Radiation Spectrum(辐射光谱)研究综述
Radiation Spectrum 辐射光谱 - The radiation spectrum of the BMCA is close to the blackbody radiation spectrum, which covers both the mid-wave infrared (MWIR) of 3 ~ 5 μm and the longwave infrared (LWIR) of 8 ~ 12 μm. [1] For a laser pulse whose length is comparable to its wavelength, the carrier envelope phase changes the behavior of the motion of the electron and therefore the radiation spectrum. [2] Enabled by the synergetic of surface plasmon resonances and Fabry–Pérot resonances, the TCCM simultaneously achieves high absorptivity (exceed 90%), and absorption broadband covers almost the entire solar irradiation spectrum. [3] The radiation spectrum from the MU shows soft X-ray radiation can be produced with 250 MeV electron bunches. [4] The grown structures show intense luminescence, the radiation spectrum of which shifts to the short-wave side with the increase of the pump level. [5] The negative behavior observed with the borosilicate lenses is attributed to the fact that the radiation spectrum of a xenon arc lamp contains certain wavelengths, in the near ultraviolet (UV) region, that are not present in the natural solar radiation spectrum at sea level. [6] Hawking’s groundbreaking intuition that black holes are not black but have a radiation spectrum that is very similar to that of a black body makes black holes an ideal laboratory to investigate the interplay between quantum mechanics, gravity and thermodynamics. [7] The signal of an integral terahertz oscillator was detected, its power was estimated, and the radiation spectrum was measured with a resolution of about 1 Hz. [8] The propeller contribution is observed in the second and fourth tones in the radiation spectrum. [9] In the plume spectrum of hydrogen-oxygen fuel, the radiation spectrum of hydroxide radical (OH) is an obvious feature in the ultraviolet (UV) band. [10] The SPG sub-THz emitter is experimentally demonstrated to emit sub-THz waves with a radiation spectrum from 50 to 300 GHz. [11] In this method, the direction information of rays is substituted by radiation spectrums via placing an array of filters in front of camera main lens, such that the image sensor can simultaneously acquire spectrums and intensities of rays. [12] The task of determining the radiation situation, including neutron and gamma-quantum flux density, radiation spectrum, specific volumetric activity of radioactive gases in the air, etc. [13] 011 cm−1 when the radiation intensity and the width of the radiation spectrum of pump diodes are 5 kW cm−2 and 4 cm−1, respectively. [14] The order of fractional integro-differentiation in the model sets the magnitude of the broadening of the radiation spectrum. [15] This paper shows that, whilst the actual pressure jump across a flat plate tends to infinity at the leading edge while dropping to zero at the trailing edge (due to the Kutta condition), the equivalent source distribution is more uniform across the aerofoil chord, which explains why the radiation spectrum and single-frequency directivity both exhibit strong oscillations due to interference from coherent sources across the chord. [16] A Monte Carlo simulation code based on Geant4 has been developed and used to compare circular and rectangular collimators for shaping the radiation spectrum of Compton sources. [17] Then according to the characteristics of the radiation spectrum of stars and the radiation spectrum of sky background light, we analyzed and selected the observation spectrum of the image-forming system. [18] The radiation spectrums of burning coal particles