英语翻译Another method was proposed by Mazzoni et al.(2007) and named here extended FLD (eFLD).With a spectralresolution of 0.03 nm,they estimated F in the three main absorptionbands.With this very high resolution a number of dark lines appear in

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英语翻译Another method was proposed by Mazzoni et al.(2007) and named here extended FLD (eFLD).With a spectralresolution of 0.03 nm,they estimated F in the three main absorptionbands.With this very high resolution a number of dark lines appear in
英语翻译
Another method was proposed by Mazzoni et al.
(2007) and named here extended FLD (eFLD).With a spectral
resolution of 0.03 nm,they estimated F in the three main absorption
bands.With this very high resolution a number of dark lines appear in
the incident spectruminstead of one single absorption band (see Fig.2).
Similar to what has been described for cFLD and iFLD,the eFLD
method first reconstructs the apparent reflectance at all the resolved
absorption lines present in a single feature (i.e.,band).For this purpose
it assumes that local maxima in the incident irradiance spectrum
correspond to no absorption –which is not always satisfied – and fits r at
these local maxima to obtain a continuous reflectance baseline.F is then
determined by using this reflectance baseline,according to the following
equation:
In this
way,an assumption similar to those of iFLD is made on the reflectance
function only,while the spectral shape of F is not prescribed.
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英语翻译Another method was proposed by Mazzoni et al.(2007) and named here extended FLD (eFLD).With a spectralresolution of 0.03 nm,they estimated F in the three main absorptionbands.With this very high resolution a number of dark lines appear in
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Mazzoni et al(人名)提出了另一种方法。(2007)并且在这里被命名为延伸荧光检测器(eFLD),其光谱分辨率是0.03nm。他们估计F在三个主要的吸收波段。这一系列黑线随着甚高型分辨率出现在一个单一的吸收带而来代替频谱(见图2)。类似我们已经描述的cFLD和iFLD。这种方法(eFLD)首要目的是重建表面反射率在所有已知的吸收线呈现的一个单一特征(即波段)。因为这个目的,我们假设局部...

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Mazzoni et al(人名)提出了另一种方法。(2007)并且在这里被命名为延伸荧光检测器(eFLD),其光谱分辨率是0.03nm。他们估计F在三个主要的吸收波段。这一系列黑线随着甚高型分辨率出现在一个单一的吸收带而来代替频谱(见图2)。类似我们已经描述的cFLD和iFLD。这种方法(eFLD)首要目的是重建表面反射率在所有已知的吸收线呈现的一个单一特征(即波段)。因为这个目的,我们假设局部最大值在这个事件中的辐射谱没用相应的被吸收-并不总是满意-并且适合R这些局部最大值去获得连续的反射基线,根据下面的公式:
在这种方式下。类似的假设对那些iFLD仅仅是基于反射功能,其F的频谱形状并没有确定(规定)。

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另一种方法,提出了Mazzoni等。
(2007)和命名,这里FLD(eFLD扩展。与光谱
股东大会的决议,他们估计有华氏度(约为38.9 0.03纳米的三个主要的吸收
乐队。这非常高分辨率的出现在深色的线条
这个事件的一个单一的吸收spectruminstead乐队(见图2)。
类似被形容为cFLD和iFLD,eFLD
首先...

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另一种方法,提出了Mazzoni等。
(2007)和命名,这里FLD(eFLD扩展。与光谱
股东大会的决议,他们估计有华氏度(约为38.9 0.03纳米的三个主要的吸收
乐队。这非常高分辨率的出现在深色的线条
这个事件的一个单一的吸收spectruminstead乐队(见图2)。
类似被形容为cFLD和iFLD,eFLD
首先重建方法有明显的反射全部的解决
吸收线出现在同一特征(例如,乐队)。为达到这个目的
它假设极值的事件。辐照
与不吸收——并非总是满意——适合r
这些局部极值获得连续的反射率基线。F
利用该光谱测定基线,按照以下
方程。
这样,一个假定的iFLD类似的反射
函数的谱形,而不是规定的。
希望能帮到你

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