50 For what it concerns the method c) it, basically, requires to solve the equation: |
50 For what it concerns the method c) it, basically, requires to solve the equation: |
51 |
51 |
52 .. math:: |
52 .. math:: |
53 \alpha_s P_s + \alpha_p P_p = P |
53 \alpha_s P_s + \alpha_p P_p = P |
54 |
54 |
55 in two different of atmospheric layers with considerably different *VLDR*. So to calibrate in this way the implementation of automatic layer identification in the SCC is required. As at moment this feature is not yet available within the SCC **ONLY** the method b) is considered. |
55 in two different atmospheric layers with considerably different *VLDR*. So to calibrate in this way the implementation of automatic layer identification in the SCC is required. As at moment this feature is not yet available within the SCC **ONLY** the method b) is considered. |
56 |
56 |
57 1.3 SCC procedure to calculate the PLDRP |
57 1.3 SCC procedure to calculate the PLDRP |
58 ---------------------------------------- |
58 ---------------------------------------- |
59 |
59 |
60 According to what mentioned before the SCC calculates the *PLDR* through the following steps: |
60 According to what mentioned before the SCC calculates the *PLDR* through the following steps: |
143 Let's suppose, for example, we have the perpendicular polarized lidar signal on the transmitted channel and the parallel polarized on reflected channel. For an ideal system (no diattenuation and cross-talk) we have: |
143 Let's suppose, for example, we have the perpendicular polarized lidar signal on the transmitted channel and the parallel polarized on reflected channel. For an ideal system (no diattenuation and cross-talk) we have: |
144 |
144 |
145 .. math:: |
145 .. math:: |
146 G_T=1 , \qquad H_T=-1, \qquad G_R=1, \qquad H_R=1 |
146 G_T=1 , \qquad H_T=-1, \qquad G_R=1, \qquad H_R=1 |
147 |
147 |
148 If, on the other hands, we have the perpendicular polarized lidar signal on reflected channel and the total polarized on the transmitted for and ideal system we have: |
148 If, on the other hand, we have the perpendicular polarized lidar signal on reflected channel and the total polarized on the transmitted for and ideal system we have: |
149 |
149 |
150 .. math:: |
150 .. math:: |
151 G_T=1 , \qquad H_T=0, \qquad G_R=1, \qquad H_R=-1 |
151 G_T=1 , \qquad H_T=1, \qquad G_R=1, \qquad H_R=-1 |
152 |
152 |
153 |
153 |
154 **Table 1.1:** Polarization cross-talk correction parameters for ideal systems |
154 **Table 1.1:** Polarization cross-talk correction parameters for ideal systems |
155 |
155 |
156 +----------------------+-----------------------------+-----------------+-----------------+-----------------+ |
156 +----------------------+-----------------------------+-----------------+-----------------+-----------------+ |
160 + +-----------------------------+-----------------+-----------------+-----------------+ |
160 + +-----------------------------+-----------------+-----------------+-----------------+ |
161 | | :math:`G_T` | :math:`H_T` | :math:`G_R` | :math:`H_R` | |
161 | | :math:`G_T` | :math:`H_T` | :math:`G_R` | :math:`H_R` | |
162 +----------------------+-----------------------------+-----------------+-----------------+-----------------+ |
162 +----------------------+-----------------------------+-----------------+-----------------+-----------------+ |
163 | total | 1 | 0 | 1 | 0 | |
163 | total | 1 | 0 | 1 | 0 | |
164 +----------------------+-----------------------------+-----------------+-----------------+-----------------+ |
164 +----------------------+-----------------------------+-----------------+-----------------+-----------------+ |
165 | parallel | 1 | 1 | 1 | 1 | |
165 | parallel | 1 | 1 | 1 | -1 | |
166 +----------------------+-----------------------------+-----------------+-----------------+-----------------+ |
166 +----------------------+-----------------------------+-----------------+-----------------+-----------------+ |
167 | cross | 1 | -1 | 1 | -1 | |
167 | cross | 1 | -1 | 1 | +1 | |
168 +----------------------+-----------------------------+-----------------+-----------------+-----------------+ |
168 +----------------------+-----------------------------+-----------------+-----------------+-----------------+ |
169 |
169 |
170 The *apparent calibration factor* (:math:`\eta^*`), *the calibration factor correction* (*K*) and the *polarization cross-talk correction parameters* are stored by **ELPP** module in the intermediate NetCDF files using the following variables: |
170 The *apparent calibration factor* (:math:`\eta^*`), *the calibration factor correction* (*K*) and the *polarization cross-talk correction parameters* are stored by **ELPP** module in the intermediate NetCDF files using the following variables: |
171 |
171 |
172 - :code:`Polarization_Channel_Gain_Factor` (*apparent calibration factor* - :math:`\eta^*` ) |
172 - :code:`Polarization_Channel_Gain_Factor` (*apparent calibration factor* - :math:`\eta^*` ) |
331 :scale: 100 % |
331 :scale: 100 % |
332 :align: center |
332 :align: center |
333 |
333 |
334 **Figure 3.1**: How to select signal types |
334 **Figure 3.1**: How to select signal types |
335 |
335 |