at different coflow temperatures and oxygen concentrations were measured by a fiber optic spectrometer and the temperatures of burning coal particles were deduced with the two-color method. [19] Key to our approach is that it offers a setting to achieve an effective description of the system's geometry {\it together} with the radiation spectrum. [20] We develop the simplest possible quantitative model of the formation of radiation spectrum in this range due to synchrotron emission and show that it fully agrees with the more complicated model of Ipser and Price 1982 for expected values of accretion rate. [21] We present the crystalrad simulation code, combining all the features of the crystal simulation code for simulations of charged particles trajectories in a bent crystal and the radcharm++ code for calculation of the radiation spectrum. [22] In this paper, we study the spectral lag for a radiating jet shell with a high-energy cut-off radiation spectrum. [23] In order to determine the capacitance required for the coupling capacitor, radiation spectrum is measured by using some coupling capacitor have different capacitance. [24] Dose rate estimation in handheld devices is usually done by summing up the channel data of the radiation spectrum. [25] The authors emphasize the necessity of analyzing the influence of the initial spent fuel parameters on the formation of the radiation spectrum and, therefore, on the radiation situation around the transport casks. [26] Owing to the absorption of two-photon pair production ($\gamma\gamma{\leftrightarrow}e^+e^-$), a high-energy spectral cutoff may appear in the radiation spectrum of GRBs. [27] The radiation spectrum of the disk and the shock are obtained for the $10\,\, M_\odot$ BH. [28] In this study, we successfully designed simulated and manufactured three kinds of periodic micro-patterns on the nickel surface and realized the manipulation of the radiation spectrum and the polarization of nickel. [29] 078, which shows a distinctly high reflectance in the whole solar-radiation spectrum, especially in the high energy UV wavebands. [30] The influence of temperature on the characteristics of the radiation spectrum was studied. [31] A full-custom Multi-Channel-Analyzer reconstructs the radiation spectrum, which is then processed by advanced Neural Network algorithms performing both image reconstruction and foreign bodies detection. [32] These mechanisms involve dependencies on the radiation spectrum due to the ash chemical composition and ash-sintering effects that enhance or hinder the overall heat transfer. [33] Seasonal variety would be enhanced for sulfa-group kind antibiotics, which having only tail overlapped with irradiation spectrum. [34] Moreover, the coupling of CN with ZnO facilitates the photodegradation phenomena by providing active sites, producing rich oxygen species and limiting the electrons and hole recombination, which lead to better degradation of TC under the solar irradiation spectrum. [35] The radiation spectrum of the thin film conforms to the characteristics of blackbody spectrum, and the average emissivity in infrared band is 0. [36] As a result, the radiation spectrum can be largely extended, for example to strong gamma-ray regime. [37] Solar irradiation spectrum on the earth consists of about 50% infrared energy, which has not used effectively in chemical storage and conversion into hydrogen via photocatalytic route. [38] In section two we have discussed the theory to derive an analytical expression for the electron beam trajectory that leads to an analytical expression for the radiation spectrum. [39]BMCA的辐射光谱接近黑体辐射光谱，既涵盖了3~5μm的中波红外（MWIR），也包括了8~12μm的长波红外（LWIR）。 [1] 对于长度与其波长相当的激光脉冲，载流子包络相位会改变电子运动的行为，从而改变辐射光谱。 [2] 通过表面等离子共振和法布里-珀罗共振的协同作用，TCCM同时实现了高吸收率（超过90%），吸收宽带几乎覆盖了整个太阳辐射光谱。 [3] 来自 MU 的辐射光谱显示软 X 射线辐射可以产生 250 MeV 电子束。 [4] 生长的结构显示出强烈的发光，其辐射光谱随着泵浦能级的增加向短波侧移动。 [5] 用硼硅酸盐透镜观察到的负面行为归因于这样一个事实，即氙弧灯的辐射光谱在近紫外 (UV) 区域中包含某些波长，而这些波长在海平面的自然太阳辐射光谱中不存在。 [6] 霍金突破性的直觉认为黑洞不是黑色，但其辐射光谱与黑体的辐射光谱非常相似，这使得黑洞成为研究量子力学、引力和热力学之间相互作用的理想实验室。 [7] 检测积分太赫兹振荡器的信号，估计其功率，并以约 1 Hz 的分辨率测量辐射光谱。 [8] 在辐射光谱的第二个和第四个音调中观察到螺旋桨的贡献。 [9] 在氢氧燃料的羽流光谱中，氢氧根（OH）的辐射光谱在紫外（UV）波段是一个明显的特征。 [10] 经实验证明，SPG 亚太赫兹发射器可发射辐射频谱为 50 至 300 GHz 的亚太赫兹波。 [11] 在该方法中，通过在相机主镜头前放置一排滤光片，将射线的方向信息替换为辐射光谱，使得图像传感器可以同时获取射线的光谱和强度。 [12] 确定辐射情况的任务，包括中子和伽马量子通量密度、辐射谱、空气中放射性气体的比体积活度等。 [13] 当泵浦二极管的辐射强度和辐射光谱宽度分别为 5 kW cm-2 和 4 cm-1 时，为 011 cm-1。 [14] 模型中分数积分微分的阶数决定了辐射光谱展宽的幅度。 [15] 本文表明，虽然平板上的实际压力跳跃在前缘趋于无穷大，而在后缘下降到零（由于库塔条件），但等效源分布在翼型弦上更加均匀，这解释了为什么辐射光谱和单频方向性都表现出强烈的振荡，这是由于来自弦上的相干源的干扰。 [16] 基于 Geant4 的 Monte Carlo 模拟代码已经开发出来，用于比较圆形和矩形准直器，以塑造康普顿源的辐射光谱。 [17] 然后根据恒星辐射光谱和天空背景光辐射光谱的特点，分析并选择了成像系统的观测光谱。 [18] 采用光纤光谱仪测量了不同顺流温度和氧浓度下燃烧煤颗粒的辐射光谱，并采用双色法推导了燃烧煤颗粒的温度。 [19] 我们方法的关键是它提供了一个设置来实现对系统几何 {\it together} 和辐射光谱的有效描述。 [20] 我们开发了由于同步加速器发射在该范围内形成辐射光谱的最简单的可能定量模型，并表明它与 Ipser 和 Price 1982 的更复杂的吸积率预期值模型完全一致。 [21] 我们提出了 crystalrad 模拟代码，结合了用于模拟弯曲晶体中带电粒子轨迹的晶体模拟代码和用于计算辐射光谱的 radcharm++ 代码的所有特征。 [22] 在本文中，我们研究了具有高能截止辐射光谱的辐射射流壳的光谱滞后。 [23] 为了确定耦合电容器所需的电容，通过使用一些具有不同电容的耦合电容器来测量辐射光谱。 [24] 手持设备中的剂量率估计通常是通过对辐射谱的通道数据求和来完成的。 [25] 作者强调有必要分析初始乏燃料参数对辐射谱形成的影响，从而对运输桶周围的辐射情况产生影响。 [26] 由于吸收了双光子对产生（$\gamma\gamma{\leftrightarrow}e^+e^-$），伽马暴的辐射光谱中可能出现高能光谱截止。 [27] 得到$10\,\, M_\odot$ BH的圆盘辐射谱和激波。 [28] 在本研究中，我们成功地在镍表面设计模拟制造了三种周期性微图案，实现了辐射光谱的操控和镍的极化。 [29] 078，它在整个太阳辐射光谱中显示出明显的高反射率，尤其是在高能紫外波段。 [30] 研究了温度对辐射光谱特性的影响。 [31] 一个完全定制的多通道分析仪重建辐射光谱，然后由先进的神经网络算法处理，执行图像重建和异物检测。 [32] 由于灰分化学成分和灰分烧结效应会增强或阻碍整体传热，这些机制涉及对辐射光谱的依赖性。 [33] 仅尾部与辐照光谱重叠的磺胺类抗生素增加了季节性品种。 [34] 此外，CN 与 ZnO 的耦合通过提供活性位点、产生丰富的氧物质和限制电子和空穴的复合来促进光降解现象，从而在太阳辐照光谱下更好地降解 TC。 [35] 薄膜的辐射光谱符合黑体光谱的特性，红外波段的平均发射率为0。 [36] 结果，辐射光谱可以大大扩展，例如到强伽马射线范围。 [37] 地球上的太阳辐射光谱包含约 50% 的红外能量，尚未有效地用于化学储存和通过光催化途径转化为氢气。 [38] 在第二节中，我们讨论了推导电子束轨迹解析表达式的理论，该解析表达式导致辐射光谱的解析表达式。 [39]
Solar Radiation Spectrum 太阳辐射光谱
Such SCs convert efficiently the solar radiation spectrum into electrical energy due to photon absorption in semiconductor layers with different widths of the bandgaps. [1] This phenomenon might be linked to the spectral response of the polycrystalline silicon cells and different incident solar radiation spectrum on the panels. [2] The absorption coefficients of the doped samples are greatly enhanced in visible light region and can cover the solar radiation spectrum effectively owing to the three-photon absorption with the help of intermediate band. [3] Results revealed the transition metal nitrides nanoparticles have small scattering cross-sections and broad absorption peaks, matching well the solar radiation spectrum. [4] The article presents the influence of changes in the solar radiation spectrum distribution on the properties of various photovoltaic modules, with particular emphasis on the scattered component. [5] It is indeed found out that staggered and randomly distributed nanoparticle reflects efficiently in the solar radiation spectrum, become highly reflective for thin slab and emits efficiently in the atmospheric window (8–13 µm) over the parallel arrangement with slight variation. [6] Inspired by tree branches, we designed and chemically synthesized silver fractals, which enable self-constructed hotspots and multiple plasmonic resonances, extending the broadband generation of hot electrons