Go to the documentation of this file.
46 #define DESCRIPTION(x) x
116 (
NAME(
"abs_coef" ),
119 "The matrix of total absorption coefficients.\n"
121 "This variable is not used explicitly in a standard calculation, where\n"
122 "absorption comes from the lookup table *abs_lookup*. However, it is\n"
123 "useful for testing the methods that actually calculate line-by-line\n"
124 "absorption, which have this variable as output. These methods are\n"
125 "called internally by the method *abs_lookupCreate*, which generates\n"
126 "the lookup table.\n"
128 "Dimensions: [f_grid, abs_p]\n"
136 (
NAME(
"abs_coef_per_species" ),
139 "These are the absorption coefficients individually for each\n"
140 "tag group. The Array contains one matrix for each tag group,\n"
141 "the matrix format is the same as that of abs_coef\n"
143 GROUP(
"ArrayOfMatrix" )));
156 (
NAME(
"abs_cont_models" ),
159 "Continuum / full model absorption model description parameter.\n"
160 "See the WSV `abs_cont_names' for a detailed description\n"
161 "of the allowed continuum models. There should be one string here\n"
162 "for each entry in `abs_cont_names'.See also the online\n"
163 "documentation in arts/doc/doxygen/html/continua_cc.html.\n"
165 GROUP(
"ArrayOfString" )));
169 (
NAME(
"abs_cont_names" ),
172 "Continuum / full model absorption tag names. This variable should\n"
173 "contain a list of tag names of continuum and full models, respectively.\n"
174 "Associated with this WSV is the WSV\n"
175 "`abs_cont_models' which contains the specific model version of\n"
176 "each continuum / full model absorption tag and the WSV\n"
177 "`abs_cont_parameters' which should contain the continuum / full model\n"
178 "user defined parameters. The user defined parameters are only used when\n"
179 "the specified model is 'user'. See also the online documentation in\n"
180 "arts/doc/doxygen/html/continua_cc.html.\n"
182 "The following full water vapor models are implemented:\n"
183 "'H2O-MPM87': absorption model (line and continuum) according to \n"
185 " A contribution to modeling atmospheric millimeter-wave properties,\n"
186 " Frequenz, 41, 1987, 31-36\n"
188 " H. J. Liebe and D. H. Layton,\n"
189 " Millimeter-wave properties of the atmosphere:\n"
190 " Laboratory studies and propagation modeling,\n"
191 " U.S. Dept. of Commerce, National Telecommunications and Information\n"
192 " Administration, Institute for Communication Sciences,\n"
193 " 325 Broadway, Boulder, CO 80303-3328, report 87224.\n"
194 "'H2O-MPM89': absorption model (line and continuum) according to \n"
195 " H. J. Liebe,\n Int. J. Infrared and Millimeter Waves, 10(6), 1989, 631\n"
196 "'H2O-MPM93': absorption model (line and continuum) according to \n"
197 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
198 " Propagation modeling of moist air and suspended water/ice\n"
199 " particles at frequencies below 1000 GHz,\n"
200 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
201 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21 \n"
202 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
203 "'H2O-CP98': absorption model (line and continuum) according to \n"
204 " S. L. Cruz-Pol et al.,\n Radio Science, 33(5), 1319, 1998"
205 " (ece.uprm.edu/~pol/Atmosphere.html)\n"
206 "'H2O-PWR98': absorption model (line and continuum) according to \n"
207 " P. W. Rosenkranz,\n "
208 " Radio Science, 33(4), 919, 1998, Radio Science, 34(4), 1025, 1999\n"
209 " (ftp: mesa.mit.edu/phil/lbl_rt).\n"
211 "The following full oxygen models are implemented:\n"
212 "'O2-MPM93': absorption model (line and continuum) according to\n"
213 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
214 " Propagation modeling of moist air and suspended water/ice\n"
215 " particles at frequencies below 1000 GHz,\n"
216 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
217 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21\n"
218 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
219 "'O2-PWR93': absorption model (line and continuum) according to \n"
220 " P. W. Rosenkranz,\n Chapter 2, in M. A. Janssen, \n"
221 " Atmospheric Remote Sensing by Microwave Radiometry\n"
222 " John Wiley & Sons, Inc., 1993 (mesa.mit.edu/phil/lbl_rt)\n"
224 "The following continuum parameterizations are implemented:\n"
225 "H2O-H2O ('H2O-SelfContStandardType'):\n"
226 " P. W. Rosenkranz, \n"
227 " Radio Science, Vol. 33, No 4, Pages 919-928, 1998 and \n"
228 " Radio Science, Vol. 34, No 4, Page 1025, 1999 (mesa.mit.edu/phil/lbl_rt)\n"
229 "H2O-air ('H2O-ForeignContStandardType'): \n"
230 " P. W. Rosenkranz, \n"
231 " Radio Science, Vol. 33, No 4, Pages 919-928, 1998 and \n"
232 " Radio Science, Vol. 34, No 4, Page 1025, 1999 (mesa.mit.edu/phil/lbl_rt)\n"
233 "H2O-air ('H2O-ContMPM93'): \n"
234 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
235 " Propagation modeling of moist air and suspended water/ice\n"
236 " particles at frequencies below 1000 GHz,\n"
237 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
238 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21\n"
239 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
240 "O2-air ('O2-SelfContStandardType'):\n"
241 " P. W. Rosenkranz,\n"
242 " Chapter 2, in M. A. Janssen,\n"
243 " Atmospheric Remote Sensing by Microwave Radiometry,\n"
244 " John Wiley & Sons, Inc., 1993\n"
245 " (mesa.mit.edu/phil/lbl_rt)\n"
246 " and also described in \n"
247 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
248 " Propagation modeling of moist air and suspended water/ice\n"
249 " particles at frequencies below 1000 GHz,\n"
250 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
251 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21\n"
252 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
253 "N2-N2 ('N2-SelfContStandardType'):\n"
254 " The functional form of Rosenkranz but with more input parameters.\n"
255 " P. W. Rosenkranz,\n"
256 " Chapter 2, in M. A. Janssen,\n"
257 " Atmospheric Remote Sensing by Microwave Radiometry,\n"
258 " John Wiley & Sons, Inc., 1993 (mesa.mit.edu/phil/lbl_rt)\n"
259 "N2-N2 ('N2-SelfContMPM93'):\n"
260 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
261 " Propagation modeling of moist air and suspended water/ice\n"
262 " particles at frequencies below 1000 GHz,\n"
263 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
264 " Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21 \n"
265 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
266 "CO2-CO2 ('CO2-SelfContPWR93'):\n"
267 " P. W. Rosenkranz,\n"
268 " Chapter 2, in M. A. Janssen,\n"
269 " Atmospheric Remote Sensing by Microwave Radiometry,\n"
270 " John Wiley & Sons, Inc., 1993 (mesa.mit.edu/phil/lbl_rt)\n"
271 "CO2-N2 ('CO2-ForeignContPWR93'):\n"
272 " P. W. Rosenkranz,\n"
273 " Chapter 2, in M. A. Janssen,\n"
274 " Atmospheric Remote Sensing by Microwave Radiometry,\n"
275 " John Wiley & Sons, Inc., 1993 (mesa.mit.edu/phil/lbl_rt)\n"
277 "The following cloud absorption models are implemented:\n"
278 "Suspended water droplet ('liquidcloud-MPM93') \n"
279 " absorption parameterization from the MPM93 model:\n"
280 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
281 " Propagation modeling of moist air and suspended water/ice\n"
282 " particles at frequencies below 1000 GHz,\n"
283 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
284 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21\n"
285 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
286 "Ice water droplet absorption ('icecloud-MPM93') \n"
287 " parameterization from MPM93 model:\n"
288 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
289 " Propagation modeling of moist air and suspended water/ice\n"
290 " particles at frequencies below 1000 GHz,\n"
291 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
292 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21\n"
293 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
295 "The following rain extinction model is implemented:\n"
296 "Rain extinction parameterization ('rain-MPM93') from the\n"
297 " MPM93 model, described in:\n"
299 " MPM - An Atmospheric Millimeter-Wave Propagation Model,\n"
300 " Int. J. Infrared and Millimeter Waves, vol. 10(6),\n"
301 " pp. 631-650, 1989;\n"
303 " Olsen, R.L., D.V. Rogers, and D. B. Hodge,\n"
304 " The aR^b relation in the calculation of rain attenuation,\n"
305 " IEEE Trans. Antennas Propagat., vol. AP-26, pp. 318-329, 1978.\n"
306 " IMPORTANT NOTE: rain-MPM93 parameterizes the EXTINCTION by rain,\n"
307 " not just the absorption. Therefore it is not suitable for \n"
308 " calculating thermal emission by rain!\n"
309 " Please use rain-MPM93 only for calculation of attenuation.\n"
311 GROUP(
"ArrayOfString" )));
315 (
NAME(
"abs_cont_parameters" ),
318 "Continuum model parameters. See the WSV *abs_cont_names*\n"
319 "for a detailed description of the allowed continuum models. There\n"
320 "should be one parameter vector here for each entry in\n"
321 "*abs_cont_names*. See also the online documentation in\n"
322 "arts/doc/doxygen/html/continua_cc.html.\n"
324 GROUP(
"ArrayOfVector" )));
331 "The total water profile associated with the pressures in *abs_p* [-]\n"
337 (
NAME(
"abs_lines" ),
340 "A list of spectral line data.\n"
342 GROUP(
"ArrayOfLineRecord" )));
346 (
NAME(
"abs_lineshape" ),
349 "Lineshape specification: function, norm, cutoff. There is one entry for\n"
350 "each abs_tag, not for each species. This means if you have several\n"
351 "abs_tags for different isotopes or transitions of a species, you\n"
352 "may use different lineshapes.\n"
354 GROUP(
"ArrayOfLineshapeSpec" )));
358 (
NAME(
"abs_lines_per_species" ),
361 "A list of spectral line data for each tag.\n"
362 "Dimensions: (tag_groups.nelem()) (# of lines for this tag)\n"
364 GROUP(
"ArrayOfArrayOfLineRecord" )));
368 (
NAME(
"abs_lookup" ),
371 "An absorption lookup table.\n"
373 "This holds an absorption lookup table, as well as all information that\n"
374 "is necessary to use the table to extract absorption. Extraction\n"
375 "routines are implemented as member functions. \n"
377 "This has quite a complicated structure. See Doxygen documentation for\n"
378 "class GasAbsLookup for details. See also the Arts User Guide, \n"
379 "Chapter 3.1 (\"The gas absorption lookup table\").\n"
381 GROUP(
"GasAbsLookup" )));
388 "Nonlinear species for absorption lookup table generation.\n"
390 "A list of absorption species that should be treated non-linearly.\n"
391 "This means that the H2O VMR should be varied when calculating the\n"
392 "lookup table for those species.\n"
394 "A typical example is for this to containt the Rosenkranz full\n"
395 "absorption model species for water vapor and oxygen \n"
396 "([\"H2O-PWR98\", \"O2-PWR93\"]).\n"
398 "It only makes sense to put a species here if is either a water vapor\n"
399 "species, or some other species that uses *abs_h2o*, that is, for which\n"
400 "the absorption coefficient depends directly on water vapor.\n"
402 "See user guide and online documentation of *abs_pts* and *abs_lookupCreate*\n"
403 "for more details and usage examples.\n"
405 GROUP(
"ArrayOfArrayOfSpeciesTag" )));
409 (
NAME(
"abs_nls_pert" ),
412 "Fractional perturbations for the nonlinear species in the absorption\n"
415 "This is a vector of fractional perturbations that should contain 1\n"
416 "(the unperturbed reference profile). A value of 0 may lead to error\n"
417 "messages from some absorption routines, so a possible content for this\n"
418 "variable is: [1e-24, 1, 2].\n"
419 "(This is similar to *abs_t_pert*, but multiplicative, not additive.)\n"
425 (
NAME(
"abs_nls_interp_order" ),
428 "The interpolation order to use when interpolating absorption between\n"
429 "the H2O values given by *abs_nls_pert*. This is used by methods\n"
430 "extracting absorption coefficients from the lookup table, and by\n"
431 "methods setting up parameters for lookup table generation. Has a\n"
432 "default value, which is set in general.arts.\n"
434 "Note that the number of points used in the interpolation scheme is\n"
435 "interpolation order + 1 (e.g., two for first order interpolation).\n"
441 (
NAME(
"abs_p_interp_order" ),
444 "The interpolation order to use when interpolating absorption\n"
445 "between pressure levels. This is used by methods extracting\n"
446 "absorption coefficients from the lookup table, and by methods\n"
447 "setting up parameters for lookup table generation. Has a\n"
448 "default value, which is set in general.arts.\n"
450 "Note that the number of points used in the interpolation scheme is\n"
451 "interpolation order + 1 (e.g., two for first order interpolation).\n"
457 (
NAME(
"abs_t_pert" ),
460 "Temperature perturbations for the absorption lookup table.\n"
462 "This is a vector containing temperature perturbations (in Kelvin) that\n"
463 "should be added to the reference temperature profile. (Similar to\n"
464 "*abs_nls_pert*, but additive, not multiplicative.) Should normally\n"
465 "contain 0, to include the reference profile itself. Example content:\n"
472 (
NAME(
"abs_t_interp_order" ),
475 "The interpolation order to use when interpolating absorption between\n"
476 "the temperature values given by *abs_t_pert*. This is used by methods\n"
477 "extracting absorption coefficients from the lookup table, and by\n"
478 "methods setting up parameters for lookup table generation. Has a\n"
479 "default value, which is set in general.arts.\n"
481 "Note that the number of points used in the interpolation scheme is\n"
482 "interpolation order + 1 (e.g., two for first order interpolation).\n"
488 (
NAME(
"abs_lookup_is_adapted" ),
491 "Flag to indicate whether *abs_lookupAdapt* has already been\n"
494 "Values: 0=false, 1=true.\n"
503 "The total nitrogen profile associated with the pressures in *abs_p* [-]\n"
512 "List of pressures to be used for the calculation of absorption\n"
515 "This can be copied from the global *p_grid*, but could also be\n"
518 "Any absorption method should check that the length of this vector\n"
519 "is the same as that of *abs_t*\n"
