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1.
HJ-1B卫星IRS传感器热红外通道交叉定标   总被引:2,自引:1,他引:1  
以TERRA卫星中分辨率成像光谱仪(MODIS)传感器热红外通道的星上定标结果为标准,采用交叉定标方法获取HJ-lB卫星红外多光谱相机(IRS)传感器热红外通道定标系数.首先,获取两个传感器的对应通道,利用MODTRAN模拟光谱响应、观测角、大气条件和温度变化对匹配因子的影响.然后确定此研究只考虑对应通道的波谱响应和地表温度差异,并计算出不同地表温度下匹配因子的变化趋势.选择7次不同时间双星同步观测青海湖区域的图像作为交叉定标数据,根据MODIS的辐射亮度和匹配因子计算出IRS传感器热红外通道的辐射亮度,最后,将得到的辐射亮度和DN值进行线性回归,获得IRS热红外通道的定标系数.将此次定标结果与HJ-1B卫星IRS传感器热红外通道星上4次黑体定标结果进行比较,定标结果一致性较好.  相似文献   

2.
为获取2013年HJ-1B/IRS热红外通道(B08)绝对辐射定标系数,以TERRA/MODIS为参考传感器,以青海湖为研究区域,采用双通道差分模型进行交叉定标。对比分析不同观测角度、成像时差对定标精度的影响,结果表明,参考传感器观测角度30以内、成像时差1 h左右交叉定标条件最佳,且回归拟合的定标系数精度最高。通过采用2013年10月26日宁德附近海域星地同步实验数据进行精度验证,结果表明,此定标系数得到的表观辐亮度误差在0.02 Wm-2m-1sr-1以内,表观亮温误差在0.15℃以内。同时,通过与历年辐射定标系数(2008~2012年)进行对比,所得定标系数精度分别提高98.50%、98.24%、90.21%、20.87%和98.31%。总之,此文定标系数精度较高、结果可靠,可应用于IRS B08通道。  相似文献   

3.
马秀秀  王海燕  韩启金  张学文  赵航  徐兆鹏  曾健  马灵玲  王宁 《红外与激光工程》2023,52(4):20220644-1-20220644-11
以GF5B卫星发射前实验室定标为基础,采用星上0级黑体定标数据,建立了适用于GF5B热红外通道的星上绝对辐射定标模型。通过对2022年01月12日星上黑体定标数据进行处理,获得成像仪热红外通道的绝对辐射定标系数。对星上定标系统精度进行分析,并采用地面同步烟台浮标数据对定标结果进行精度验证,结果表明,在轨后星上定标系统的绝对定标精度为0.9 K;星地验证结果显示B11和B12通道亮温的偏差分别为0.33、0.77 K。说明基于星上黑体的定标方法具有较好的精度,定标结果可靠,可满足遥感数据定量化应用的需要,为实时准确获取热红外通道定标系数提供了方法借鉴。  相似文献   

4.
建立CBERS—1上搭载的红外多光谱扫描仪(IRMSS)与FY—1C通道4及Landsat-7上ETM 波段6多星星载热红外遥感仪器交叉定标的算法模型,利用美国Landsat-7上搭载的ETM 红外通道6和FY—1C通道4分别对IRMSS热红外通道进行交叉定标,得到二组定标结果.相同地标点对比分析结果表明,二个定标结果得到的目标点亮度温度相对偏差为1.2K;IRMSS交叉定标结果与Landsat-7ETM 热红外通道在轨定标结果独立样本对比分析结果,均方根偏差为1.6K.  相似文献   