for better matching with the solar radiation spectrum. [7] It is a continuation of the article: Analysis of solar energy resources in southern Poland for photovoltaic applications [ 1 ], describing the method to determine spectral parameters of average photon energy ( APE ) and useful fraction ( UF ) with the use of a solar radiation spectrum simulator. [8] Maximizing the utilization of the ultraviolet portion in the solar radiation spectrum has always been a goal for plant growth in order to minimize the harm and harvest the benefits. [9] The polymer nanocomposite LSCs have broad absorption band covering a significant portion of the solar radiation spectrum, high spectral conversion efficiency, and low reabsorption due to minimal overlap between the absorption and emission spectra (large Stokes shift). [10] Micrometeorological data of global and photosynthetically active solar radiation, air temperature, substrate temperature, relative humidity and the solar radiation spectrum were recorded in each module. [11] 1 eV with absorption peaks at 515 and 554 nm, matching well with the strongest region of the solar radiation spectrum. [12] After optimizing the metamaterials-based absorber, a unity absorptance value at 540THz was achieved, while at the same time achieved absorptance rates over 80% for other sub-frequency bands within the solar radiation spectrum. [13] The possibilities of absorption (processing) by such structures of both short-wave radiation and long-wave part of the solar radiation spectrum for the purpose of generation of electric energy by increasing the efficiency of solar cells on their basis have been demonstrated. [14] We report over 99% absorption using molybdenum (metal) - germanium (dielectric) layers at normal incidence in the visible and nearinfrared regime of the solar radiation spectrum. [15] Computer processing of the series of multispectral satellite images (MSI) using the method of synthesizing (superposition of the long and short wavelengths of solar radiation spectrum) was carried out using the licensed software package ENVI 5. [16] The model was used to simulate actual PV performance and energy yield based on measured outdoor environmental parameters including solar radiation spectrum and temperature. [17] The matching of extinction spectrum and solar radiation spectrum is tuned by adjusting the proportion of components in blended nanofluid. [18] Interaction of the adjacent higher-order HE modes results in broadband light absorption enhancement in the solar radiation spectrum. [19]由于具有不同带隙宽度的半导体层中的光子吸收，此类 SC 有效地将太阳辐射光谱转换为电能。 [1] 这种现象可能与多晶硅电池的光谱响应和面板上不同的入射太阳辐射光谱有关。 [2] 掺杂样品在可见光区的吸收系数大大提高，由于借助中带的三光子吸收，可以有效地覆盖太阳辐射光谱。 [3] 结果表明，过渡金属氮化物纳米粒子散射截面小，吸收峰宽，与太阳辐射光谱匹配良好。 [4] 文章介绍了太阳辐射光谱分布的变化对各种光伏组件性能的影响，特别强调了散射分量。 [5] 确实发现交错和随机分布的纳米粒子在太阳辐射光谱中有效反射，对薄板具有高反射性，并在平行排列的大气窗口（8-13 µm）中有效发射，但变化很小。 [6] nan [7] 它是文章的延续：波兰南部太阳能资源的光伏应用分析 [1]，描述了使用太阳辐射确定平均光子能量 (APE) 和有用分数 (UF) 光谱参数的方法频谱模拟器。 [8] 最大限度地利用太阳辐射光谱中的紫外线部分一直是植物生长的目标，以最大限度地减少危害并收获益处。 [9] 由于吸收光谱和发射光谱之间的重叠最小（大斯托克斯位移），聚合物纳米复合材料 LSC 具有覆盖大部分太阳辐射光谱的宽吸收带、高光谱转换效率和低再吸收。 [10] 在每个模块中记录了全球和光合有效太阳辐射、气温、基质温度、相对湿度和太阳辐射光谱的微气象数据。 [11] 1 eV，在 515 和 554 nm 处有吸收峰，与太阳辐射光谱的最强区域非常匹配。 [12] 对超材料基吸收体进行优化后，在540THz处实现了统一的吸收值，同时在太阳辐射光谱内的其他子频段实现了80%以上的吸收率。 [13] 已经证明了通过这种结构吸收（处理）太阳辐射光谱的短波辐射和长波部分的可能性，以通过在其基础上提高太阳能电池的效率来产生电能。 [14] nan [15] nan [16] nan [17] nan [18] nan [19]
Thermal Radiation Spectrum 热辐射光谱