521 "Dimension: [number of pressures]\n"
529 (
NAME(
"abs_scalar_gas" ),
532 "Scalar gas absorption coefficients.\n"
534 "This contains the absorption coefficients for one point in the\n"
535 "atmosphere (one set of pressure, temperature, and VMR values). There\n"
536 "are two distinct cases:\n"
538 "Case a: For all frequencies and all species:\n"
539 "Dimension: [ f_grid, abs_species ]\n"
541 "Case b: For a single frequency for all species:\n"
542 "Dimension: [ 1, abs_species ]\n"
550 (
NAME(
"abs_scalar_gas_agenda" ),
559 (
NAME(
"abs_field" ),
562 "Scalar gas absorption field.\n"
564 "Contains the scalar gas absorption for all species as a function of\n"
565 "*f_grid*, *p_grid*, *lat_grid*, and *lon_grid*. \n"
567 "This is mainly for testing and plotting gas absorption. For RT\n"
568 "calculations, gas absorption is calculated or extracted locally,\n"
569 "therefore there is no need to store a global field. But this variable\n"
570 "is handy for easy plotting of absorption vs. pressure, for example.\n"
574 "Dimensions: [species, f_grid, p_grid, lat_grid, lon_grid]\n"
576 GROUP(
"Tensor5" )));
580 (
NAME(
"abs_species" ),
583 "Tag groups for scalar gas absorption.\n"
585 "This is an array of arrays of SpeciesTag tag definitions. It defines the\n"
586 "available tag groups for the calculation of scalar gas absorption\n"
587 "coefficients. See online documentation of method *SpeciesSet* for\n"
588 "more detailed information how tag groups work and some examples.\n"
590 GROUP(
"ArrayOfArrayOfSpeciesTag" )));
597 "List of temperatures to be used for the calculation of absorption\n"
600 "In contrast to the global *t_field*, this is just a vector. Any\n"
601 "absorption method should check that the length of this vector is the\n"
602 "same as that of *abs_p*\n"
604 "Dimension: [number of pressures]\n"
615 "Total absorption vector.\n"
617 "This variable contains the absorption coefficient vector which \n"
618 "is used in the RTE calculation. It is \n"
619 "the physical absorption which includes particle absorption \n"
620 "for all chosen particle types as well as gaseous absorption for\n"
621 "all chosen gaseous species.\n"
622 "The vector is calculated by the agendas *opt_prop_gas_agenda* \n"
623 "and, if scattering calculations are performed, \n"
624 "*opt_prop_part_agenda* \n"
625 "The dimensision of the variable adapts to *stokes_dim*.\n"
627 "See further the ARTS user guide (AUG). Use the index to find where\n"
628 "this variable is discussed. The variable is listed as a subentry to\n"
629 "\"workspace variables\".\n"
631 "Usage: Output of the agendas *opt_prop_gas_agenda* \n"
632 " and *opt_prop_part_agenda* \n"
636 "Dimensions: [f_grid, stokes_dim]\n"
642 (
NAME(
"abs_vec_spt"),
645 "Absorption vector for a single particle type.\n"
647 "This variable contains the elements of absorption vector of a \n"
648 "single particle, given It is calculated in the agenda \n"
649 "*spt_calc_agenda*.\n"
651 "ARTS user guide (AUG) gives the formulas used for computing all \n"
652 "the elements of absorption vector.\n"
654 "Usage: Input and Output of the method abs_vec_sptCalc\n"
658 "Dimensions: [part_types,stokes_dim]\n"
660 GROUP(
"Matrix" ) ));
667 "The VMRs (unit: absolute number) on the abs_p grid.\n"
668 "Dimensions: [tag_groups.nelem(), abs_p.nelem()]\n"
674 (
NAME(
"abs_xsec_per_species" ),
677 "Absorption cross sections.\n"
679 "This variable contains absorption cross section xsec individually for\n"
680 "each tag group. The Array contains one matrix for each tag group, the\n"
681 "matrix format is the same as that of abs_coef.\n"
683 "Dimensions: [abs_species](f_grid, abs_p)\n"
685 "Unit: m^2 (alpha = xsec * n * VMR),\n"
686 " where n is total density.\n"
688 GROUP(
"ArrayOfMatrix" )));
692 (
NAME(
"antenna_dim" ),
695 "The dimensionality of the antenna pattern (1-2).\n"
697 "A dimensionality of 1 means that only the respons variation in the\n"
698 "zenith direction is considered. The provided respons shall then be the\n"
699 "integrated in the azimuth direction. For 2D, the respons of the\n"
700 "antenna has both a zenith and azimuth variation.\n"
702 "Usage: Set by the user.\n"
704 "Unit: Integer value [1-2].\n"
710 (
NAME(
"antenna_los" ),
713 "The relative line-of-sight of each antenna pattern.\n"
715 "This variable describes the line-of-sight of the individual antennae\n"
716 "relative to *sensor_los*. If only one antenna is present the matrix\n"
717 "should contain a row of zero(s). The number of columns corresponds to\n"
718 "the *antenna_dim*, with the first column containing zenith angles\n"
719 "and the second azimuth angles. If each measurement block corresponds\n"
720 "to a single antenna pattern, the normal choice is to set the angle(s)\n"
721 "of this variable to zero.\n"
723 "See further the ARTS user guide (AUG). Use the index to find where\n"
724 "this variable is discussed. The variable is listed as a subentry to\n"
725 "\"workspace variables\".\n"
727 "Usage: Set by the user.\n"
729 "Unit: [ degrees, degrees ]\n"
731 "Size: [ number of antennae, 1 or 2 ]\n"
737 (
NAME(
"antenna_response" ),
740 "The antenna pattern/response.\n"
742 "This WSV describes the antenna response as a function of polarisation\n"
743 "(pol), frequencue (f), zenith angle (za) and azimuth angle (aa).\n"
745 "Polarisation dimension: If this dimension has size 1, the data are\n"
746 "applied for all polarisations of concern. The data are otherwise used\n"
747 "in sequential order. This signifies that, in general, the first\n"
748 "polarisation \"layer\" corresponds to the first stokes dimension\n"
749 "etc. An exception is if a polarisation rotation has been applied. In\n"
750 "any case, it is up to the user to ensure that polarisations are\n"
751 "consistently defined.\n"
753 "Frequency dimension: If this dimension has size 1, the data are\n"
754 "applied for all frequencies of concern. The given frequency must be\n"
755 "inside the frequency range of concern. A linear interpolation is\n"
756 "otherwise applied.\n"
758 "Zenith angle dimension: This dimension must always have a size >= 2\n"
759 "The response outside covered grid range is treated as zero. If\n"
760 "*antenna_dim* equals 1, the data should correspond to the response\n"
761 "integrated in the azimuthal direction.\n"
763 "Azimuth angle dimension: If *antenna_dim* equals 1, this dimension\n"
764 "must have size 1. A size >= 2 is otherwise required. The response\n"
765 "outside covered grid range is treated as zero.\n"
767 "Usage: Set by the user.\n"
771 " ArrayOfString field_names[N_pol]\n"
772 " Vector f_grid[N_f]\n"
773 " Vector za_grid[N_za]\n"
774 " Vector aa_grid[N_aa]\n"
775 " Tensor4 data[N_pol][N_f][N_za][N_aa]\n"
777 GROUP(
"GriddedField4" )));
781 (
NAME(
"atmosphere_dim" ),
784 "The atmospheric dimensionality (1-3).\n"
786 "This variable defines the complexity of the atmospheric structure.\n"
787 "The dimensionality is given by an integer between 1 and 3, where 1\n"
788 "means 1D etc. This is the master variable for the atmospheric\n"
789 "dimensionality, variables which size changes with the dimensionality\n"
790 "are checked to match this variable. \n"
792 "Methods adapt automatically to this variable. That is, it should\n"
793 "not be needed to change any methods if the dimensionality is\n"
794 "changed. However, not all methods are working for higher dimensions.\n"
796 "Usage: Set by the user.\n"
798 "Unit: Integer value.\n"
804 (
NAME(
"atm_fields_compact" ),
807 "A compact combination of all atmospheric fields for a clear-sky\n"
808 "calculation on a common set of grids.\n"
810 "This concerns temperature, altitude, and gas VMRs.\n"
812 "The data are stored in a *GriddedField4*.\n"
814 "The order of the fields must be:\n"
815 "T[K] z[m] VMR_1[1] ... VMR_n[1]\n"
816 "(the field names for the gases do not have to start with VMR_)\n"
818 "Usage: Used inside batch calculations, to hold successive atmospheric\n"
819 " states from an *ArrayOfGriddedField4*.\n"
821 "Possible future extensions: Add a similar variable\n"
822 "particle_fields_compact for hydrometeors?\n"
826 " ArrayOfString field_names[N_fields]\n"
827 " Vector p_grid[N_p]\n"
828 " Vector lat_grid[N_lat]\n"
829 " Vector lon_grid[N_lon]\n"
830 " Tensor4 data[N_fields][N_p][N_lat][N_lon]\n"
832 GROUP(
"GriddedField4" )));
836 (
NAME(
"atm_fields_compact_all" ),
839 "A compact combination of all atmospheric fields for a clear-sky\n"
840 "and cloud particle scattering calculation on a common set of grids.\n"
842 "This concerns temperature, altitude, scattering particles and gas VMRs.\n"
844 "The data are stored in a *GriddedField4*.\n"
846 "The order of the fields must be:\n"
847 "T[K] z[m] LWC[kg/m3] IWC[kg/m3] Rain[kg/m2/s] Snow[kg/m2/s] VMR_1[1] ... VMR_n[1]\n"
848 "(the field names for the gases do not have to start with VMR_)\n"
850 "Usage: Used inside batch calculations, to hold successive atmospheric\n"
851 " states from an *ArrayOfGriddedField4*.\n"
855 " ArrayOfString field_names[N_fields]\n"
856 " Vector p_grid[N_p]\n"
857 " Vector lat_grid[N_lat]\n"
858 " Vector lon_grid[N_lon]\n"
859 " Tensor4 data[N_fields][N_p][N_lat][N_lon]\n"
861 GROUP(
"GriddedField4" )));
865 (
NAME(
"backend_channel_response" ),
868 "The response of each backend channel.\n"
870 "The response is given as an *ArrayOfGriddedField1*. The grid consists of\n"
871 "relative frequencies. These relative frequencies are added to \n"
872 "*f_backend* to obtain the absolute frequency for each response value.\n"
873 "The actual data are the response at each frequency grid point.\n"
875 "There are here two options. If the array has length 1, the same\n"
876 "response is applied for all channels. Accordingly, this assumes that\n"
877 "all channels have the same response function. The second option is to\n"
878 "specify the response for each channel seperately. This signifies that\n"
879 "the *backend_channel_response* array has either 1 or n elements, where\n"
880 "n is the length of *f_backend*\n"
882 "Usage: Set by the user.\n"
884 "Size: Array[N_ch]\n"
889 GROUP(
"ArrayOfGriddedField1" )));
893 (
NAME(
"backend_channel_response_multi" ),
896 "As *backend_channel_response* but describes an instrument with\n"
897 "muliple mixer/reciever chains.\n"
899 "See *f_backend_multi* for when to use this variable and size\n"
902 "Usage: Set by the user.\n "
904 GROUP(
"ArrayOfArrayOfGriddedField1" )));
908 (
NAME(
"basics_checked" ),
911 "OK-flag for basic variables and grids.\n"
913 "For example, this variable flags that the (clear-sky) atmosphere\n"
914 "and the surface are defined in a formally correct way, e.g. that\n"
915 "the sizes of atmospheric fields match the atmospheric grids.\n"
917 "Shall be set by *basics_checkedCalc*. See that WSM for treated WSVs.\n"
923 (
NAME(
"batch_atm_fields_compact" ),
926 "An array of compact atmospheric states.\n"
928 "This is used to hold a set of *atm_fields_compact* for batch\n"
931 GROUP(
"ArrayOfGriddedField4" )));
935 (
NAME(
"batch_atm_fields_compact_all" ),
938 "An array of compact atmospheric states, including scattering particles.\n"
940 "This is used to hold a set of *atm_fields_compact_all* for batch\n"
943 GROUP(
"ArrayOfGriddedField4" )));
947 (
NAME(
"batch_cloudbox_limits" ),
950 "An array of cloudbox_limits.\n"
952 "This is used to hold a set of *cloudbox-limits* for batch\n"
955 GROUP(
"ArrayOfArrayOfIndex" )));
959 (
NAME(
"batch_pnd_fields" ),
962 "An array of compact pnd states.\n"
964 "This is used to hold a set of 1D *pnd_field* for batch\n"
967 GROUP(
"ArrayOfTensor4" )));
971 (
NAME(
"cloudbox_checked" ),
974 "OK-flag for variables associated with the cloudbox.\n"
976 "This variable flags that cloudbox variables are defined in a formally\n"
977 "and practically correct way. For example, that there is sufficient\n"
978 "space between the cloudbox and edges of the model atmosphere (for\n"
979 "2D and 3D). Pure clear-sky variables are covered by *basics_checked*.\n"
981 "Relevant checks are performed by *cloudbox_checkedCalc.\n"
987 (
NAME(
"cloudbox_on" ),
990 "Flag to activate the cloud box.\n"
992 "Scattering calculations are confined to a part of the atmosphere\n"
993 "denoted as the cloud box. The extension of the cloud box is given by\n"
994 "*cloudbox_limits*. This variable tells methods if a cloud box is\n"
995 "activated or not. \n"
997 "See further the ARTS user guide (AUG). Use the index to find where\n"
998 "this variable is discussed. The variable is listed as a subentry to\n"
999 "\"workspace variables\".\n"
1001 "Usage: Set by the user.\n"
1009 (
NAME(
"cloudbox_limits" ),
1012 "The limits of the cloud box.\n"
1014 "This variable defines the extension of the cloud box. The cloud box \n"
1015 "is defined to be rectangular in the used coordinate system, with \n"
1016 "limits exactly at points of the involved grids. This means, for \n"
1017 "example, that the vertical limits of the cloud box are two pressure \n"
1018 "levels. For 2D, the angular extension of the cloud box is between \n"
1019 "two points of the latitude grid, and likewise for 3D but then also \n"
1020 "with a longitude extension between two grid points. The latitude and\n"
1021 "longitude limits for the cloud box cannot be placed at the end \n"
1022 "points of the corresponding grid as it must be possible to calculate\n"
1023 "the incoming intensity field.\n"
1025 "The variable *cloudbox_limits* is an array of index value with\n"
1026 "length twice *atmosphere_dim*. For each dimension there is a lower \n"
1027 "limit and an upper limit. The order of the dimensions is as usual \n"
1028 "pressure, latitude and longitude. The upper limit index must be \n"
1029 "greater then the lower limit index. For example, \n"
1030 "*cloudbox_limits* = [0 5 4 11 4 11] means that cloud box extends\n"
1031 "between pressure levels 0 and 5, and latitude and longitude points 4\n"
1034 "If *cloudbox_on* = 0, the content of this variable is neglected, but\n"
1035 "it must be initiated to some dummy values.\n"
1037 "See further the ARTS user guide (AUG). Use the index to find where\n"