5.
HJ-1B卫星热红外通道在轨场地定标与验证   总被引:1,自引:0,他引:1       下载免费PDF全文
在对热红外辐射计CE312定标的基础上,基于青海湖水面辐射校正场,采用CE312开展同步测量实验,对HJ-1B卫星热红外通道进行在轨绝对辐射定标。由于HJ-1B卫星在轨星上定标系统不稳定,高温点难以准确获取,因此分别使用单点法和两点法,对2010年8月1日和5日两组传感器入瞳等效辐亮度值和卫星通道计数值回归得到该卫星通道绝对定标系数,并使用内蒙达里湖水面辐射校正场2010年6月29日实测数据进行定标系数的验证工作。验证结果表明,青海湖场地两次定标系数有较好的一致性,定标结果稳定可信。两点法所得定标系数的精度高于单点法。  相似文献   

6.
针对FY-3A/VIRR传感器定标精度有限,且场地定标机会有限的问题,介绍了利用高精度的TERRA/MODIS 31通道对FY-3A/VIRR 红外4通道进行绝对交叉定标的方法。选用2013年1、3、和9三个月的卫星数据进行了交叉定标计算,并对交叉定标结果进行的验证。结果表明,VIRR利用交叉定标系数计算的通道亮温与MODIS匹配点处的实测结果具有很好的一致性,绝大多数的亮温偏差在1 K以内。对不同月份交叉定标结果进行的验证表明,交叉定标系数具有普遍适用性。  相似文献   

7.
HJ-1B热红外通道在轨星上定标精度直接影响着后续遥感数据的定量化应用。以往针对整个通道的星上辐射定标忽视了各个探元的响应差异问题。使用查找表法、半高宽法和矩方法,分别对2009年9月14日星上下传的黑体数据进行处理,得到HJ-1B热红外通道探元级辐射定标结果。分析结果,红外相机热红外通道各探元扫描校正黑体时存在2个DN左右的波动,引入误差约0.28%~0.45%。其中,探元9和10相对其他探元波动范围较大。  相似文献   

8.
HJ-1B卫星自发射以红外通道共进行了7次星上黑体定标,针对星上定标系数的验证工作开展较少,以MODIS第31、32通道为参考源,分别基于光谱响应差异和线性统计关系两种方法对HJ-1B红外通道星上定标系数进行验证.首先,计算两个传感器表观辐亮度的匹配关系,进而计算出HJ-1B红外通道的等效离表亮温,通过与HJ-1B红外通道基于星上定标系数反演得到的离表亮温进行比较,实现对星上定标系数的验证.通过半高宽法、矩方法和查找表法这三种不同的方法计算得到了2009年9月14日星上定标系数.结果表明:三种方法中,查找表法精度较高, 且HJ-1B查找表法星上定标系数反演亮温与基于光谱响应差异和线性统计关系计算的等效亮温偏差较小,分别为0.02 K和0.81 K.这两种交叉验证方法的精度均在1 K以内,证明了该方法的可行性,且基于光谱响应差异的验证方法精度更高.该研究为光学载荷在轨辐射定标的验证提供了理论基础.  相似文献   

9.
黑体辐射源作为初级标准,其辐射特性的测量精度决定了整个标准传递链路的不确定度。为了提高黑体的辐亮度测量精度,研制了一台可直接观测黑体辐亮度的双通道热红外标准辐亮度计。根据仪器的工作原理,采用自行研制的高精度水浴黑体获取标准辐亮度计的定标系数。实验结果表明,该辐亮度计的1 h信号非稳定性优于0.3%,定标系数拟合不确定度优于1.23%,5 m通道整体不确定度为0.39%,10 m通道整体不确定度为1.3%。可实现黑体辐亮度与实验室辐射标准之间的传递。  相似文献   

10.
高分一号卫星相机的辐射交叉定标研究   总被引:1,自引:0,他引:1       下载免费PDF全文
利用Landsat8-OLI时间序列图像数据对高分一号(GF-1)的16 m宽覆盖多光谱传感器进行交叉定标。试验首先通过安排GF-1夜间深海成像,确定GF-1传感器的定标公式的截距,再选取定标靶标场的双星同步观测数据,利用回归分析得到定标公式的增益。利用交叉定标系数结果计算的GF-1辐亮度值与同步观测的Landsat8的辐亮度值相关性在95%以上,4个波段定标精度相对误差分别是4.25%、6.21%、5.83%和5.66%。结果表明该方法获得的定标系数精度与Landsat8定标数据辐射定标精度相当,GF-1卫星可以满足定量化应用的要求。  相似文献   