The instrumental accuracy of determining the desired temperature is estimated depending on the choice of a spectral window in the thermal radiation spectrum. [1] The block diagram of the test stand for spectrometer calibration is presented and relations for the correction of the recorded signals of the thermal radiation spectrum of the objects under study are derived. [2] One of these methods is spectral pyrometry, which is based on temperature measurement from the energy distribution in thermal radiation spectrum of investigated object. [3] We derive a simple and useful formula for the emissivity, which is then used to calculate the thermal radiation spectrum of semiconducting single-walled carbon nanotubes as a representative of 1D semiconductors. [4] This method is based on the measurement of thermal radiation spectrum in each pixel and its approximation of Planck's law by selecting proper values of temperature and emissivity. [5] We report highly emissive and radiatively cooled metallic surfaces that sustain multiple and high-amplitude gap plasmon cavity modes within the principal thermal radiation spectrum at room temperature (i. [6] This causes multiple resonances in the thermal radiation spectrum to which correspond the same spatial distribution of near-field thermal radiation [1]. [7] When determining the thermodynamic (true) temperature of an opaque material by the thermal radiation spectrum, the parametric model of spectral emissivity is chosen so that this model and sought material temperature can be considered adequate to the initial experimental data. [8] During the operation of the LHDAC system, temperature of the sample is determined from the thermal radiation spectrum between 640 and 740 nm to fit Planck's law. [9]确定所需温度的仪器精度取决于热辐射光谱中光谱窗口的选择。 [1] 给出了光谱仪校准试验台的框图，并推导了研究对象热辐射光谱记录信号的校正关系。 [2] 其中一种方法是光谱测温法，它基于从被调查对象的热辐射光谱中的能量分布进行温度测量。 [3] nan [4] nan [5] nan [6] nan [7] 当通过热辐射光谱确定不透明材料的热力学（真实）温度时，选择光谱发射率的参数模型，以便可以认为该模型和寻找的材料温度足以满足初始实验数据。 [8] 在 LHDAC 系统运行期间，样品的温度由 640 和 740 nm 之间的热辐射光谱确定，以符合普朗克定律。 [9]
Electromagnetic Radiation Spectrum 电磁辐射谱
In this method, the electromagnetic radiation spectrum of typical image transmitted by HDMI cable is simulated. [1] This technology is easily adaptable to the tasks of integrating images of different parts of the electromagnetic radiation spectrum. [2] It is shown that the doping of titanium dioxide by bismuth ions results in a shift of light absorption to the visible region of electromagnetic radiation spectrum. [3] Forming of controlled states and error signals is carried out by means of the multichannel optical spectrometer where the spectral decomposition is based on a resonance phenomenon in the narrow-band optical interference filters on the measurement data of the electromagnetic radiation spectrum as one of the results of the combustion process. [4] The concentration of the cChD additive is calculated, so that the peak of selective reflection and its rearrangement occurs in the visible range of the electromagnetic radiation spectrum (380-780 nm). [5]在该方法中，模拟了HDMI电缆传输的典型图像的电磁辐射谱。 [1] 这项技术很容易适应整合电磁辐射光谱不同部分的图像的任务。 [2] 结果表明，铋离子掺杂二氧化钛导致光吸收向电磁辐射光谱的可见区域移动。 [3] 受控状态和误差信号的形成是通过多通道光谱仪进行的，其中光谱分解是基于窄带光学干涉滤波器中的共振现象，对电磁辐射光谱的测量数据作为结果之一燃烧过程。 [4] nan [5]
Infrared Radiation Spectrum
The object of research is the interaction of the infrared radiation spectrum with ice. [1] According to the characteristics of target infrared radiation spectrum, assuming that the target is grey body, this paper uses infrared dual-band temperature measurement algorithm and Monte Carlo method to extract the temperature feature of the object under test. [2] The combustion of moxa floss was investigated by thermogravimetric/differential scanning calorimeter (TG/DSC), thermogravimetric/Fourier transform infrared spectroscopy (TG-FTIR) and an infrared radiation spectrum-detecting system. [3] The purpose of this study was to observe the characteristics of infrared radiation spectrum of Zigong acupoint (EX-CA1) within the menstrual cycle of healthy female. [4]研究对象是红外辐射光谱与冰的相互作用。 [1] 根据目标红外辐射光谱的特点，假设目标为灰体，本文采用红外双波段测温算法和蒙特卡罗方法提取被测物体的温度特征。 [2] nan [3] nan [4]