1038 "this variable is discussed. The variable is listed as a subentry to\n"
1039 "\"workspace variables\".\n"
1041 "Usage: Set by the user, either directly or using a method\n"
1042 " checking the extension of scattering particles.\n"
1044 "Unit: Index values.\n"
1046 "Size: [ 2 * atmosphere_dim ]\n"
1048 GROUP(
"ArrayOfIndex" )));
1052 (
NAME(
"complex_n"),
1055 "Complex refractive index (n).\n"
1057 "This matrix describes the dielectric properties of a medium. \n"
1058 "A typical usage of this variable is to describe the properties of\n"
1059 "the surface (if it is assumed to be flat).\n"
1061 "This is a two-column matrix. The first column holds the real part\n"
1062 "of n, and the second column the imaginary part. The number of rows\n"
1063 "should match *f_grid*. The case of one row is also accepted,\n"
1064 "interpreted as that the refractive index is constant with \n"
1069 "Dimensions: [f_grid or 1,2]\n"
1071 GROUP(
"Matrix" ) ));
1078 "Derivative of *iy* with respect to retrieval quantities.\n"
1080 "The variable gives the derivative if *iy* with respect to some\n"
1081 "variables (but not all jacobian variables). Handled are only variables\n"
1082 "affecting monochromatic pencil beam radiances where an (semi-)\n"
1083 "analytical expression can be applied (and that this calculation way\n"
1084 "has been selected when the jacobian has been set-up).\n"
1086 "Usage: Output of *iy_clearsky_agenda*.\n"
1089 " [n_quantities][ ppath.np, f_grid, stokes_dim ]\n"
1091 GROUP(
"ArrayOfTensor3" )));
1095 (
NAME(
"doit_conv_flag" ),
1098 "Flag for the convergence test.\n"
1100 "This variable is initialized with 0 inside the method \n"
1101 "*doit_i_fieldIterate*.\n"
1102 "If after an iteration the convergence test is fulfilled, 1 is \n"
1103 "assigned which means that the iteration is completed. \n"
1105 "Usage: Method output. \n"
1111 (
NAME(
"doit_conv_test_agenda" ),
1116 GROUP(
"Agenda" )));
1120 (
NAME(
"doit_i_field" ),
1123 "Radiation field.\n"
1125 "This variable is used to store the monochromatic radiation field \n"
1126 "inside the cloudbox which is found by an iterative solution (DOIT).\n"
1127 "Refer to AUG for further information.\n"
1129 "Usage: Method output. \n"
1131 "Unit: W / (m^2 Hz sr) for each Stokes component.\n"
1133 "Size: [(cloudbox_limits[1] - cloudbox_limits[0]) +1, \n"
1134 " (cloudbox_limits[3] - cloudbox_limits[2]) +1, \n"
1135 " (cloudbox_limits[5] - cloudbox_limits[4]) +1, \n"
1136 " N_za, N_aa, N_i ]\n"
1138 GROUP(
"Tensor6" )));
1142 (
NAME(
"doit_i_field1D_spectrum" ),
1145 "Radiation field for the whole frequency spectrum. \n"
1147 "This variable holds the radiation field. In contrast to \n"
1148 "*doit_i_field* this variable has an additional freqeuncy \n"
1149 "dimension. This variable is only used for 1D DOIT \n"
1152 "Usage: Output of *DoitCloudboxFieldPut*\n"
1154 "Unit: W / (m^2 Hz sr)\n"
1157 " (cloudbox_limits[1] - cloudbox_limits[0]) +1, \n"
1158 " N_za, N_aa, N_i ]\n"
1160 GROUP(
"Tensor4" )));
1164 (
NAME(
"doit_i_field_old" ),
1167 "Intensity field inside the cloudbox.\n"
1169 "This variable is used to store the intensity field inside the\n"
1170 "cloudbox while performing the iteration. One has to store the\n"
1171 "intensity field of the previous iteration to be able to do the \n"
1172 "convergence test after each iteration.\n"
1173 "Refer to AUG for more information.\n"
1175 "Usage: Method output. \n"
1177 "Unit: W / (m^2 Hz sr) for each Stokes component.\n"
1179 "Size: [(cloudbox_limits[1] - cloudbox_limits[0]) +1, \n"
1180 " (cloudbox_limits[3] - cloudbox_limits[2]) +1, \n"
1181 " (cloudbox_limits[5] - cloudbox_limits[4]) +1, \n"
1182 " N_za, N_aa, N_i ]\n"
1184 GROUP(
"Tensor6" )));
1188 (
NAME(
"doit_is_initialized" ),
1191 "Flag to determine if *DoitInit* was called.\n"
1193 "This flag is checked by *ScatteringDoit* to make sure that\n"
1194 "*DoitInit* was called before.\n"
1200 (
NAME(
"doit_iteration_counter" ),
1203 "Counter for number of iterations.\n"
1205 "This variable holds the number of iterations \n"
1206 "while solving the VRTE using the DOIT method. \n"
1212 (
NAME(
"doit_mono_agenda" ),
1217 GROUP(
"Agenda" )));
1221 (
NAME(
"doit_rte_agenda" ),
1226 GROUP(
"Agenda" )));
1230 (
NAME(
"doit_scat_field_agenda" ),
1235 GROUP(
"Agenda" )));
1239 (
NAME(
"doit_scat_field" ),
1242 "Scattered field field inside the cloudbox.\n"
1244 "This variable holds the value of the scattering integral for all\n"
1245 "points inside the cloudbox. For more information refer to AUG.\n"
1247 "Usage: Input to *doit_i_fieldUpdate...*. \n"
1249 "Unit: W / (m^2 Hz sr) for each Stokes component.\n"
1251 "Size: [(cloudbox_limits[1] - cloudbox_limits[0]) +1, \n"
1252 " (cloudbox_limits[3] - cloudbox_limits[2]) +1, \n"
1253 " (cloudbox_limits[5] - cloudbox_limits[4]) +1, \n"
1254 " N_za, N_aa, N_i ]\n"
1256 GROUP(
"Tensor6" )));
1260 (
NAME(
"doit_za_grid_opt" ),
1263 "Optimized zenith angle grid.\n"
1265 "Output of the method *doit_za_grid_optCalc*.\n"
1267 "Usage: Output of *doit_za_grid_optCalc* \n"
1271 GROUP(
"Vector" )));
1275 (
NAME(
"doit_za_grid_size" ),
1278 "Number of equidistant grid points of the zenith angle grid, \n"
1279 "defined from 0 to 180 deg, for the scattering integral calculation. \n"
1281 "Usage: Output of *DoitAngularGridsSet*.\n"
1287 (
NAME(
"doit_za_interp" ),
1290 "Flag for interplation method in zenith angle dimension.\n"
1292 "0 - linear interpolation \n"
1293 "1 - cubic interpolation \n"
1295 "Usage: Set by user in *doit_za_interpSet*. \n"
1301 (
NAME(
"emission" ),
1304 "Thermal emission source term.\n"
1306 "This variable holds the emission at one position along the\n"
1307 " propagation path. Inside scattering methods, such as DOIT, the\n"
1308 "calculation of this source term can be hard coded.\n"
1310 "Usage: Set by *emission_agenda*.\n"
1312 "Unit: W / (m^2 Hz sr) or optical thickness \n"
1314 "Dimensions: [ f_grid ]\n"
1316 GROUP(
"Vector" )));
1320 (
NAME(
"emission_agenda" ),
1325 GROUP(
"Agenda" )));
1329 (
NAME(
"ext_mat" ),
1332 "Total extinction matrix.\n"
1334 "This variable contains the extinction coefficient matrix which\n"
1335 "is used in the RT calculation in the cloudbox . It is the physical\n"
1336 "extinction matrix which includes particles extinction for all chosen\n"
1337 "particle types and gaseous extinction for all chosen gaseous species.\n"
1339 "See further the ARTS user guide (AUG). Use the index to find where\n"
1340 "this variable is discussed. The variable is listed as a subentry to\n"
1341 "\"workspace variables\".\n"
1343 "Usage: Output of the agendas *opt_prop_gas_agenda* \n"
1344 " and *opt_prop_part_agenda* \n"
1346 "Unit: [Hz, m^2, m^2] "
1348 "Dimensions: [f_grid, stokes_dim, stokes_dim]\n"
1350 GROUP(
"Tensor3" )));
1354 (
NAME(
"ext_mat_spt" ),
1357 "Extinction matrix for a single particle type.\n"
1359 "This variable contains the elements for extinction matrix of a \n"
1360 "single particle for a given propagation direction. It is calculated\n"
1361 "input as well as the output of the agenda *spt_calc_agenda*. \n"
1363 "Usage: Output of *spt_calc_agenda* \n"
1367 "Dimensions: [part_types, stokes_dim, stokes_dim]\n"
1369 GROUP(
"Tensor3" )));
1373 (
NAME(
"file_index" ),
1376 "Index number for files.\n"
1378 "See *WriteXMLIndexed* for further information.\n"
1380 "Usage: Input to *WriteXMLIndexed* and *ReadXMLIndexed*. \n"
1386 (
NAME(
"forloop_agenda" ),
1391 GROUP(
"Agenda" )));
1395 (
NAME(
"forloop_index" ),
1398 "The index for for-loops.\n"
1400 "This is the index that is used by method *ForLoop* to loop over\n"
1401 "*forloop_agenda*. \n"
1407 (
NAME(
"f_backend" ),
1410 "The frequency position of each backend (spectrometer) channel.\n"
1412 "Usage: Set by the user.\n "
1416 GROUP(
"Vector" )));
1420 (
NAME(
"f_backend_multi" ),
1423 "As *f_backend* but describes an instrument with muliple\n"
1424 "mixer/reciever chains.\n"
1426 "This variable is needed when e.g. the reciever has several mixers\n"
1427 "or the the reciever measures several polarisation and the channels\n"
1428 "differ in position or response function. \n"
1430 "The array has one element for each \"reciever chain\". The array\n"
1431 "length must match *backend_channel_response_multi*, and possibly\n"
1432 "also *lo_multi*.\n"
1434 "Usage: Set by the user.\n "
1438 GROUP(
"ArrayOfVector" )));
1445 "The frequency grid for monochromatic pencil beam calculations.\n"
1447 "Usage: Set by the user.\n "
1451 GROUP(
"Vector" )));
1458 "Frequency index. \n"
1460 "Not all methods handle all monochromatic frequencies (of *f_grid*) in\n"
1461 "parellel and this variable is used for communication between methods,\n"
1462 "holding the index of the frequency treated presently.\n"
1464 "In some contexts, a negative f_index means all frequencies.\n"
1466 "Usage: Method output.\n"
1500 "Measurement block index. \n"
1502 "Used to tell agendas the index of present measurement block.\n"
1504 "Usage: Used internally.\n"
1513 "Monochromatic pencil beam radiance spectrum.\n"
1515 "This variable holds a single spectrum, with values corresponding\n"
1516 "to infinite frequency and spatial resolution (compare to *y*).\n"
1518 "The variable is used to represent spectra at all positions of the\n"
1519 "propagation path and can e.g. temporarily hold radiation entering\n"
1520 "the atmpophere from space. The unit depends on if emission is \n"
1521 "considered or not (no conversion to e.g. brightness temperature shall\n"
1524 "Usage: Used by radiative transfer methods.\n"
1526 "Unit: W / (m^2 Hz sr) or transmission.\n"
1528 "Dimensions: [ f_grid, stokes_dim ]\n"
1530 GROUP(
"Matrix" )));
1534 (
NAME(
"iy_agenda_call1" ),
1537 "Flag to handle recursive calls of *iy_clearsky_agenda*\n"
1539 "The agenda *iy_clearsky_agenda* can be used recursively and this flag\n"
1540 "is used to tell the methods inside the agenda which is the primary\n"
1541 " call. This is handled automatically for methods using\n"
1542 "*iy_clearsky_agenda*, such as *yCalc*, but the user must set this\n"
1543 "variable to 1 if the agenda is called directly inside the control\n"
1544 "file (which should be a rare case).\n"
1553 "Data auxilary to *iy*.\n"
1555 "This variable makes it possible to provide auxilary information for\n"
1556 "each value in *iy*. The standard usage is to provide transmission,\n"
1557 "then to complement radiance data. See the relevant WSMs for details.\n"
1559 "The data are not used for any calculations. The data are just passed\n"
1560 "on to create *y_aux*. A possibility here is to set *iy_aux* to e.g.\n"
1561 "-1000 inside *iy_cloudbox_agenda*, to obtain a way to catch\n"
1562 "interceptions with the cloudbox.\n"
1564 "Usage: Used by radiative transfer methods.\n"
1566 "Dimensions: [ f_grid, stokes_dim ]\n"
1568 GROUP(
"Matrix" )));
1572 (
NAME(
"iy_clearsky_agenda" ),
1577 GROUP(
"Agenda" )));
1581 (
NAME(
"iy_clearsky_basic_agenda" ),
1586 GROUP(
"Agenda" )));
1590 (
NAME(
"iy_cloudbox_agenda" ),
1595 GROUP(
"Agenda" )));
1599 (
NAME(
"iy_error" ),
1602 "Estimation of calculation errors in *iy*.\n"
1604 "As *y_error*, but treats *iy* and can be left empty if\n"
1605 "*iy_error_type* is 0.\n"
1607 "Usage: Used by radiative transfer methods.\n"
1609 "Unit: W / (m^2 Hz sr) or transmission.\n"
1611 "Dimensions: [ f_grid, stokes_dim ]\n"
1613 GROUP(
"Matrix" )));
1617 (
NAME(
"iy_error_type" ),
1620 "Characteristics of error values in *iy_error*.\n"
1622 "These options are defined:\n"
1623 " 0: The error is zero. *iy_error* can then be left undefined or\n"
1625 " 1: The error values are totally uncorrelated.\n"
1626 " 2: The error values are totally correlated.\n"
1627 "The distinction between case 1 and 2 is important, as the weighting\n"
1628 "with sensor response data must be performed differently for the two\n"
1635 (
NAME(
"iy_space_agenda" ),
1640 GROUP(
"Agenda" )));
1644 (
NAME(
"iy_transmission" ),
1647 "Transmission to be included in *iy*.\n"
1649 "The calculation of *iy* can be performed over several propation path\n"
1650 "branches, and there can be recursive calls of *iy_clearsky_agenda*.\n"
1651 "This variable gives the transmission from the end point of the present\n"
1652 "branch and the sensor for such recursive cases.\n"
1654 "This variable is used purely internally. The exact usage can vary\n"
1655 "between different RT integration schemes.\n"
1657 "Usage: Internally inside iy_clearsky_agenda.\n"
1661 "Dimensions: [ f_grid, stokes_dim, stokes_dim ]\n"
1663 GROUP(
"Tensor3" )));
1670 "Monochromatic pencil beam data for one measurement block.\n"
1672 "The data for all *iy* of a measurement block appended to a vector,\n"
1673 "following the sorting order used for *y*.\n"
1675 "Usage: Used internally.\n"
1677 "Unit: W / (m^2 Hz sr) or transmission.\n"
1679 "Dimensions: [ naa*nza*nf*stokes_dim ] where naa is length of\n"
1680 " mblock_aa_grid, za length of mblock_za_grid and nf is\n"
1681 " length of f_grid.\n"
1683 GROUP(
"Vector" )));
1687 (
NAME(
"jacobian" ),
1690 "The Jacobian matrix.\n"
1692 "The matrix holding the Jacobians of the retrieval quantities. Each\n"
1693 "quantity, and its subdivision into atmospheric grids, are stored as\n"
1694 "columns in the matrix. The matrix has to be initialised before the\n"
1695 "quantities can be defined. Initialisation WSM is *jacobianInit*.\n"
1696 "Retrieval quantities are then added with *jacobianAdd...* methods.\n"
1697 "See the online help. Pure numerical calculation is described by\n"
1698 "*jacobian_calc_agenda* and are performed by *jacobianCalc*.\n"
1700 "Units: See the different retrieval quantities.\n"
1702 "Dimension: [ y, number of retrieval quantities and grids ]\n"
1704 GROUP(
"Matrix" )));
1708 (
NAME(
"jacobian_do" ),
1711 "Flag to activate jacobian calculations.\n"
1713 "If this variable is set to 0, no jacobian calculations will be\n"
1714 "even if such calculations have been set-up (through the jacobianAddXxx\n"
1721 (
NAME(
"jacobian_agenda" ),
1726 GROUP(
"Agenda" )));
1730 (
NAME(
"jacobian_indices" ),
1733 "First and last column index in *jacobian* for each retrieval quantity."
