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991.
鲁圣洁 《纯粹数学与应用数学》2006,22(3):318-324,329
研究一类含有五个反馈权值二维细胞神经网络系统,以系统的输出反馈权值及阈值为参数构成参数空间,引入几何方法,将此空间分解分块成有限个区域,当输出反馈权值及阈值在某一区域上时,给出系统具有M osaic解所有可能的输出函数M osaic模式的充要条件. 相似文献
992.
利用最小二乘估计方法和权函数法给出了半参数模型Y=βX g(T) ε在某种污染方式下,,βg和污染系数的估计,并在适当条件下证明了它们具有相合性. 相似文献
993.
The asymptotic expressions of the covariance matrices for both the least square estimates
L
α
T
and Markov (best linear) estimates
are obtained, based on a sample in a finite interval (0, T) of the regression co-efficients α = (α
1, …, α
m
0)′ of a parameter-continuous process with a stationary residual. We assume that the regression variables φ
ν(t), t ⩾ 0, ν = 1, …, m
0, are continuous in t, and satisfy conditions (3.1)–(3.3). For the residual, we assume that it is a stationary process that possesses a bounded
continuous spectral density f(λ). Under these assumptions, it is proven that
where the matrices D
T
, B(0), α(λ) are defined in Section 3.
Under the assumptions mentioned above, if, furthermore, there exist some positive integer m and a constant C such that g(λ)(1 + λ
2)m ⩾ C > 0, where g(λ) is the spectral density of the residual, and for every N > 0,
converge uniformly in h, l ∈ (−N, N), then the following formula holds.
The asymptotic equivalence of the least square estimates and the Markov estimates is also discussed.
Translated by Wang Ting from the Chinese version of the paper published in Journal of Beijing Normal University (Natural Sciences), 1965, 1: 15–44 相似文献
994.
Choi JH Oh IG Ryoo KS Lim WT Park YC Habibi MH 《Spectrochimica acta. Part A, Molecular and biomolecular spectroscopy》2006,65(5):1138-1143
The structure of [CrF(2)([15]aneN(4))]ClO(4).H(2)O ([15]aneN(4)=1,4,8,12-tetraazacyclopentadecane) has been determined by a single-crystal X-ray diffraction study at 173 K. The complex crystallizes in the space group P1- of the triclinic system with two mononuclear formula units in a cell of dimensions a=9.6117(7) A, b=10.2882(7) A, c=11.0001(7) A and alpha=99.7570(10) degrees, beta=105.6080(10) degrees and gamma=113.7130(10) degrees. The complex cation unit has its central Cr atom in an octahedral coordination with four nitrogen atoms and two fluorine atoms in a trans position. Three six-membered and one five-membered chelate rings of the [15]aneN(4) ligand are in a chair-twist(skew)-chair-gauche conformation sequence. The gauche five-membered ring is disordered with the twist six-membered ring opposite. The four H atoms in the chiral N atoms have the trans-II (CTCg) type configuration. The mean Cr-N and Cr-F bonds are 2.095(2) and 1.8752(13) A, respectively. The IR and visible spectral properties are consistent with the result of X-ray crystallography. The resolved band maxima of the electronic d-d spectrum are fitted with secular determinant for quartet state energy of d(3) configuration in tetragonal field including configurational but neglecting spin-orbit coupling. It is confirmed that the fluoride has strong sigma- and pi-donor properties toward the chromium(III) ion and the nitrogen atoms of the [15]aneN(4) ligand also have a strong sigma-donor character. 相似文献
995.
Zhong De‐Gao Teng Bing Yu Zheng‐He Ge Xiao‐Hui You Fei Xu Hui Zhang Shi‐Ming Yu Yue‐Juan Ma Jiangtao 《Crystal Research and Technology》2010,45(11):1127-1131
Mixed crystals of K1‐x(NH4)xH2PO4(KADP) were grown from KDP (KH2PO4) dominated mixed solutions with varying molar proportion of ADP (NH4H2PO4) addition. It was found that, as the increase of ADP molar concentration, the growth rate along z‐axis of KADP crystal decreased rapidly. The structure of KADP crystals was investigated by powder XRD and the lattice parameter was calculated. The results showed that the lattice parameter c of KADP crystal increased with the molar concentration of ADP. The optical homogeneity of grown KADP crystals was determined with a differential phase‐shifting interferometry. Frequency dependences of the dielectric constant and dielectric loss of KADP crystals were measured at room temperature (290 K). The dielectric constants of KADP crystals were almost invariant with the increase of frequency. In the region of 102∼104Hz, the values of the dielectric loss reduced with the increase of frequency. The piezo‐resonance coupling effect still exists in KADP crystals at room temperature, but shifted to low frequency band. (© 2010 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
996.