Different Radiation Spectrum
In conclusion, the need to maintain the greenhouse microclimate and supplementary lighting with the different radiation spectrum for the efficient cultivation of greenhouse plants is shown. [1] It is worth noting that the spacewalks not only confer a higher dose activity but are also characterized by a different radiation spectrum than inside the space craft since the primary particles would not interact with the vehicle shell to generate secondary radiation. [2] It is worth noting that the spacewalks not only confer a higher dose activity but are also characterized by a different radiation spectrum than inside the space craft since the primary particles would not interact with the vehicle shell to generate secondary radiation. [3]总之，需要保持温室小气候和具有不同辐射光谱的补充照明，以有效种植温室植物。 [1] 值得注意的是，太空行走不仅具有更高的剂量活动，而且还具有与航天器内部不同的辐射光谱，因为初级粒子不会与飞行器外壳相互作用产生次级辐射。 [2] 值得注意的是，太空行走不仅具有更高的剂量活动，而且还具有与航天器内部不同的辐射光谱，因为初级粒子不会与飞行器外壳相互作用产生次级辐射。 [3]
Hawking Radiation Spectrum 霍金辐射光谱
This study explores the emission of massive charged spin-1 particles from the background of Bardeen regular spacetime by the semi-classical method used to study the Hawking radiation spectrum. [1] Based on the semiclassical Hawking radiation spectrum, a finite nonvanishing value for quantum corrections to the Love number of Schwarzschild black holes in general relativity is computed using the sum rule, which is known to classically vanish. [2] We consider the back reaction of emitted particles to the space-time, and get the corrected Hawking radiation spectrum. [3]本研究通过用于研究霍金辐射光谱的半经典方法，探索了巴丁规则时空背景中大量带电自旋 1 粒子的发射。 [1] 基于半经典霍金辐射光谱，使用和规则计算广义相对论中史瓦西黑洞 Love 数的量子校正的有限非消失值，已知该求和规则在经典上消失。 [2] nan [3]
Body Radiation Spectrum
We derive a discrete black-body radiation spectrum, deriving a different formulation for $F(a)$ than the one presented in the original theory. [1] Thus, the gas temperature was evaluated by assuming that the continuous spectrum was a black-body radiation spectrum. [2]我们推导出了一个离散的黑体辐射光谱，为 $F(a)$ 推导出了与原始理论中提出的不同的公式。 [1] 因此，通过假设连续光谱是黑体辐射光谱来评估气体温度。 [2]
Light Radiation Spectrum
The light radiation spectrum of objects is around 1000, 1100, 1200, and 1300 $^{\circ}$C. [1] A non-contact system is designed for light radiation spectrum and image acquisition of furnace mouth. [2]物体的光辐射光谱在1000、1100、1200、1300$^{\circ}$C左右。 [1] 设计了一种非接触式的炉口光辐射光谱和图像采集系统。 [2]
Flat Radiation Spectrum
Another option of the fiber diameter profile provides flat radiation spectrum in the range 2–2. [1] Another option of the fiber diameter profile provides flat radiation spectrum in the range 2-2. [2]光纤直径分布的另一种选择提供了 2-2 范围内的平坦辐射光谱。 [1] 光纤直径分布的另一种选择提供了 2-2 范围内的平坦辐射光谱。 [2]
Continuou Radiation Spectrum
A Levenberg-Marquardt (LM) method, sensitive to the expected spectral function, is improved to reliably generate a continuous radiation spectrum, by utilizing spectral information from the least-squares (LS) method that reconstructs a discrete spectrum with low spectral resolution directly from the VCs. [1] The large width of the components is explained by the continuous radiation spectrum of returned positrons incident on the surface. [2]对预期光谱函数敏感的 Levenberg-Marquardt (LM) 方法通过利用最小二乘 (LS) 方法的光谱信息得到改进，以可靠地生成连续辐射光谱，该方法直接从低光谱分辨率重建离散光谱。风投。 [1] nan [2]