1735 "This variable tells which part of *jacobian* that corresponds to \n"
1736 "each jacobian quantity.\n"
1738 "Usage: Set by *jacobianClose*.\n"
1740 GROUP(
"ArrayOfArrayOfIndex" )));
1755 (
NAME(
"jacobian_quantities" ),
1758 "The retrieval quantities in the Jacobian matrix.\n"
1760 "An array of retrieval quantities for which the jacobians are\n"
1763 "Usage: Quantities are added by the jacobianAdd WSMs.\n"
1765 GROUP(
"ArrayOfRetrievalQuantity" )));
1769 (
NAME(
"jacobian_y_agenda" ),
1774 GROUP(
"Agenda" )));
1778 (
NAME(
"lat_grid" ),
1781 "The latitude grid.\n"
1783 "The latitudes for which the atmospheric fields are defined. The\n"
1784 "atmosphere is undefined outside the range covered by the grid.\n"
1785 "The grid must be sorted in increasing order, with no repetitions.\n"
1787 "Geocentric latitudes shall be used.\n"
1789 "For 1D calculations this vector can is some cases be set to be empty.\n"
1790 "Some methods are requiring a latitude even for 1D and the latitude\n"
1791 "is then taken from this vector. That is, for 1D the length can either\n"
1794 "For 2D cases the latitudes shall be interpreted as the angular\n"
1795 "distance inside the orbit plane from an arbitrary zero point (values\n"
1796 "outside +-90 deg are allowed).\n"
1798 "For 3D, the valid latitude range is [-90,90].\n"
1800 "See further the ARTS user guide (AUG). Use the index to find where\n"
1801 "this variable is discussed. The variable is listed as a subentry to\n"
1802 "\"workspace variables\".\n"
1804 "Usage: Set by the user.\n"
1808 GROUP(
"Vector" )));
1816 "The local oscillator frequency.\n"
1818 "A local oscillator frequency is used in a heterodyne system when\n"
1819 "the mixer folds the spectra from from radio frequencies (RF) to\n"
1820 "intermediate frequencies (IF).\n"
1824 "Usage: Set by the user.\n"
1826 GROUP(
"Numeric" )));
1830 (
NAME(
"lo_multi" ),
1833 "Local oscillator frequencies.\n"
1835 "As *lo* but describes an instrument with multiple mixers. A vector\n"
1836 "element for each LO. The size of this variable and\n"
1837 "*sideband_response_multi* shall match, and probably also\n"
1838 "*sideband_mode_multi*.\n"
1842 "Usage: Set by the user.\n"
1844 GROUP(
"Vector" )));
1848 (
NAME(
"lon_grid" ),
1851 "The longitude grid.\n"
1853 "The longitudes for which the atmospheric fields are defined. The\n"
1854 "atmosphere is undefined outside the range covered by the grid.\n"
1855 "The grid must be sorted in increasing order, with no repetitions.\n"
1857 "For 1D and 2D, some methods could expect this vector to have\n"
1858 "length 1, and holding a longitude representing the case. Otherwise\n"
1859 "the length can be 0. That is, works as *lat_grid* for 1D.\n"
1861 "Allowed values for longitudes is the range [-360,360].\n"
1863 "See further the ARTS user guide (AUG). Use the index to find where\n"
1864 "this variable is discussed. The variable is listed as a subentry to\n"
1865 "\"workspace variables\".\n"
1867 "Usage: Set by the user.\n"
1871 GROUP(
"Vector" )));
1875 (
NAME(
"main_agenda" ),
1880 GROUP(
"Agenda" )));
1884 (
NAME(
"massdensity_field" ),
1887 "The field of atmospheric scattering particle types in unit of massdensity\n"
1888 "(like IWC/LWC/Rain/Aerosol etc.).\n"
1890 "If *massdensity_field* is obtained from Chevallier91L data, the scat. particles are\n"
1891 "hydrometeors of type: CLW[kg/m^3] CIW[kg/m^3] Rain[kg/(m2*s)] Snow[kg/(m2*s)]\n"
1893 "NOTE: naming discussion: *massdensity_field* should be renamed in the future\n"
1894 "to a more general term (not limited to massdensities).\n"
1896 "Possible future extension: In the future a *massdensity_field_raw* might be needed,\n"
1897 "which contains the not-interpolated mass concentrations of scattering particles.\n"
1898 "This is not needed in the moment, since *massdensity_field* is only used with \n"
1899 "batch profile data (where all atmospheric variables are on the same grid).\n"
1901 "Usage:\tmassdensity data is used to calculate pnd_fields\n"
1903 "Unit:\tdepending on what is read, usually [kg/m3]\n"
1905 "Dimension:\t[ type, p_grid, lat_grid, lon_grid ]\n"
1908 GROUP(
"Tensor4" )));
1926 (
NAME(
"mblock_aa_grid" ),
1929 "The azimuthal angle grid for each measurement block.\n"
1931 "This variable should normally contain the azimuth grid of the\n"
1932 "antenna pattern. The grid is given as an angular off-set with\n"
1933 "respect to the angles in *sensor_los*.\n"
1935 "See further the ARTS user guide (AUG). Use the index to find where\n"
1936 "this variable is discussed. The variable is listed as a subentry to\n"
1937 "\"workspace variables\".\n"
1939 "Usage: Set by the user.\n"
1943 GROUP(
"Vector" )));
1947 (
NAME(
"mblock_za_grid" ),
1950 "The zenith angle grid for each measurement block.\n"
1952 "This variable should normally contain the zenith grid of the\n"
1953 "antenna pattern. The grid is given as an angular off-set with\n"
1954 "respect to the angles in *sensor_los*.\n"
1956 "See further the ARTS user guide (AUG). Use the index to find where\n"
1957 "this variable is discussed. The variable is listed as a subentry to\n"
1958 "\"workspace variables\".\n"
1960 "Usage: Set by the user.\n"
1964 GROUP(
"Vector" )));
1968 (
NAME(
"mc_antenna" ),
1971 "Antenna pattern description for dedicated MC calculaions.\n"
1973 "Usage: Input to MCGeneral. Set by *mc_antennaSetGaussian* and similar\n"
1976 GROUP(
"MCAntenna" )));
1980 (
NAME(
"mc_cloud_opt_path" ),
1983 "The cloud optical path integrated over the field of view.\n"
1985 "Usage: Output from mc_IWP_cloud_opt_pathCalc \n"
1987 GROUP(
"Numeric" )));
1991 (
NAME(
"mc_cloud_opt_path_error" ),
1994 "Standad error in the cloud optical path integrated over the field\n"
1997 "Usage: Output from mc_IWP_cloud_opt_pathCalc \n"
1999 GROUP(
"Numeric" )));
2003 (
NAME(
"mc_error" ),
2006 "Error in simulated *y* when using a Monte Carlo approach.\n"
2008 "Usage: Output from Monte Carlo functions. \n"
2010 "Units: Depends on *y_unit*.\n"
2012 "Size: [ stokes_dim ]\n"
2014 GROUP(
"Vector" )));
2018 (
NAME(
"mc_iteration_count" ),
2021 "Counts the number of iterations (or photons) used in the MC\n "
2022 "scattering algorithm.\n"
2024 "Usage: Set by MCGeneral and other MC methods.\n"
2033 "The ice water path integrated over the field of view\n"
2035 "Usage: Output from mc_IWP_cloud_opt_pathCalc \n"
2037 GROUP(
"Numeric" )));
2041 (
NAME(
"mc_IWP_error" ),
2044 "The standard error of ice water path integrated over the field of view\n"
2046 "Usage: Output from mc_IWP_cloud_opt_pathCalc \n"
2048 GROUP(
"Numeric" )));
2052 (
NAME(
"mc_points" ),
2055 "Counts the number of MC endpoints in each grid cell.\n"
2057 "Usage: Set by MCGeneral and other MC methods.\n"
2059 GROUP(
"Tensor3" )));
2063 (
NAME(
"mc_seed" ),
2066 "The integer seed for the random number generator used by\n"
2067 "Monte Carlo methods.\n"
2069 "Usage: Set by MCSetSeed.\n"
2075 (
NAME(
"mc_std_err" ),
2078 "Target precision (1 std. dev.) for Monte Carlo calculations.\n"
2080 "Usage: Set by the user.\n"
2082 GROUP(
"Numeric" )));
2086 (
NAME(
"mc_max_time" ),
2089 "The maximum time allowed for Monte Carlo calculations.\n"
2091 "Usage: Set by the user.\n"
2099 (
NAME(
"mc_max_iter" ),
2102 "The maximum number of iterations allowed for Monte Carlo\n"
2105 "Usage: Set by the user.\n"
2111 (
NAME(
"mc_z_field_is_1D" ),
2114 "Flag for MCGeneral and associated methods.\n"
2116 "If fields outside the cloud box are 1D, this flag can be set to 1\n"
2117 "and the calculations will be more rapid.\n"
2119 "Usage: Set by the user.\n"
2125 (
NAME(
"met_amsu_data" ),
2128 "The AMSU data set.\n"
2130 "This is intended as input for the method ybatchMetProfiles. It holds the\n"
2131 "latitude, longitude, satellite zenith angle and amsu-b corrected and \n"
2132 "uncorrected brightness temperatures. It also has information about \n"
2133 "the particular pixel corresponds to a land or sea point. This will be \n"
2134 "read in the method ybatchMetProfiles and the profiles corresponding to \n"
2135 "each latitude and longitude will be read in.\n"
2137 "See documentation of WSM *ybatchMetProfiles* for more information.\n"
2139 GROUP(
"Matrix" )));
2146 "This variable is used by the VectorSet workspace method.\n"
2155 "This variable is used by the MatrixSet, Tensor3Set, etc. \n"
2156 "workspace methods.\n"
2189 (
NAME(
"nshelves" ),
2198 (
NAME(
"nvitrines" ),
2207 (
NAME(
"nlibraries" ),
2216 (
NAME(
"met_profile_calc_agenda" ),
2221 GROUP(
"Agenda" )));
2225 (
NAME(
"opt_prop_gas_agenda" ),
2230 GROUP(
"Agenda" )));
2234 (
NAME(
"opt_prop_part_agenda" ),
2239 GROUP(
"Agenda" )));
2243 (
NAME(
"output_file_format" ),
2246 "Output file format. \n"
2248 "This variable sets the format for output files. It could be set to\n"
2249 "\"ascii\" for plain xml files, \"zascii\" for zipped xml files, or\n"
2252 "To change the value of this variable use the workspace methods\n"
2253 "*output_file_formatSetAscii*, *output_file_formatSetZippedAscii*, and\n"
2254 "*output_file_formatSetBinary*\n"
2256 GROUP(
"String" )));
2260 (
NAME(
"particle_masses" ),
2263 "The mass of each particle type stored in a vector \n"
2265 "Usage: Set by the user.\n"
2267 GROUP(
"Vector" )));
2271 (
NAME(
"part_species" ),
2274 "*part_species* is an Array of Strings containing user defined input,\n"
2275 "for particle number density calculations performed by *pnd_fieldSetup*.\n"
2277 "Each single String must contain:\n"
2278 "scattering particle type [*String*]:\t e.g. 'LWC', 'IWC', 'Rain'\n"
2279 "particle size distribution [*String*]:\t e.g. 'MH97', 'liquid', 'H11'\n"
2280 "sizerange-start [*Numeric*]:\tthe first particle radius(liquid)/melted radius(ice)\n"
2281 " \tthe calculations shall start with.\n"
2282 "sizerange-end [*Numeric*]:\tthe last particle radius(liquid)/melted radius(ice)\n"
2283 " \tthe calculations shall end with.\n"
2285 "NOTE: the sizerange inputs must be given in MICRONS!\n"
2287 "The Array needs to looks like this: [''IWC-MH97-2-1000'', ''LWC-liquid-0.1-10'', ...]\n"
2289 GROUP(
"ArrayOfString" )));
2293 (
NAME(
"pha_mat" ),
2296 "Ensemble averaged phase matrix.\n"
2298 "This workspace variable represents the actual physical phase\n"
2299 "matrix (averaged over all particle types) for given propagation\n"
2300 "directions. It is calculated in the method *pha_matCalc*\n"
2302 "ARTS user guide (AUG) gives the formula used for computing this\n"
2303 "variable. Use the index to find where this variable is discussed.\n"
2304 "The variable is listed as a subentry to \"workspace variables\".\n"
2306 "Usage: Output of the method *pha_matCalc*\n"
2310 "Dimensions: [ scat_za_grid, scat_aa_grid, stokes_dim, stokes_dim ]\n"
2312 GROUP(
"Tensor4" )));
2316 (
NAME(
"pha_mat_spt" ),
2319 "Phase matrix for a single particle type.\n"
2321 "This variable contains the elements of phase matrix for a single \n"
2322 "particle for given propagation direction. \n"
2323 "It is the calculated in the agenda *pha_mat_spt_agenda*. \n"
2324 "The elements of the phase matrix are calculated from \n"
2325 "the single scattering data. "
2326 "ARTS user guide (AUG) gives the formulas used for computing all \n"
2327 "elements of the phase matrix for a given particle type.\n"
2336 "Dimensions: [part_types, *scat_za_grid*, *scat_aa_grid*, *stokes_dim*, *stokes_dim*]\n"
2338 GROUP(
"Tensor5" )));
2342 (
NAME(
"pha_mat_spt_agenda" ),
2347 GROUP(
"Agenda" )));
2351 (
NAME(
"pha_mat_sptDOITOpt" ),
2354 "Interpolated phase matrix.\n"
2356 "This variable contains the data of the phase matrix in the \n"
2357 "scattering frame interpolated on the actual frequency (the variable\n"
2358 "is used inside *doit_mono_agenda*) and also interpolated on all \n"
2359 "possible scattering angles following from all combinations of \n"
2360 "*scat_za_grid* and *scat_aa_grid*. \n"
2362 "Usage: Input of the method *pha_mat_sptFromDataDOITOpt*\n"
2367 "[particle types]\n"
2368 "[T, scat_za_grid,scat_aa_grid, scat_za_grid, scat_aa_grid,\n"
2369 "stokes_dim, stokes_dim]\n"
2371 GROUP(
"ArrayOfTensor7" )));
2375 (
NAME(
"pnd_field" ),
2378 "Particle number density field.\n"
2380 "This veriable corresponds to the particle number density fields \n"
