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高质量的CO_2反演结果有助于准确认知其源汇信息、预测未来气候变化趋势及提升全球碳循环的理解。基于非线性最小二乘光谱拟合技术,研究地基高分辨率傅里叶变换红外光谱反演环境大气中CO_2浓度的反演产品质量优化方法。借助O_2窗口的反演结果,将CO_2柱浓度转化为柱平均干空气摩尔分数(column-averaged dry air mole fraction,XCO_2),能有效修正系统共有误差;采用一种经验修正模型,能有效修正与大气质量因子相关的虚假日变化;通过建立一定的红外光谱筛选法则,能有效控制XCO_2反演产品质量。以一天的典型观测结果为例,对产品质量优化前后的反演结果进行了对比,优化后反演误差减小了60%,以正午为中心两边各取一小时计算了XCO_2的反演精度,为0.071%(相当于0.28ppm),符合TCCON(total carbon column observing network)规定的0.1%精度范围。 相似文献
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In holographic encryption, double random-phase encoding in the Fresnel domain (DRPEiFD) is a preva- lent encryption method because it is lensless and secure. However, noises bring adverse effects during decryption. In this letter, we introduce quick-response (QR) coding during encryption to resist noises. We transform the original information into a QR code and then enerypt the code as a hologram through DRPEiFD. To retrieve the input, we deerypt the hologram in the opposite manner to the encryption and subsequently obtain a QR code with noises. By scanning this code with proper applications in smart- phones, we can obtain a noise-free retrieval. Numerical experiments and images scanned by a smartphone are shown to validate our proposed method. 相似文献
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新型有机-无机纳米复合粒子的制备及其固定化漆酶研究 总被引:2,自引:0,他引:2
制备了四氨基酞菁钴(CoTAPc)-Fe3O4纳米复合粒子, 用红外光谱(IR)、X射线衍射(XRD)、X射线能谱(EDS)、场发射扫描电镜(FEG-SEM)及振动样品磁强计等对其进行了表征. 结果表明, 形成了CoTAPc包覆在Fe3O4纳米粒子表面的纳米复合粒子. 粒子呈现不规则球形, 平均粒径为70 nm, 矫顽力为316.4 A/m, 接近超顺磁性. 以此纳米复合粒子作为载体, 通过交联法固定漆酶, 固定化酶最适反应温度为45 ℃, 最适pH为3; 固定化酶比游离酶具有更好的热稳定性、贮存稳定性及操作稳定性, 且易于分离. 相似文献
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A new three-dimensional (3D) optical fluorescent tomographic imaging scheme is proposed with structured illumination and spatial Fourier-domain decomposition methods for the first time. In this spatial Fourierdecomposition optical fluorescence tomography (SF-OFT), the intensity of focused excitation light from an objective lens is modulated to be a cosine function along the optical axis of the system. For a given position in a two-dimensional (2D) raster scanning process, the spatial frequency of the cosine function along the optical axis sweeps in a proper range while a series of fluorescence intensity are detected accordingly. By making an inverse discrete cosine transformation of these recorded intensity profiles, the distribution of fluorescent markers along the optical axis of a focused laser beam is obtained. A 3D optical fluorescent tomography can be achieved with this proposed SF-OFT technique with a simple 2D raster scanning process. 相似文献
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