336 The first modification concerns the settings of the channel type for the 532 cross and 532 parallel polarization channels. Starting from SCC v4.0 polarization channels are identified as transmitted and reflected polarization channels and not on the base of their polarization state. So suppose if we suppose the cross polarized channel is transmitted by a polarizer beam splitter cube and the parallel is reflected the value reported in table 3.1 should be modified as they appear in table 3.2. So using the SCC web interface, the signal type of the 532 cross channel should be changed from :code:`elCP` to :code:`elPT` and in the same way the 532 parallel channel should be changed from :code:`elPP` to :code:`elPR` (see figure 3.1). |
336 The first modification concerns the settings of the channel type for the 532 cross and 532 parallel polarization channels. Starting from SCC v4.0 polarization channels are identified as transmitted and reflected polarization channels and not on the base of their polarization state. So if we suppose that the cross polarized channel is transmitted by a polarizer beam splitter cube, and the parallel is reflected, the value reported in table 3.1 should be modified as they appear in table 3.2. So using the SCC web interface, the signal type of the 532 cross channel should be changed from :code:`elCP` to :code:`elPT` and in the same way the 532 parallel channel should be changed from :code:`elPP` to :code:`elPR` (see figure 3.1). |
337 |
337 |
338 **Table 3.2:** The same of table 3.1 but with new channel types |
338 **Table 3.2:** The same of table 3.1 but with new channel types |
339 introduced in SCC v4.0 |
339 introduced in SCC v4.0 |
340 |
340 |
341 +----------------+--------------+----------------+-------------+-----------+ |
341 +----------------+--------------+----------------+-------------+-----------+ |
590 |
590 |
591 :code:`Raw_Lidar_Data[2][2][points]` :math:`\rightarrow` 3\ :sup:`rd` measured transmitted signal at -45 degrees |
591 :code:`Raw_Lidar_Data[2][2][points]` :math:`\rightarrow` 3\ :sup:`rd` measured transmitted signal at -45 degrees |
592 |
592 |
593 :code:`Raw_Lidar_Data[2][3][points]` :math:`\rightarrow` 3\ :sup:`rd` measured transmitted signal at -45 degrees |
593 :code:`Raw_Lidar_Data[2][3][points]` :math:`\rightarrow` 3\ :sup:`rd` measured transmitted signal at -45 degrees |
594 |
594 |
595 Once this file has been created it needs to be submitted to the SCC and linked to the configuration “depol\_calibration”. The result of the SCC analysis on this file will be the calculation of the calibration constant h\ :sup:`\*` that will be logged into the SCC database and can be used to calibrate Raman/Elastic backscat ter products (see section 3.3). |
595 Once this file has been created it needs to be submitted to the SCC and linked to the configuration “depol\_calibration”. The result of the SCC analysis on this file will be the calculation of the calibration constant h\ :sup:`\*` that will be logged into the SCC database and can be used to calibrate Raman/Elastic backscatter products (see section 3.3). |
596 |
596 |
597 3.3 Definition of “Raman/Elastic backscatter and linear depolarization ratio” |
597 3.3 Definition of “Raman/Elastic backscatter and linear depolarization ratio” |
598 ----------------------------------------------------------------------------- |
598 ----------------------------------------------------------------------------- |
599 |
599 |
600 In order to calculate the *PLDR* we need to modify the polarization related products linked to the “standard” measurement configurations (the configuration called “nighttime” and/or “daytime” in table 3.2). |
600 In order to calculate the *PLDR* we need to modify the polarization related products linked to the “standard” measurement configurations (the configuration called “nighttime” and/or “daytime” in table 3.2). |
633 | Elastic backscatter | 7 | Elastic backscatter | x | x | |
633 | Elastic backscatter | 7 | Elastic backscatter | x | x | |
634 | | | | | | |
634 | | | | | | |
635 | 1064nm | | | | | |
635 | 1064nm | | | | | |
636 +-----------------------+--------------+-----------------------+-------------+-----------+ |
636 +-----------------------+--------------+-----------------------+-------------+-----------+ |
637 |
637 |
638 Product ID=1, 2, 4, 5, 7 do not need any modification as they do not involve polarization channels. The only product that need to be modified are the Product ID=3 and 6. To produce b532 files containing also *PLDR* we need to modify the “nighttime” and “daytime” configurations to include a product of type “Raman bakscatter and linear depolarization ratio” or “Elastic bakscatter and linear depolarization ratio” respectively. So the configuration reported in table 3.4 should be |
638 Product ID=1, 2, 4, 5, 7 do not need any modification as they do not involve polarization channels. The only product that need to be modified are the Product ID=3 and 6. To produce b532 files containing also *PLDR* we need to modify the “nighttime” and “daytime” configurations to include a product of type “Raman backscatter and linear depolarization ratio” or “Elastic bakscatter and linear depolarization ratio” respectively. So the configuration reported in table 3.4 should be |
639 changed to match what is included in table 3.5. |
639 changed to match what is included in table 3.5. |
640 |
640 |
641 **Table 3.5:** The same of table 3.4 but with new product types introduced in SCC v4.0 |
641 **Table 3.5:** The same of table 3.4 but with new product types introduced in SCC v4.0 |
642 |
642 |
643 +-----------------------+--------------+-----------------------------------------------------------+-------------+-----------+ |
643 +-----------------------+--------------+-----------------------------------------------------------+-------------+-----------+ |