2381 "for all particle types being read in the WSMs *ParticleTypeAdd* \n"
2382 "or *ParticleTypeAddAll*. \n"
2383 "Another alternative is to create *pnd_field* with *pnd_fieldSetup*.\n"
2385 "Usage: Calculated internally.\n"
2389 "Size: [N_part_types, \n"
2390 " (cloudbox_limits[1] - cloudbox_limits[0]) +1, \n"
2391 " (cloudbox_limits[3] - cloudbox_limits[2]) +1, \n"
2392 " (cloudbox_limits[5] - cloudbox_limits[4]) +1 ] \n"
2394 GROUP(
"Tensor4" )));
2425 (
NAME(
"pnd_field_raw" ),
2428 "The particle number density field data.\n"
2430 "This variable contains the particle number density data for all \n"
2431 "chosen particle types. It includes the grids corresponding to the \n"
2432 "grids in the database. \n"
2433 "*pnd_field_raw* is an Array of GriddedField3. It includes a\n"
2434 "GriddedField3 for each particle type which contains the data and \n"
2437 "Usage: Used in the methods *ParticleTypeAdd* and \n"
2438 " *ParticleTypeAddAll*\n"
2442 "Size: Array[N_pt]\n"
2443 " GriddedField3 \n "
2447 " [N_p, N_lat, N_lon] \n"
2449 GROUP(
"ArrayOfGriddedField3" )));
2456 "The propagation path for one line-of-sight.\n"
2458 "This variable describes the total (pencil beam) propagation path for\n"
2459 "a given combination of starting point and line-of-sight. The path is\n"
2460 "described by a data structure of type Ppath. This structure contains\n"
2461 "also additional fields to faciliate the calculation of spectra and\n"
2462 "interpolation of the atmospheric fields.\n"
2464 "The data struture is too extensive to be described here, but it is\n"
2465 "described carefully in the ARTS user guide (AUG). Use the index to\n"
2466 "find where the data structure, Ppath, for propagation paths is \n"
2467 "discussed. It is listed as a subentry to \"data structures\".\n"
2469 "Usage: Output from the method *ppathCalc*.\n"
2475 (
NAME(
"ppath_lmax" ),
2478 "Maximum length between points describing propagation paths.\n"
2480 "See *ppath_stepGeometric* for a description of this variable.\n"
2482 "Usage: Ppath methods such as *ppath_stepGeometric*.\n"
2484 GROUP(
"Numeric" )));
2488 (
NAME(
"ppath_lraytrace" ),
2491 "Maximum length of ray tracing steps when determining propagation\n"
2494 "See *ppath_stepRefractionEuler* for a description of this variable.\n"
2496 "Usage: Refraction ppath methods such as *ppath_stepRefractionEuler*.\n"
2498 GROUP(
"Numeric" )));
2502 (
NAME(
"ppath_step" ),
2505 "A propagation path step.\n"
2507 "The main intention of this variable is communication with the agenda\n"
2508 "*ppath_step_agenda*.\n"
2510 "See *ppathCalc* for more information on this variable and\n"
2511 "the calculation of propagation paths. Or read the chapter on\n"
2512 "propagation paths in the ARTS user guide.\n"
2514 "Usage: In/output to/from *ppath_step_agenda*.\n"
2516 "Members: See AUG.\n"
2522 (
NAME(
"ppath_step_agenda" ),
2527 GROUP(
"Agenda" )));
2534 "The pressure grid.\n"
2536 "The pressure levels on which the atmospheric fields are defined.\n"
2537 "This variable must always be defined. The grid must be sorted in\n"
2538 "decreasing order, with no repetitions.\n"
2540 "No gap between the lowermost pressure level and the surface is \n"
2541 "allowed. The uppermost pressure level defines the practical upper\n"
2542 "limit of the atmosphere as vacuum is assumed above.\n"
2544 "See further the ARTS user guide (AUG). Use the index to find where\n"
2545 "this variable is discussed. The variable is listed as a subentry to\n"
2546 "\"workspace variables\".\n"
2548 "Usage: Set by the user.\n"
2552 GROUP(
"Vector" )));
2559 "Reference pressure calculation of hydrostatic equilibrium.\n"
2561 "The altitude specified by this pressure is used as the reference\n"
2562 "when calculating hydrostatic equilibrium. That is, the geometrical\n"
2563 "altitude at this pressure is not changed.\n"
2565 "Usage: Set by the user.\n"
2569 GROUP(
"Numeric" )));
2573 (
NAME(
"refr_index" ),
2576 "Refractive index of air (only real part).\n"
2578 "This variable contains the refractive index summed over all relevant\n"
2579 "constituents, at one position in the atmosphere. The standard set of\n"
2580 "functions assumes that all frequency components propagate along the\n"
2581 "same path. That is, dispersion is neglected and this variable has no\n"
2582 "frequency dimension.\n"
2586 GROUP(
"Numeric" )));
2590 (
NAME(
"refr_index_agenda" ),
2595 GROUP(
"Agenda" )));
2599 (
NAME(
"rte_doppler" ),
2602 "A doppler shift for radiative transfer calculations.\n"
2604 "This scalar variable can hold the local doppler shift. It is intended\n"
2605 "mainly for communication with various methods and agendas, such as\n"
2606 "methods and agendas calculating absorption coefficients.\n"
2608 "Positive values mean that the spectrum is shifted towards higher\n"
2611 "Usage: Communication variable.\n"
2615 GROUP(
"Numeric" )));
2619 (
NAME(
"rte_do_vmr_jacs" ),
2622 "Index of gas species for which *rte_agenda* shall calculate "
2623 "VMR jacobians (with respect to changes along the propagation path).\n"
2625 "These indexes refer to the position in *abs_species*.\n"
2627 "Usage: Set internally, by *RteCalc*.\n"
2629 GROUP(
"ArrayOfIndex" )));
2633 (
NAME(
"rte_do_t_jacs" ),
2636 "Flag to *rte_agenda* to calculate jacobians for temperature.\n"
2638 "Usage: Set internally, by *RteCalc*.\n"
2644 (
NAME(
"rte_gp_p" ),
2647 "The pressure grid position of *rte_pos*.\n"
2649 "This variable is used to give the grid position for an end point\n"
2650 "of the propagation path to some workspace method part of the\n"
2651 "radiative transfer calculations.\n"
2653 "Usage: Set internally.\n"
2655 GROUP(
"GridPos" )));
2659 (
NAME(
"rte_gp_lat" ),
2662 "The latitude grid position of *rte_pos*.\n"
2664 "This variable is used to give the grid position for an end point\n"
2665 "of the propagation path to some workspace method part of the\n"
2666 "radiative transfer calculations.\n"
2668 "Usage: Set internally.\n"
2670 GROUP(
"GridPos" )));
2674 (
NAME(
"rte_gp_lon" ),
2677 "The longitude grid position of *rte_pos*.\n"
2679 "This variable is used to give the grid position for an end point\n"
2680 "of the propagation path to some workspace method part of the\n"
2681 "radiative transfer calculations.\n"
2683 "Usage: Set internally.\n"
2685 GROUP(
"GridPos" )));
2689 (
NAME(
"rte_los" ),
2692 "A line-of-sight for radiative transfer calculations.\n"
2694 "The main purpose of this WSV and *rte_pos* is communication with \n"
2695 "different agendas involved in the RTE calculations. These variables \n"
2696 "can also be used to enable calling of *ppathCalc* (and maybe other \n"
2697 "methods) from the workspace. \n"
2699 "For 1D and 2D cases, *rte_los* is a vector of length 1 holding the \n"
2700 "zenith angle. For 3D, the length of the vector is 2, where the\n"
2701 "additional element is the azimuthal angle. These angles are defined\n"
2702 "in the ARTS user guide (AUG). Look in the index for \"zenith angle\"\n"
2703 "and \"azimuthal angle\".\n"
2705 "Usage: See above.\n"
2707 "Units: [ degree, degree ]\n"
2709 "Size: [ 1 or 2 ]\n"
2711 GROUP(
"Vector" )));
2715 (
NAME(
"rte_pos" ),
2718 "A geographical position for radiative transfer calculations.\n"
2720 "The main purpose of this WSV and *rte_los* is communication with \n"
2721 "different agendas involved in the RTE calculations. These variables \n"
2722 "can also be used to enable calling of *ppathCalc* (and maybe other \n"
2723 "methods) from the workspace. \n"
2725 "This variable is a vector with a length equalling the atmospheric\n"
2726 "dimensionality. The first element is the radius (from the coordinate\n"
2727 "system centre) of the position. Element 2 is the latitude and \n"
2728 "element 3 is the longitude. Please note that the vertical position \n"
2729 "is given as the radius, not the altitude above the geoid.\n"
2731 "Usage: See above. \n"
2733 "Units: [ m, degree, degree ]\n"
2735 "Size: [ atmosphere_dim ]\n"
2737 GROUP(
"Vector" )));
2741 (
NAME(
"rte_pressure" ),
2744 "A pressure for radiative transfer calculations.\n"
2746 "This scalar variable can hold the local pressure. It is intended\n"
2747 "mainly for communication with various methods and agendas, such as\n"
2748 "methods and agendas calculating absorption coefficients.\n"
2750 "Usage: Communication variable.\n"
2754 GROUP(
"Numeric" )));
2758 (
NAME(
"rte_temperature" ),
2761 "A temperature for radiative transfer calculations.\n"
2763 "This scalar variable can hold the local temperature. It is intended\n"
2764 "mainly for communication with various methods and agendas, such as\n"
2765 "methods and agendas calculating absorption coefficients.\n"
2767 "Usage: Communication variable.\n"
2771 GROUP(
"Numeric" )));
2775 (
NAME(
"rte_vmr_list" ),
2778 "A list of VMR values for radiative transfer calculations.\n"
2780 "This vector variable holds the local VMR value for all used species\n"
2781 "(as given by *abs_species*). It is intended mainly for communication\n"
2782 "with various methods and agendas, such as methods and agendas \n"
2783 "calculating absorption coefficients.\n"
2785 "Usage: Communication variable.\n"
2787 "Units: [ Absolute value ]\n"
2789 "Size: Should match abs_species.nelem()\n"
2791 GROUP(
"Vector" )));
2795 (
NAME(
"r_geoid" ),
2800 "Geometrical altitudes are defined as the vertical distance above the\n"
2801 "geoid, and the geoid is the reference surface used when giving, for\n"
2802 "example, *z_surface* and *z_field*. \n"
2804 "The geoid is defined by giving the radius from the coordinate centre\n"
2805 "to the geoid surface for each crossing of the latitude and longitude\n"
2806 "grids. The geoid should normally be selected to be an ellipsoid but\n"
2807 "any shape is allowed. For 1D calculations, the geoid is by\n"
2808 "definition a sphere.\n"
2810 "The radius for a point between the grid crossings is obtained by\n"
2811 "linear (2D) or bi-linear (3D) interpolation of the *r_geoid*. For 1D\n"
2812 "cases the geoid radius is constant.\n"
2814 "See further the ARTS user guide (AUG). Use the index to find where\n"
2815 "this variable is discussed. The variable is listed as a subentry to\n"
2816 "\"workspace variables\".\n"
2818 "Usage: Set by using a method for a geodetic datum.\n"
2822 "Dimensions: [ lat_grid, lon_grid ]\n"
2824 GROUP(
"Matrix" )));
2828 (
NAME(
"scat_aa_grid" ),
2831 "Azimuthal angle grid.\n"
2833 "The azimutal angle grid, on which the intensity field is stored. \n"
2834 "This grid is used for RT calculations inside the cloudbox, \n"
2835 "therefore one has to define it if the cloudbox is activated by \n"
2836 "the flag *cloudbox_on*.\n"
2837 "The grid must be sorted in increasing order, with no repetitions.\n"
2839 "Usage: Set by the user.\n"
2843 GROUP(
"Vector" )));
2847 (
NAME(
"scat_aa_index" ),
2850 "Azimuth angle index for scattering calculations.\n"
2852 "This variable is used in methods used for computing scattering\n"
2854 "It holds the information about the azimuth angles for which the \n"
2855 "scattering calculations are done. The angles used for computing \n"
2856 "scattering properties of particles can be different from that used \n"
2857 "for radiative transfer calculation. \n"
2859 "Usage: Method output.\n"
2865 (
NAME(
"scat_data_meta" ),
2868 "Structure for the scattering meta data.\n"
2870 "This variable holds the scattering meta data for a single particle.\n"
2871 "This data is needed for particle size distribution calculations.\n"
2873 "Currently some of the meta data entries are not used by ARTS,\n"
2874 "but were included for future extensions of pnd calculations in ARTS.\n"
2875 "This applies to: \"shape\", \"A_proje\", \"asratio\"\n"
2877 "Usage: Set by the user.\n"
2879 "Dimensions/Units:\n"
2880 "\tString[description]\t[particle description]\n"
2881 "\tString[type]\t\t[''Ice'', ''Water''...]\n"
2882 "\tString[shape]\t\t[''Droxtal'', ''Aggregate'', ''Spherical'', ...]\n"
2883 "\tNumeric[density]\t[kg/m3]\n"
2884 "\tNumeric[d_max]\t\t[m]\n"
2885 "\tNumeric[V]\t\t[m3]\n"
2886 "\tNumeric[A_proje]\t[m2]\n"
2887 "\tNumeric[asratio]\t[]\n"
2889 GROUP(
"ScatteringMetaData" )));
2893 (
NAME(
"scat_data_meta_array" ),
2896 "An Array of ScatteringMetaData.\n"