11.
Waveguide multilayer optical card (WMOC) is a novel storage device of three-dimensional optical information. An advanced readout system fitting for the WMOC is introduced in this paper. The hardware mainly consists of the light source for reading, WMOC, motorized stages addressing unit, microscope imaging unit, CCD detecting unit and PC controlling & processing unit. The movement of the precision motorized stage is controlled by the computer through Visual Basic (VB) language in software. A control panel is also designed to get the layer address and the page address through which the position of the motorized stages can be changed. The WMOC readout system is easy to manage and the readout result is directly displayed on computer monitor.  相似文献   

12.
IntroductionNanoimprint Lithography is a well-acknowl-edged low cost, high resolution, large area pattern-ing process. It includes the most promising methods,high-pressure hot embossing lithography (HEL) [2],UV-cured imprinting (UV-NIL) [3] and micro contactprinting (m-CP, MCP) [4]. Curing of the imprintedstructures is either done by subsequent UV-lightexposure in the case of UV-NIL or by cooling downbelow the glass transition temperature of the ther-moplastic material in case of HEL…  相似文献   

13.
The collinearly phase-matching condition of terahertz-wave generation via difference frequency mixed in GaAs and InP is theoretically studied. In collinear phase-matching, the optimum phase-matching wave hands of these two crystals are calculated. The optimum phase-matching wave bands in GaAs and lnP are 0.95-1.38μm and 0.7-0.96μm respectively. The influence of the wavelength choice of the pump wave on the coherent length in THz-wave tuning is also discussed. The influence of the temperature alteration on the phase-matching and the temperature tuning properties in GaAs crystal are calculated and analyzed. It can serve for the following experiments as a theoretical evidence and a reference as well.  相似文献   

14.
Composition dependence of bulk and surface phonon-polaritons in ternary mixed crystals are studied in the framework of the modified random-element-isodisplacement model and the Bom-Huang approximation. The numerical results for Several Ⅱ - Ⅵ and Ⅲ- Ⅴ compound systems are performed, and the polariton frequencies as functions of the compositions for ternary mixed crystals AlxGa1-xAs, GaPxAS1-x, ZnSxSe1-x, GaAsxSb1-x, GaxIn1-xP, and ZnxCd1-xS as examples are given and discussed. The results show that the dependence of the energies of two branches of bulk phonon-polaritons which have phonon-like characteristics, and surface phonon-polaritons on the compositions of ternary mixed crystals are nonlinear and different from those of the corresponding binary systems.  相似文献   

15.
A doping system consisting of NPB and PVK is employed as a composite hole transporting layer (CHTL). By adjusting the component ratio of the doping system, a series of devices with different concentration proportion of PVK : NPB are constracted. The result shows that doping concentration of NPB enhances the competence of hole transporting ability, and modifies the recombination region of charge as well as affects the surface morphology of doped film. Optimum device with a maximum brightness of 7852 cd/m^2 and a power efficiency of 1.75 lm/W has been obtained by choosing a concentration proportion of PVK : NPB at 1:3.  相似文献   

16.
An insert layer structure organic electroluminescent device(OLED) based on a new luminescent material (Zn(salen)) is fabricated. The configuration of the device is ITO/CuPc/NPD/Zn(salen)/Liq/LiF/A1/CuPc/NPD/Zn(salen)/Liq/LiF/A1. Effective insert electrode layers comprising LiF(1nm)/Al(5 nm) are used as a single semitransparent mirror, and bilayer cathode LiF(1 nm)/A1(100 nm) is used as a reflecting mirror. The two mirrors form a Fabry-Perot microcavity and two emissive units. The maximum brightness and luminous efficiency reach 674 cd/m^2 and 2.652 cd/A, respectively, which are 2.1 and 3.7 times higher than the conventional device, respectively. The superior brightness and luminous efficiency over conventional single-unit devices are attributed to microcavity effect.  相似文献   

