematite/ZSM-5 composite is formed. The catalytic activity is attributed to iron located and stabilized in ionic dispersion. 相似文献
77.
Fanni Laura Bazsó Oliver Ozohanics Gitta Schlosser Krisztina Ludányi Károly Vékey László Drahos 《Journal of the American Society for Mass Spectrometry》2016,27(8):1357-1365
The similarity between two tandem mass spectra, which were measured on different instruments, was compared quantitatively using the similarity index (SI), defined as the dot product of the square root of peak intensities in the respective spectra. This function was found to be useful for comparing energy-dependent tandem mass spectra obtained on various instruments. Spectral comparisons show the similarity index in a 2D “heat map”, indicating which collision energy combinations result in similar spectra, and how good this agreement is. The results and methodology can be used in the pharma industry to design experiments and equipment well suited for good reproducibility. We suggest that to get good long-term reproducibility, it is best to adjust the collision energy to yield a spectrum very similar to a reference spectrum. It is likely to yield better results than using the same tuning file, which, for example, does not take into account that contamination of the ion source due to extended use may influence instrument tuning. The methodology may be used to characterize energy dependence on various instrument types, to optimize instrumentation, and to study the influence or correlation between various experimental parameters. 相似文献
78.
Fractal percolation or Mandelbrot percolation is one of the most well studied families of random fractals. In this paper we study some of the geometric measure theoretical properties (dimension of projections and structure of slices) of these random sets. Although random, the geometry of those sets is quite regular. Our results imply that, denoting by $E\subset\mathbb{R}^{2}$ a typical realization of the fractal percolation on the plane,
- If $\dim_{\rm H}E<1$ then for all lines ? the orthogonal projection E ? of E to ? has the same Hausdorff dimension as E,
- If $\dim_{\rm H}E>1$ then for any smooth real valued function f which is strictly increasing in both coordinates, the image f(E) contains an interval.
79.
Károly Bezdek 《Discrete and Computational Geometry》2012,48(2):298-309
The contact graph of an arbitrary finite packing of unit balls in Euclidean 3-space is the (simple) graph whose vertices correspond to the packing elements and whose two vertices are connected by an edge if the corresponding two packing elements touch each other. One of the most basic questions on contact graphs is to find the maximum number of edges that a contact graph of a packing of n unit balls can have. Our method for finding lower and upper estimates for the largest contact numbers is a combination of analytic and combinatorial ideas and it is also based on some recent results on sphere packings. In particular, we prove that if C(n) denotes the largest number of touching pairs in a packing of n>1 congruent balls in Euclidean 3-space, then $0.695<\frac{6n-C(n)}{n^{\frac{2}{3}}}< \sqrt[3]{486}=7.862\dots$ for all $n=\frac{k(2k^{2}+1)}{3}$ with k??2. 相似文献
80.
We give the general and the so-called density function solutions of equation
lllfU(x)fV(y)=fX(\frac1-y1-xy ) fY (1-xy) \fracy1-xy ( (x, y) ? (0,1)2 )\begin{array}{lll}f_{U}(x)f_{V}(y)=f_{X}\left(\frac{1-y}{1-xy} \right) f_{Y} (1-xy) \frac{y}{1-xy} \qquad \left( (x, y) \in (0,1)^2 \right)\end{array} 相似文献 |