2898 "The elements of the array hold the scattering meta data for a single particle.\n"
2899 "This data is needed for particle size distribution calculations, with *pnd_fieldSetup*.\n"
2901 "Currently some of the meta data entries are not used by ARTS, but were included for \n"
2902 "future extensions of pnd calculations in ARTS.\n"
2903 "This applies to: \"shape\", \"A_proje\", \"asratio\"\n"
2905 "Note: This array must contain as many elements as *scat_data_raw*\n"
2907 "Usage: Set by the user.\n"
2909 "Dimensions/Units: Array[particle types]\n"
2910 "\tString[description]\t[particle description]\n"
2911 "\tString[type]\t\t[''Ice'', ''Water''...]\n"
2912 "\tString[shape]\t\t[''Droxtal'', ''Aggregate'', ''Spherical'', ...]\n"
2913 "\tNumeric[density]\t[kg/m3]\n"
2914 "\tNumeric[d_max]\t\t[m]\n"
2915 "\tNumeric[V]\t\t[m3]\n"
2916 "\tNumeric[A_proje]\t[m2]\n"
2917 "\tNumeric[asratio]\t[]\n"
2919 GROUP(
"ArrayOfScatteringMetaData" )));
2924 (
NAME(
"scat_data_mono" ),
2927 "Monochromatic single scattering data.\n"
2929 "This variable holds the single scattering properties for all \n"
2930 "hydrometeor species. It is calculated from *scat_data_raw* by \n"
2931 "*scat_data_monoCalc*, which interpolates *scat_data_raw* for the \n"
2932 "required frequency.\n"
2934 GROUP(
"ArrayOfSingleScatteringData" )));
2938 (
NAME(
"scat_data_nelem" ),
2941 "This Array has the same size as *part_species*. \n"
2943 "Each element holds the number of scattering data files, associated\n"
2944 "with the criteria given by *part_species*.\n"
2946 "Usage: WSM *ScatteringParticlesSelect* creates *scat_data_nelem*.\n"
2948 GROUP(
"ArrayOfIndex" )));
2952 (
NAME(
"scat_data_raw" ),
2955 "Raw data of single scattering data.\n"
2957 "This variable holds the single scattering properties for all \n"
2958 "hydrometeor species included in a calculation by using the \n"
2959 "methods *ParticleTypeAdd* or *ParticleTypeAddAll*. \n"
2960 "For more information refer to ArtsWiki.\n"
2962 "Option: See also *ScatteringParticleTypeAndMetaRead* for reading \n"
2963 "*SingleScatteringData* and *ScatteringMetaData*.\n"
2965 "The unit of the single scattering properties is m^2.\n"
2967 "This may be used in combination with *scat_data_meta_array*\n"
2969 "Usage: Method ouput.\n"
2971 "Dimensions: Array[particle types] \n"
2972 " SingleScatteringData \n"
2973 " Enum[particle type attribute]\n"
2974 " String[description] \n"
2977 " Vector[za_grid]\n"
2978 " Vector[aa_grid]\n"
2979 " Tensor7[pha_mat_data]\n"
2980 " [f_grid, T_grid, za_grid, aa_grid, za_grid, aa_grid, matrix_element]\n"
2981 " ^^^^^^^^^^^^^^^^ ^^^^^^^^^^^^^^^^\n"
2982 " scattered incoming\n"
2983 " Tensor5[ext_mat_data]\n"
2984 " [f_grid, T_grid, za_grid, aa_grid, matrix_element]\n"
2985 " Tensor5[abs_vec_data]\n"
2986 " [f_grid, T_grid, za_grid, aa_grid, matrix_element]\n"
2988 GROUP(
"ArrayOfSingleScatteringData" )));
2992 (
NAME(
"scat_i_lat" ),
2995 "Intensity field on cloudbox boundary (constant latitude slice).\n"
2997 "This variable gives the intensity field from all directions defined \n"
2998 "in *scat_aa_grid* and *scat_za_grid* on each grid point on the two \n"
3000 "latitude levels of the cloudbox boundary. It contains all four \n"
3001 "components of the Stokes vector.\n"
3003 "This variable is used as interface between the clear sky and the \n"
3004 "scattering calculations. \n"
3006 "See further the ARTS user guide (AUG). Use the index to find where\n"
3007 "this variable is discussed. The variable is listed as a subentry to\n"
3008 "\"workspace variables\".\n"
3010 "Usage: In/Output from/to *ScatteringDoit* and *ScatteringDisort*\n"
3012 "Unit: W / (m^2 Hz sr) \n"
3014 "Dimensions: [ f_grid, p_grid, 2, lon_grid, \n"
3015 " scat_za_grid \n scat_aa_grid, stokes_dim ]\n"
3017 GROUP(
"Tensor7" )));
3021 (
NAME(
"scat_i_lon" ),
3024 "Intensity field on cloudbox boundary (equal longitude slice).\n"
3026 "This variable gives the intensity field from all directions defined \n"
3027 "in *scat_aa_grid* and *scat_za_grid* on each grid point on the equal\n"
3028 "longitude level of the boundary of the cloudbox, which is defined \n"
3029 "by the workspace variable *cloudbox_limits*. It contains all four \n"
3030 "components of the Stokes vector.\n"
3032 "This variable is used as interface between the clear sky and the \n"
3033 "scattering calculations. \n"
3035 "See further the ARTS user guide (AUG). Use the index to find where\n"
3036 "this variable is discussed. The variable is listed as a subentry to\n"
3037 "\"workspace variables\".\n"
3039 "Usage: Output from *ScatteringDoit* and *ScatteringDisort* \n"
3041 "Unit: W / (m^2 Hz sr) \n"
3043 "Dimensions: [ f_grid, p_grid, lat_grid, 2, \n"
3044 " scat_za_grid, scat_aa_grid, stokes_dim]\n"
3046 GROUP(
"Tensor7" )));
3050 (
NAME(
"scat_i_p" ),
3053 "Intensity field on cloudbox boundary (equal pressure slice).\n"
3055 "This variable gives the intensity field from all directions defined \n"
3056 "in *scat_aa_grid* and *scat_za_grid* on each grid point on the equal\n"
3057 "pressure levels of the cloudbox boundary. It contains all four \n"
3058 "components of the Stokes vector.\n"
3060 "This variable is used as interface between the clear sky and the \n"
3061 "scattering calculations. \n"
3063 "See further the ARTS user guide (AUG). Use the index to find where\n"
3064 "this variable is discussed. The variable is listed as a subentry to\n"
3065 "\"workspace variables\".\n"
3067 "Usage: In/Output from *ScatteringDoit* and *ScatteringDisort* \n"
3069 "Unit: W / (m^2 Hz sr) \n"
3071 "Dimensions: [ f_grid, 2, lat_grid, lon_grid, \n"
3072 " scat_za_grid, scat_aa_grid, stokes_dim]\n"
3074 GROUP(
"Tensor7" )));
3078 (
NAME(
"scat_lat_index" ),
3081 "Latitude index for scattering calculations.\n"
3083 "This variable is used in methods used for computing scattering\n"
3084 "properties of particles like *opt_prop_sptFromData* and *pha_matCalc*.\n"
3085 "It holds the information about the position for which the \n"
3086 "scattering calculations are done. \n"
3088 "Usage: Input to the methods *spt_calc_agenda*,\n"
3089 " *pha_mat_spt_agenda*\n"
3095 (
NAME(
"scat_lon_index" ),
3098 "Longitude index for scattering calculations.\n"
3100 "This variable is used in methods used for computing scattering\n"
3101 "properties of particles like *opt_prop_sptFromData* and *pha_matCalc*.\n"
3102 "It holds the information about the position for which the \n"
3103 "scattering calculations are done. \n"
3105 "Usage: Input to the methods *spt_calc_agenda*,\n"
3106 " *pha_mat_spt_agenda*\n"
3112 (
NAME(
"scat_p_index" ),
3115 "Pressure index for scattering calculations.\n"
3117 "This variable is used in methods used for computing scattering\n"
3118 "properties of particles like *opt_prop_sptFromData* and *pha_matCalc*.\n"
3119 "It holds the information about the location for which the \n"
3120 "scattering calculations are done.\n"
3122 "Usage: Input to the methods *spt_calc_agenda*,\n"
3123 " *pha_mat_spt_agenda*\n"
3129 (
NAME(
"scat_za_grid" ),
3132 "Zenith angle grid.\n"
3134 "The zenith angle grid, on which the intensity field is stored. \n"
3135 "This grid is used for RT calculations inside the cloudbox, therefore\n"
3136 "the grid has to be defined\n"
3137 "if the cloudbox is activated by the flag *cloudbox_on*.\n"
3138 "The grid must be sorted in increasing order, with no repetitions.\n"
3140 "Usage: Set by the user.\n"
3144 GROUP(
"Vector" )));
3148 (
NAME(
"scat_za_index" ),
3151 "Zenith angle index for scattering calculations.\n"
3153 "This variable is used internally in WSMs for computing scattering \n"
3156 "Usage: Input to the agendas *spt_calc_agenda*, \n "
3157 " *pha_mat_spt_agenda*.\n"
3163 (
NAME(
"sensor_description_amsu" ),
3166 "Sensor description for simple AMSU setup.\n"
3168 "This is a compact description of an AMSU-type sensor. The matrix\n"
3169 "contains one row for each instrument channel. Each row contains three\n"
3170 "elements: LO position [Hz], offset of the channel center from the LO\n"
3171 "[Hz], and channel width [Hz].\n"
3173 "Usage: Set by the user.\n"
3175 "Unit: All entries in Hz.\n"
3177 "Size: [number of channels, 3]\n"
3179 GROUP(
"Matrix" )));
3183 (
NAME(
"sensor_los" ),
3186 "The sensor line-of-sight (LOS) for each measurement block.\n"
3188 "Line-of-sights are specified by giving the zenith and azimuth angles.\n"
3189 "Column 1 holds the zenith angle. This angle is simply the angle \n"
3190 "between the zenith and LOS directions. For 1D and 3D the valid\n"
3191 "range is [0 180], while for 2D angles down to -180 degrees are\n"
3192 "allowed. Negative angles signifies for 2D observations towards\n"
3193 "lower latitudes, while positive angles means observations towards\n"
3194 "higher latitudes. Nadir corresponds throughout to 180 degrees.\n"
3196 "The azimuth angle is given with respect to the meridian plane. That\n"
3197 "is, the plane going through the north and south poles. The valid \n"
3198 "range is [-180,180] where angles are counted clockwise; 0 means\n"
3199 "that the viewing or propagation direction is north-wise and +90 means\n"
3200 "that the direction of concern goes eastward.\n"
3202 "See further the ARTS user guide (AUG). Use the index to find where\n"
3203 "this variable is discussed. The variable is listed as a subentry to\n"
3204 "\"workspace variables\".\n"
3206 "Usage: Set by the user.\n"
3208 "Unit: [ degrees, degrees ]\n"
3210 "Size: [ number of measurement blocks, 1 or 2 ]\n"
3212 GROUP(
"Matrix" )));
3216 (
NAME(
"sensor_norm" ),
3219 "Flag if sensor response should be normalised or not (0 or 1).\n"
3221 "If the flag is set to 1 each sensor response is normalised (where\n"
3222 "applicable). If set to 0 the sensor responses are left as provided.\n"
3224 "See further the ARTS user guide (AUG). Use the index to find where\n"
3225 "this variable is discussed. The variable is listed as a sub-entry to\n"
3226 "\"workspace variables\".\n"
3228 "Usage: Set by the user.\n"
3234 (
NAME(
"sensor_pol" ),
3237 "Sensor polarisations.\n"
3239 "The default for output is to give data for the selected Stokes\n"
3240 "elements (1:stokes_dim). This variable defines the polarisations\n"
3241 "that are actually measured (= or just what shall be outputted).\n"
3242 "This variable is used as input for WSM that handles the extraction\n"
3243 "of polarisation components. This in contrast to *sensor_response_pol*\n"
3244 "and that are used for internal bookkeeping\n"
3246 "The polarisation states/components are coded as\n"
3248 " 1 = I, total intensity.\n"
3249 " 2 = Q, second Stokes component, Iv - Ih.\n"
3250 " 3 = U, third Stokes component, I+45 - I-45.\n"
3251 " 4 = V, forth Stokes component, Irc - Ilc\n"
3252 " 5 = Iv, intensity of vertically polarised component.\n"
3253 " 6 = Ih, intensity of horizontally polarised component.\n"
3254 " 7 = I+45, intensity of +45 deg linearly polarised component.\n"
3255 " 8 = I-45, intensity of -45 deg linearly polarised component.\n"
3256 " 9 = Irhc, intensity of right-hand circularly polarised component.\n"
3257 " 10 = Ilhc, intensity of left-hand circularly polarised component.\n"
3259 "See the documentation for definition of the Stokes vector and the\n"
3260 "different components.\n"
3262 "If the sensor measures the vertical and horisontal componenets, this\n"
3263 "variable shall accordingly be set to [5,6].\n"
3265 "The conversion to Planck-BT of components 2-4 requires that component\n"
3266 "1 is kept, and is put as first element.\n"
3268 "The shift from the Stokes vector can be made at any stage when of the\n"
3269 "sensor response set-up. The responses used must of course be adopted\n"
3270 "correspondingly. Or reversed, if the antenna response is defined for\n"
3271 "Iv and Ih it could be useful to shift polarisation as first sensor\n"
3274 "Usage: Set by the user.\n"
3276 GROUP(
"ArrayOfIndex" )));
3280 (
NAME(
"sensor_pos" ),
3283 "The sensor position for each measurement block.\n"
3285 "The sensor positions are specified as a matrix, where the number of\n"
3286 "columns shall be equal to *atmosphere_dim*. Column 1 shall contain\n"
3287 "the radius of observation posotion, column 2 the latitude and the \n"