17.
Due to variable symbol length of digital pulse interval modulation(DPIM), it is difficult to analyze the error performances of Turbo coded DPIM. To solve this problem, a fixed-length digital pulse interval modulation(FDPIM) method is provided. The FDPIM modulation structure is introduced. The packet error rates of uncoded FDPIM are analyzed and compared with that of DPIM. Bit error rates of Turbo coded FDPIM are simulated based on three kinds of analytical models under weak turbulence channel. The results show that packet error rate of uncoded FDPIM is inferior to that of uncoded DPIM. However, FDPIM is easy to be implemented and easy to be combined, with Turbo code for soft-decision because of its fixed length. Besides, the introduction of Turbo code in this modulation can decrease the average power about 10 dBm, which means that it can improve the error performance of the system effectively.  相似文献   

18.
It is a key problem to accurately calculate beam spots' center of measuring the warp by using a collimated laser. A new method, named double geometrical center method (DGCM), is put forward for the first time. In this method, a plane wave perpendicularly irradiates an aperture stop, and a charge couple device (CCD) is employed to receive the diffraction-beam spots, then the geometrical centers of the fast and the second diffraction-beam spots are calculated respectively, and their mean value is regarded as the center of datum beam. In face of such adverse instances as laser intension distributing defectively, part of the image being saturated, this method can still work well. What's more, this method can detect whether an unacceptable error exits in the courses of image receiving, processing and calculating. The experimental results indicate the precision of this method is high.  相似文献   

19.
High purity organic-tantalum precursors for thin film ALD TaN were synthesized and characterized.Vapor pressure and thermal stability of these precursors were studied.From the vapor pressure analysis,it was found that TBTEMT has a higher vapor pressure than any other published liquid TaN precursor,including TBTDET,TAITMATA,and IPTDET.Thermal stability of the alkyl groups on the precursors was investigated using a 1H NMR technique.The results indicated that the tertbutylimino group is the most stable group on TBTDET and TBTEMT as compared to the dialkylamido groups.Thermal stability of TaN precursors decreased in the following order:TBTDET > PDMAT > TBTEMT.In conclusion,precursor vapor pressure and thermal stability were tuned by making slight variations in the ligand sphere around the metal center.  相似文献   

20.
In order to diagnose the laser-produced plasmas, a focusing curved crystal spectrometer has been developed for measuring the X-ray lines radiated from a laser-produced plasmas. The design is based on the fact that the ray emitted from a source located at one focus of an ellipse will converge on the other focus by the reflection of the elliptical surface. The focal length and the eccentricity of the ellipse are 1350 mm and 0.9586, respectively. The spectrometer can be used to measure the X- ray lines in the wavelength range of 0.2-0.37 nm, and a LiF crystal (200) (2d = 0.4027 nm) is used as dispersive element covering Bragg angle from 30° to 67.5°. The spectrometer was tested on Shengnang- Ⅱ which can deliver laser energy of 60-80 J/pulse and the laser wavelength is 0.35 μm. Photographs of spectra including the 1 s2p ^1P1-1s^2 ^1S0 resonance line(w), the 1s2p ^3P2-1s^2 1S0 magnetic quadrupole line(x), the 1s2p ^3P1-1 s^2 ^1S0 intercombination lines(y), the 1 s2p ^3S~1-1 s^2 ^1S0 forbidden line(z) in helium-like Ti Ⅹ Ⅺ and the 1 s2s2p ^2P3/2-1 s622s ^2S1/2 line(q) in lithium-like Ti Ⅹ Ⅹhave been recorded with a X-ray CCD camera. The experimental result shows that the wavelength resolution(λ/△ 2) is above 1000 and the elliptical crystal spectrometer is suitable for X-ray spectroscopy.  相似文献   

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