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221.
Summary Pressure broadening and shift parameters are measured for theJ=1−0 line of CH3C14N at 18.4 GHz, both for the three hyperfine components and for the single line which envelopes the hyperfine components, observed
at higher pressures (p≥40 mTorr). In agreement with theoretical predictions, these parameters are the same for all the observed lines: Γ
p
= (50 ± 5) MHz/Torr,s=(7±2) MHz/Torr. These values are compared with previous measurements, showing a large variance expecially for the shift parameter.
The measured broadening parameter is 40% lower than prediction of the Anderson theory.
Riassunto Sono stati misurati i parametri di allargamento e spostamento per pressione della rigaJ=1−0 del CH3C14N a 18.4 GHz. Tali misure sono state eseguite, sulle tre componenti iperfini e sul loro inviluppo osservato a pressionip≥40 mTorr. In accordo con le previsioni teoriche, questi parametri risultano gli stessi per tutte le righe osservate: Γ p = (50 ± 5) MHz/Torr,s=(7±2) MHz/Torr. Questi valori sono confrontati con quelli delle precedenti misure che mostrano una considerevole dispersione, specialmente per quanto riguarda il parametro di spostamento. L'allargamento per pressione è risultato piú basso di quello previsto dalla teoria di Anderson di circa il 40%.相似文献
222.
Background
High-frequency Doppler imaging is highly potential for detection of blood flow in microcirculation. In a swept-scan system, however, the spectral broadening of tissue clutter limits the detectability of low-velocity flow signal. Conventionally, the scanning speed of transducer has to be reduced to alleviate the clutter interference but at the cost of imaging frame rate. For example, the blood velocity of 0.5 mm/s becomes detectable only with a scanning speed lower than 1 mm/s. In this study, an alternative method is examined by suppressing the clutter magnitude to reduce the interference to flow signal without sacrificing scanning speed.Methods
The method of third harmonic (3f0) transmit phasing can suppress the tissue harmonic clutter by transmitting at the fundamental and the additional 3f0 frequencies to achieve mutual cancellation between the frequency-sum and the frequency-difference components of the second harmonic signal. With 3f0 transmit phasing, the cut-off frequency of wall filtering can be reduced to preserve low-velocity flow without compromising the frame rate.Results
Our results indicate that the 3f0 transmit phasing effectively reduces the harmonic clutter magnitude and thus improves the flow signal-to-clutter ratio. Compared to the conventional counterpart, the clutter-suppressed color flow and power Doppler images show fewer clutter artifacts and is capable of detecting more low-velocity flow of microbubbles. The resultant color-pixel-density also improves with clutter suppression.Conclusion
For the swept-scan high-frequency (>20 MHz) system, 3f0 transmit phasing is capable of providing effective clutter suppression. With the same achievable scanning speed, the resultant Doppler image has higher sensitivity for low-velocity flow and is less susceptible to clutter artifacts. 相似文献223.
Kawashima K 《Ultrasonics》2012,52(2):287-293
An inverse spectral procedure was applied to reconstruct the acoustic impedance profile along the thickness direction of a plate using its thickness resonance frequencies, density and thickness. For a successful reconstruction, the material-property profile must be symmetric about the mid-plane of the plate. Several cases of numerical simulations, including plates with a few layers and with a high number of layers are described. The calculated resonance frequencies were used to reconstruct the acoustic impedance profile, a process that was successful for all cases. We assume that a plate with a high number of layers, each with a different but constant acoustic impedance, simulates a plate with a smoothly varying acoustic impedance profile. It can be concluded that such a plate, which generates small, virtually undetectable, internally reflected waves, can also be reconstructed. In the special case of a plate of unknown thickness and unknown but constant density, the method is still useful, because a relative variation of the material property can be reconstructed using only the resonance frequencies. An experiment using a resonance-mode electromagnetic acoustic transducer (resonance-mode EMAT) is also described. EMAT is a non-contact ultrasonic method that can measure thickness resonance frequencies, making it appropriate for this method. Some examples of applications are measurement of the temperature profile inside a rolled metal sheet, measurement of a clad metal plate, and monitoring of a metal casting. 相似文献
224.
数字全息成像由CCD记录数字全息图后经过计算机数值重建物光波场,这个过程从傅里叶变换角度看等同于数字全息图的频谱分析。讨论了数字成像系统的脉冲响应函数,并分别推导了其实像、虚像、零级像在平面波和球面波照射下的波前复振幅分布。结果表明,实像和虚像是移位的夫琅和费衍射分布,而零级像是CCD光瞳的菲涅耳衍射分布,且与参考光波前分布无关。 相似文献
225.
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227.
利用发光二极管(LED)光色电综合测试系统测量不同颜色不同功率的LED在多个电流下的光谱,提出并构建了由多个高斯函数组成的LED光谱模型,并根据各颜色LED在额定电流下的光谱计算模型中的系数,最后将该模型与已报道的模型进行了对比。研究表明:对于光谱有n(n≥1)个波峰的LED,可用3n个高斯函数形式的模型来表示,大功率红、黄、蓝、绿、白色LED模型与实测光谱之间平均误差分别为3.45%、1.01%、2.33%、4.65%、2.49%,小功率LED的平均误差分别为2.61%、2.65%、3.77%、2.87%、2.48%。与已报道的模型相比,该模型精度高,普适性好。本研究对LED光度色度测量仪器的研制及智能化LED产品的设计具有重要意义。 相似文献
228.
超高分辨率光谱定标技术发展概况 总被引:1,自引:0,他引:1
介绍了高光谱分辨率光谱定标经常采用的几种技术手段,包括谱线灯法、单色准直光法、利用可调谐激光器和气体吸收池的方法等。通过对比几种国外高光谱分辨率大气痕量气体探测仪的光谱定标技术,阐述了不同光谱定标技术的原理、实施方法以及技术特点。针对大气痕量气体探测遥感器超高分辨率光谱定标的特点,指出定标设备的带宽应能达到0.001nm的水平,同时还应考虑采取优化定标算法、结合多种光谱定标方法等措施来满足高光谱分辨率大气痕量气体探测仪光谱定标的要求。 相似文献
229.
230.
We report simulations concerning optical amplification in Er:Ti:LiNbO3 curved waveguides. The derivation and the evaluation of the spectral optical gain, the spectral noise figure, the amplified spontaneous emission photon number, and the signal to noise ratio are performed under the small gain approximation. The simulations show the evolution of these parameters under various pump regimes, Er concentration profiles and waveguide lengths. The results obtained are of significant interest for the design of complex, rare earth-doped integrated optics structures involving bent waveguides. 相似文献