3288 "last column the longitude. The number of rows corresponds to the\n"
3289 "number of measurement blocks.\n"
3291 "Valid range for latitudes in 3D is [-90,90], while for 2D any value\n"
3292 "is accepted. Accepted range for longitudes are [-360,360].\n"
3294 "See further the ARTS user guide (AUG). Use the index to find where\n"
3295 "this variable is discussed. The variable is listed as a subentry to\n"
3296 "\"workspace variables\".\n"
3298 "Usage: Set by the user.\n"
3300 "Unit: [ m, degrees, degrees ]\n"
3302 "Size: [ number of measurement blocks, atmosphere_dim ]\n"
3304 GROUP(
"Matrix" )));
3308 (
NAME(
"sensor_response" ),
3311 "The matrix modelling the total sensor response.\n"
3313 "This matrix describes the sensor respons for one measurement block\n"
3314 "The response is assumed to be identical for each such block.\n"
3316 "The matrix is the product of all the individual sensor response\n"
3317 "matrices. Therefore its dimensions are depending on the total sensor\n"
3318 "configuration. The *sensor_response* has to initialised by the \n"
3319 "*sensor_responseInit* method.\n"
3321 "Usage: Output/input to the *sensor_response...* methods.\n"
3325 "Dimension: See the individual *sensor_response...* method. \n"
3327 GROUP(
"Sparse" )));
3331 (
NAME(
"sensor_response_aa" ),
3334 "The relative azimuth angles associated with the output of\n"
3335 "*sensor_response*.\n"
3337 "Definition of angle matches *mblock_aa_grid*. Works otherwise as\n"
3338 "*sensor_response_f*.\n"
3340 "The variable shall not be set manually, it will be set together with\n"
3341 "*sensor_response* by sensor response WSMs.\n"
3343 "Usage: Set by sensor response methods.\n"
3345 "Unit: [ degrees ]\n"
3347 GROUP(
"Vector" )));
3351 (
NAME(
"sensor_response_aa_array" ),
3354 "As *sensor_response_aa* refers to *sensor_response_array*.\n"
3356 GROUP(
"ArrayOfVector" )));
3360 (
NAME(
"sensor_response_aa_grid" ),
3363 "The azimuth angle grid associated with *sensor_response*.\n"
3365 "A variable for communication between sensor response WSMs. Matches\n"
3366 "initially *mblock_aa_grid*, but is later adjusted according to the\n"
3367 "sensor specifications. Only defined when a common grid exists. Values\n"
3368 "are here not repeated as in *sensor_response_aa*\n"
3370 "The zenith and azimuth dimensions are joined into a single dimension\n"
3371 "after the antenna. The variables *sensor_response_za_grid* and \n"
3372 "*sensor_response_aa_grid* have then the same length after the antenna\n"
3373 "(if antenna_dim = 2), holding data taken from the columns of \n"
3376 "Usage: Set by sensor response methods.\n"
3378 "Unit: [ degrees ]\n"
3380 GROUP(
"Vector" )));
3384 (
NAME(
"sensor_response_agenda" ),
3389 GROUP(
"Agenda" )));
3393 (
NAME(
"sensor_response_array" ),
3396 "A set of *sensor_response* matrices.\n"
3398 "The main application of this variable should be to describe the\n"
3399 "sensor characterstics for different measurement blocks (then\n"
3400 "together with *sensor_response_index*.)\n"
3402 GROUP(
"ArrayOfSparse" )));
3406 (
NAME(
"sensor_response_f" ),
3409 "The frequencies associated with the output of *sensor_response*.\n"
3411 "This vector gives the frequency for each element of the measurement\n"
3412 "vector produced inside one measurement block. The frequencies of\n"
3413 "the total measurement vector, *y*, are obtained by repeating these\n"
3414 "frequencies n times, where n is the number of measurement blocks\n"
3415 "(e.g. the number of rows in *sensor_pos*).\n"
3417 "The variable shall not be set manually, it will be set together with\n"
3418 "*sensor_response* by sensor response WSMs.\n"
3420 "Usage: Set by sensor response methods.\n"
3424 GROUP(
"Vector" )));
3428 (
NAME(
"sensor_response_f_array" ),
3431 "As *sensor_response_f* refers to *sensor_response_array*.\n"
3433 GROUP(
"ArrayOfVector" )));
3437 (
NAME(
"sensor_response_f_grid" ),
3440 "The frequency grid associated with *sensor_response*.\n"
3442 "A variable for communication between sensor response WSMs. Matches\n"
3443 "initially *f_grid*, but is later adjusted according to the sensor\n"
3444 "specifications. Only defined when a common grid exists. Values are\n"
3445 "here not repeated as in *sensor_response_f*\n"
3447 "Usage: Set by sensor response methods.\n"
3451 GROUP(
"Vector" )));
3455 (
NAME(
"sensor_response_index" ),
3458 "Identification of *sensor_response* for each measurement block.\n"
3460 "This variable shall hold an index number for each measurement block.\n"
3461 "Typically this index identifies which element of\n"
3462 "*sensor_response_array* that shall be applied.\n"
3464 "Zero based indexing is applied.\n"
3466 GROUP(
"ArrayOfIndex" )));
3470 (
NAME(
"sensor_response_pol" ),
3473 "The polarisation states associated with the output of\n"
3474 "*sensor_response*.\n"
3476 "Works basically as *sensor_response_f*.\n"
3478 "See *sensor_pol* for coding of polarisation states.\n"
3480 "The variable shall not be set manually, it will be set together with\n"
3481 "*sensor_response* by sensor response WSMs.\n"
3483 "Usage: Set by sensor response methods.\n"
3487 GROUP(
"ArrayOfIndex" )));
3491 (
NAME(
"sensor_response_pol_array" ),
3494 "As *sensor_response_pol* refers to *sensor_response_array*.\n"
3496 GROUP(
"ArrayOfArrayOfIndex" )));
3500 (
NAME(
"sensor_response_pol_grid" ),
3503 "The \"polarisation grid\" associated with *sensor_response*.\n"
3505 "A variable for communication between sensor response WSMs. It is\n"
3506 "initially 1:stokes_dim, but can later adjusted according to the \n"
3507 "sensor specifications. Only defined when a common grid exists. \n"
3509 "See *sensor_pol* for coding of polarisation states.\n"
3511 "Usage: Set by sensor response methods.\n"
3515 GROUP(
"ArrayOfIndex" )));
3519 (
NAME(
"sensor_response_za" ),
3522 "The relative zenith angles associated with the output of\n"
3523 "*sensor_response*.\n"
3525 "Definition of angle matches *mblock_za_grid*. Works otherwise as\n"
3526 "*sensor_response_f*.\n"
3528 "The variable shall not be set manually, it will be set together with\n"
3529 "*sensor_response* by sensor response WSMs.\n"
3531 "Usage: Set by sensor response methods.\n"
3533 "Unit: [ degrees ]\n"
3535 GROUP(
"Vector" )));
3539 (
NAME(
"sensor_response_za_array" ),
3542 "As *sensor_response_za* refers to *sensor_response_array*.\n"
3544 GROUP(
"ArrayOfVector" )));
3548 (
NAME(
"sensor_response_za_grid" ),
3551 "The zenith angle grid associated with *sensor_response*.\n"
3553 "A variable for communication between sensor response WSMs. Matches\n"
3554 "initially *mblock_za_grid*, but is later adjusted according to the\n"
3555 "sensor specifications. Only defined when a common grid exists. Values\n"
3556 "are here not repeated as in *sensor_response_za*\n"
3558 "The zenith and azimuth dimensions are joined into a single dimension\n"
3559 "after the antenna. The variables *sensor_response_za_grid* and \n"
3560 "*sensor_response_aa_grid* have then the same length after the antenna\n"
3561 "(if antenna_dim = 2), holding data taken from the columns of \n"
3564 "Usage: Set by sensor response methods.\n"
3566 "Unit: [ degrees ]\n"
3568 GROUP(
"Vector" )));
3605 (
NAME(
"sensor_time" ),
3608 "The time for each measurement block.\n"
3610 "This WSV is used when a time must be assigned to the measurements.\n"
3611 "No specific time format has (yet) been specified.\n"
3613 "Usage: Set by the user.\n"
3615 "Unit: [ arbitrary ]\n"
3617 "Size: [ number of measurement blocks ]\n"
3619 GROUP(
"Vector" )));
3623 (
NAME(
"sideband_mode" ),
3626 "Description of target sideband.\n"
3628 "A text string describing which of the two sidebands (of a heterodyne\n"
3629 "instrument) that can be seen as \"main\" band. Possible choices are:\n"
3630 " \"lower\" : Low frequency sideband shall be considered as target.\n"
3631 " \"upper\" : High frequency sideband shall be considered as target.\n"
3633 "Usage: Set by the user.\n"
3635 GROUP(
"String" )));
3639 (
NAME(
"sideband_mode_multi" ),
3642 "Description of target sideband for a multiple LO reciever.\n"
3644 "As *sideband_mode* but handles an instrument with several LO chains.\n"
3645 "See further *lo_multi* and *sideband_response_multi*. This length of\n"
3646 "this array must match the size of those WSVs.\n"
3648 "Usage: Set by the user.\n"
3650 GROUP(
"ArrayOfString" )));
3655 (
NAME(
"sideband_response" ),
3658 "Description of (mixer) sideband response.\n"
3660 "This variable describes the response of each sideband of a heterodyne\n"
3661 "receiver. The response is given as a GriddedField1, with frequency as the\n"
3662 "grid. The actual data describe the sideband filter function at each\n"
3663 "frequency grid point. An interpolation is applied to obtain the\n"
3664 "response for other frequencies.\n"
3666 "The frequency grid should be given in terms of IF, with end points\n"
3667 "symmetrically placed around zero. That is, the grid must contain\n"
3668 "both negative and positive values. The sideband response (after \n"
3669 "summation with *lo*) is not allowed to extend outside the range\n"
3670 "for which spectral data exist (normally determined by *f_grid*).\n"
3672 "Usage: Set by the user.\n"
3676 " Vector f_grid[N_f]\n"
3677 " Vector data[N_f]\n"
3679 GROUP(
"GriddedField1" )));
3683 (
NAME(
"sideband_response_multi" ),
3686 "Description of multiple (mixer) sideband responses.\n"
3688 "As *sideband_response* but describes an instrument with multiple\n"
3689 "mixers. An array element for each LO. The size of this variable and\n"
3690 "*lo_multi* shall match.\n"
3694 "Usage: Set by the user.\n"
3696 GROUP(
"ArrayOfGriddedField1" )));
3700 (
NAME(
"single_scattering_data" ),
3703 "Structure for the single scattering data.\n"
3705 "See futher the ArtsWiki documentation were the SingleScatteringData\n"
3706 "structure is disussed.\n"
3708 "Usage: Set by the user.\n"
3710 "Dimensions: SingleScatteringData \n"
3711 " Enum[particle type attribute]\n"
3712 " String[description] \n"
3715 " Vector[za_grid]\n"
3716 " Vector[aa_grid]\n"
3717 " Tensor7[pha_mat_data]\n"
3718 " [f_grid, T_grid, za_grid, aa_grid, za_grid, aa_grid, matrix_element]\n"
3719 " ^^^^^^^^^^^^^^^^ ^^^^^^^^^^^^^^^^\n"
3720 " scattered incoming\n"
3721 " Tensor5[ext_mat_data]\n"
3722 " [f_grid, T_grid, za_grid, aa_grid, matrix_element]\n"
3723 " Tensor5[abs_vec_data]\n"
3724 " [f_grid, T_grid, za_grid, aa_grid, matrix_element]\n"
3726 GROUP(
"SingleScatteringData" )));
3730 (
NAME(
"stokes_dim" ),
3733 "The dimensionality of the Stokes vector (1-4).\n"
3735 "Usage: Set by the user.\n"
3741 (
NAME(
"spt_calc_agenda" ),
3746 GROUP(
"Agenda" )));
3750 (
NAME(
"surface_emission" ),
3752 (
"The emission from the surface.\n"
3754 "See specific methods generating *surface_emission* and the user guide\n"
3755 "for more information.\n"
3757 "Unit: W / (m^2 Hz sr)\n"
3759 "Dimensions: [ f_grid, stokes_dim ]\n"
3761 GROUP(
"Matrix" )));
3765 (
NAME(
"surface_emissivity_DISORT" ),
3767 (
"The surface emissivity specified on lat_grid and lon_grid.\n"
3769 "Remnant from a first solution for surface emissivity fields.\n"
3770 "Should be replaced with more flexible solution allowing emissivity\n"
3771 "to vary with incidence angle.\n"
3773 "Dimensions: [ lat_grid, lon_grid ]\n"
3775 GROUP(
"Matrix" )));
3779 (
NAME(
"surface_los" ),
3782 "Directions for which to calculate downwelling radiation when \n"
3783 "considering a surface reflection.\n"
3785 "See further the user guide.\n"
3789 "Size: [ any number, 1 or 2 ]\n"
3791 GROUP(
"Matrix" )));
3795 (
NAME(
"surface_prop_agenda" ),
3800 GROUP(
"Agenda" )));
3804 (
NAME(
"surface_rmatrix" ),
3807 "The reflection coefficients for the directions given by\n"
3808 "*surface_los* to the direction of interest.\n"
3810 "The rows and columns of this tensor holds the reflection\n"
3811 "coefficient matrix for one frequency and one LOS. The reflection\n"
3812 "coefficients shall take into accound the angular weighting if the\n"
3813 "downwelling radiation.\n"
3815 "See specific methods generating *surface_rmatrix* and the user guide\n"
3816 "for more information.\n"
3818 "Usage: Input to methods for *surface_prop_agenda*."