997.
We use the Radial Baryon Acoustic Oscillation (RBAO) measurements, distant type Ia supernovae (SNe Ia), the observational H(z) data (OHD) and the Cosmic Microwave Background (CMB) shift parameter data to constrain cosmological parameters of ΛCDM and XCDM cosmologies and further examine the role of OHD and SNe Ia data in cosmological constraints. We marginalize the likelihood function over h by integrating the probability density P∝e−χ2/2 to obtain the best fitting results and the confidence regions in the Ωm–ΩΛ plane. With the combination analysis for both of the ΛCDM and XCDM models, we find that the confidence regions of 68.3%, 95.4% and 99.7% levels using OHD+RBAO+CMB data are in good agreement with that of SNe Ia+RBAO+CMB data which is consistent with the result of Lin et al.'s (2009) [24] work. With more data of OHD, we can probably constrain the cosmological parameters using OHD data instead of SNe Ia data in the future. 相似文献
998.
The structural and thermodynamic properties of a confined hard ellipse fluid are studied using Monte Carlo simulation. The angular, average number densities and order parameters of hard ellipses confined between hard parallel walls are obtained for various bulk densities, aspect ratios and wall separations. The results show that the effect of the existence of the wall on the molecular fluid structure, either on their directions or their locations, with respect to the bulk, especially close to the walls, is significant. For this system the pressure is also obtained and it is shown that the average density at the wall is proportional to the pressure, βP=〈ρw〉. Our simulation results show that the order parameters depend on the number of the particles in the box unless it exceeds thousand. 相似文献
999.
BeH~+(X~1∑~+)离子势能函数及其分子常数研究 总被引:1,自引:1,他引:0
本文利用CCSD(T)方法和系列相关一致基,对BeH~+(X~1∑~+)离子的几何结构进行了优化,结果发现在CCSD(T)/aug-cc-pV5Z理论水平下得到的光谱数据(R_e=0.13142 nm,ω_e=2212.7 cm~(-1),D_e=3.1750 eV)与实验值非常接近.在CCSD(T)/aug-cc-pV5Z理论水平下又对BeH~+(X~1∑~+)离子的势能曲线进行了计算,再用最小二乘法将计算结果拟合成了Murrell-Sorbie函数.利用拟合出的解析势能函数,进一步计算出了BeH~+离子X~1∑~+态的其它光谱常数(B_e,α_e,ω_e和ω_ex_e),且与实验及其它理论计算结果进行了比较.以得到的解析势能函数为基础,通过求解双原子分子核运动的径向Schr(o|¨)dinger方程,找到了J=0时基态的全部20个振动态,并求出了每一振动态的振动能级、转动惯量及离心畸变常数(D_v,H_v,L_v,M_v,N_v,O_v).计算结果与实验数据的比较表明,BeH~+(X~1∑~+)离子的势能函数可用Murrell-Sorbie函数来表达,而且由此计算出的光谱常数、振动能级和转动惯量等都达到了相当高的精度. 相似文献
1000.
采用内收缩多参考组态相互作用(MRCI)方法和系列相关一致基aug-cc-pVnZ对GaH (X1Σ+)自由基的光谱性质进行了研究. 通过与实验结果的比较, 发现在aug-cc-pV5Z基组、且考虑相对论修正时得到的De, Re和ωe与实验结果较为一致. 在这一基组下对GaH(X1Σ+)自由基的势能曲线进行了计算、并将计算结果拟合成了Murrell-Sorbie函数, 由此得到的光谱常数(ωeχe, αe和 Be)也与实验结果较为相符. 以得到的解析势能函数为基础, 通过求解双原子分子核运动的径向Schrödinger方程, 找到了J = 0时该自由基存在的全部27个振动态. 针对每一振动态, 还计算了它的振动能级、经典转折点、转动惯量和离心畸变常数, 文中的大部分分子常数均属首次报导. 相似文献