3822 "Dimensions: [ surface_los, f_grid, stokes_dim, stokes_dim ]\n"
3824 GROUP(
"Tensor4" )));
3828 (
NAME(
"surface_skin_t" ),
3831 "Surface skin temperature.\n"
3833 "This temperature shall be selected considering the radiative\n"
3834 "properties of the surface, and can differ from the \"bulk\"\n"
3837 "Usage: Input to methods for *surface_prop_agenda*.\n"
3839 GROUP(
"Numeric" )));
3843 (
NAME(
"surface_scalar_reflectivity" ),
3846 "Surface reflectivity, assuming it can be described as a scalar value.\n"
3848 "This variable describes the surface reflectivity at one position.\n"
3850 "The variable is primarily intended for scalar radiative transfer.\n"
3851 "The assumptions made, when using this variable with values of\n"
3852 "*stokes_dim* above 1, are described in the methods using this\n"
3853 "variable as input.\n"
3855 "The length of the vector shall either match *f_grid* or be 1. The \n"
3856 "later case is interpreted as the reflectivity is the same for all\n"
3857 "frequencies (ie. matches a constant vector).\n"
3859 "Usage: Input to some surface properties methods.\n"
3861 "Dimensions: [ f_grid or 1]\n"
3863 GROUP(
"Vector" )));
3867 (
NAME(
"test_agenda" ),
3872 GROUP(
"Agenda" )));
3879 "Stores the starting time for time measurements.\n"
3885 (
NAME(
"t_field" ),
3888 "The field of atmospheric temperatures.\n"
3890 "This variable gives the atmospheric temperature at each crossing of\n"
3891 "the pressure, latitude and longitude grids.\n"
3893 "The temperature for a point between the grid crossings is obtained \n"
3894 "by (multi-)linear interpolation of the *t_field*.\n"
3896 "See further the ARTS user guide (AUG). Use the index to find where\n"
3897 "this variable is discussed. The variable is listed as a subentry to\n"
3898 "\"workspace variables\".\n"
3900 "Usage: Output of *AtmFieldsCalc*.\n"
3904 "Dimensions: [ p_grid, lat_grid, lon_grid ]\n"
3906 GROUP(
"Tensor3" )));
3910 (
NAME(
"t_field_raw" ),
3913 "Raw data for atmospheric temperatures.\n"
3915 "This variable gives the atmospheric temperature as stored in the \n"
3916 "database for the atmospheric scenarios.\n"
3918 "See further the ARTS user guide (AUG). Use the index to find where\n"
3919 "this variable is discussed. The variable is listed as a subentry to\n"
3920 "\"workspace variables\".\n"
3922 "Usage: Set by the user by choosing a climatology.\n"
3926 "Size GriddedField3 \n "
3930 " [N_p, N_lat, N_lon] \n"
3932 GROUP(
"GriddedField3" )));
3936 (
NAME(
"t_surface" ),
3939 "The surface temperature.\n"
3941 "This variable holds the temperature of the surface at each latitude\n"
3942 "and longitude grid crossing. The normal case should be that this \n"
3943 "temperature field is interpolated to obtain *surface_skin_t*.\n"
3944 "Accordingly, for 1D cases it could be a better idea to specify\n"
3945 "*surface_skin_t* directly.\n"
3947 "These temperature shall be selected considering the radiative\n"
3948 "properties of the surface, and can differ from the \"bulk\"\n"
3951 "Usage: Set by user.\n"
3955 "Dimensions: [ lat_grid, lon_grid ]\n"
3957 GROUP(
"Matrix" )));
3961 (
NAME(
"use_mean_scat_data" ),
3964 "Flag to use same scattering properties for all frequencies.\n"
3966 "This flag is not considered y all scattering methods, but (at least)\n"
3967 "by *iyFOS* and *iyBeerLambertStandardCloudbox*.\n"
3969 "If set to 1, the scattering properties are extracted for a single\n"
3970 "frequency, and these properties are applied for all frequncies when\n"
3971 "performing the actual radiative transfer calculations. This can save\n"
3972 "considerable time. The option can be when the width of the band is\n"
3973 "small comapred to the mean frequency. The properties are extracted\n"
3974 "for the mean of min and max of *f_grid*.\n"
3976 "If set to 0, standard calculations are made (scattering properties\n"
3977 "extracted for each frequency).\n"
3979 "Usage: Set by user.\n"
3985 (
NAME(
"verbosity" ),
3990 "!!! UNDER CONSTRUCTION !!! Currently unused\n"
3992 "Usage: Set by user.\n"
3994 GROUP(
"Verbosity" )));
3998 (
NAME(
"vmr_field" ),
4003 "This variable gives the volume mixing ratio of the chosen gaseous \n"
4004 "species as a function of p_grid, lat_grid, lon_grid. \n"
4006 "See further the ARTS user guide (AUG). Use the index to find where\n"
4007 "this variable is discussed. The variable is listed as a subentry to\n"
4008 "\"workspace variables\".\n"
4011 "Usage: Calculated internally.\n"
4013 "Unit: absolute numbers \n"
4015 "Dimensions: [species, p_grid, lat_grid, lon_grid]\n"
4017 GROUP(
"Tensor4" )));
4021 (
NAME(
"vmr_field_raw" ),
4024 "VMR data for the chosen gaseous species.\n"
4026 "This variable contains the volume mixing ratios (VMR) for all \n"
4027 "chosen gaseous species. It includes the grids corresponding to the \n"
4028 "grids in the database. \n"
4029 "*vmr_field_raw* is an Array of Array of Tensor3. It contains one \n"
4030 "gridded field for each species which contains the data and \n"
4032 "For the calculation the data is \n"
4033 "interpolated on *p_grid*, *lat_grid* and *lon_grid*\n"
4035 "Usage: Output of *AtmRawRead*\n"
4036 " Input to *AtmFieldsCalc*.\n"
4038 "Unit: absolute number\n"
4040 "Size: Array[N_pt]\n"
4041 " GriddedField3 \n "
4045 " [N_p, N_lat, N_lon] \n"
4047 GROUP(
"ArrayOfGriddedField3" )));
4051 (
NAME(
"wmrf_channels" ),
4054 "Channel selection for WMRF fast calculation.\n"
4056 "This variable can be used to select one or several instrument channels\n"
4057 "from the list of all possible channels. Zero-based indexing is used, so\n"
4058 "Channel 0 is the first instrument channel!\n"
4060 GROUP(
"ArrayOfIndex" )));
4064 (
NAME(
"wind_u_field" ),
4067 "Meridional (second horizontal wind) component field for 3D.\n"
4069 "The east-west wind component. Air moving towards higher\n"
4070 "longitudes is a positive wind.\n"
4072 "Can be set to be empty, which is interpreted as zero wind speed\n"
4077 "Dimensions: [ p_grid, lat_grid, lon_grid ] or [ 0 0 0 ].\n"
4079 GROUP(
"Tensor3" )));
4083 (
NAME(
"wind_v_field" ),
4086 "Horizontal 1D, 2D or 3D wind components.\n"
4088 "This wind component is defined differently for the atmospheric\n"
4089 "dimensionalities.\n"
4091 " 1D: Complete vertical wind. The wind is treated to always be aligned\n"
4092 "azimuthally with the observation direction. That is, the vertical\n"
4093 "winds converge/start at geographical position of the sensor. A wind\n"
4094 "going away from the sensor is treated as positive.\n"
4096 " 2D: Complete vertical wind. The wind is treated to be aligned with\n"
4097 "the 2D cross-section the atmosphere represents. Air moving towards\n"
4098 "higher latitudes is considered as a positive wind.\n"
4100 " 3D: The north-south wind component. Air moving towards higher\n"
4101 "latitudes is a positive wind.\n"
4103 "Can be set to be empty, which is interpreted as zero wind speed\n"
4108 "Dimensions: [ p_grid, lat_grid, lon_grid ] or [ 0 0 0 ]\n"
4110 GROUP(
"Tensor3" )));
4114 (
NAME(
"wind_w_field" ),
4117 "Vertical wind component field.\n"
4119 "Upward moving air corresponds to a positive wind speed.\n"
4121 "Can be set to be empty, which is interpreted as zero wind speed\n"
4126 "Dimensions: [ p_grid, lat_grid, lon_grid ] or [ 0 0 0 ]\n"
4128 GROUP(
"Tensor3" )));
4132 (
NAME(
"wmrf_weights" ),
4135 "The weights for a WMRF fast calculation.\n"
4137 "Weights are stored in a sparse matrix. This can be used as a\n"
4138 "sensor_response matrix.\n"
4140 "The dimension of the matrix is (nchan, nfreq), where nchan\n"
4141 "is the number of instrument channels and nfreq is the number\n"
4142 "of monochromatic frequencies.\n"
4144 GROUP(
"Sparse" )));
4148 (
NAME(
"xml_output_type" ),
4151 "Flag to determine whether XML output shall be binary or ascii.\n"
4153 "This flag has to be set using the workspace method\n"
4154 "*output_file_formatSetAscii* or *output_file_formatSetBinary*.\n"
4155 "One of these methods MUST be called before writing the first\n"
4158 "Usage: Set by user.\n"
4167 "The measurement vector.\n"
4169 "This vector holds radiances averaged in frequency and spatially,\n"
4170 "and can contain many spectra appended. \n"
4172 "Usage: Output from radiative transfer calculations considering\n"
4173 " sensor response.\n"
4175 "Unit: Undefined. Possibilities include: K, W/(m^2 Hz sr) and\n "
4176 " optical thickness.\n"
4178 GROUP(
"Vector" )));
4185 "Data auxilary to *y*\n"
4187 "A general variable to provide data auxilary to *y*. The content of\n"
4188 "this variable depends on method selected for *iy_clearsky_agenda*\n"
4189 "and *iy_cloudbox_agenda*. For methods dealing with radiance data,\n"
4190 "this variable is used to report the transmission of the atmosphere.\n"
4191 "This transmission can be calculated in a simplified manner, or be\n"
4192 "set to special values to indicate e.g. an interception with the\n"
4193 "cloudbox. See the relevant WSMs for details, and also *iy_aux*. \n"
4195 "If created through *yCalc*, the weighting with *sensor_response*\n"
4196 "is included. A value of 999 indicates that no data have been\n"
4197 "provided by the agenda methods.\n"
4199 GROUP(
"Vector" )));
4203 (
NAME(
"y_error" ),
4206 "Estimate of calculation errors in *y*.\n"
4208 "This variable is used for providing an error estimate. The estimate\n"
4209 "covers only the actual calculation approach, and e.g. uncertainties\n"
4210 "in spectroscopic data or representation errors due to coarse grids\n"
4211 "are not considered. This means that the error should normally be\n"
4212 "zero for clear-sky cases where calculations are performed for the\n"
4213 "complete propagation path.\n"
4215 GROUP(
"Vector" )));
4222 "The frequencies associated with *y*.\n"
4224 "A value is returned for each element of *y*. Depending on the sensor\n"
4225 "set-up and number of measurement blocks, this can be a copy of\n"
4226 "*sensor_response_f*, sveral copies of this vector appended, or some\n"
4227 "other frequenices.\n"
4229 "Usage: Output from radiative transfer calculations considering\n"
4230 " sensor response.\n"
4234 GROUP(
"Vector" )));
4241 "The line-of-sights associated with *y*.\n"
4243 "Definition of angles matches *sensor_los* (such as first column holds\n"
4244 "zenith angles), but gives actual observed LOS. That is, the values of\n"
4245 "both *sensor_los* and *antenna_los* are considered. Data are provided\n"
4246 "for each element of *y*, following y_f, and the number of rows equals\n"
4247 "the length of *y*.\n"
4249 "Usage: Output from radiative transfer calculations considering\n"
4250 " sensor response.\n"
4252 "Unit: [ degrees, degrees ]\n"
4254 GROUP(
"Matrix" )));
4261 "The polarisation states associated with *y*.\n"
4263 "Data are provided for each element of *y*, following y_f, and the\n"
4264 "length of this variable and *y* is equal.\n"
4266 "See *sensor_pol* for coding of polarisation components.\n"
4268 "Usage: Output from radiative transfer calculations considering\n"
4269 " sensor response.\n"
4273 GROUP(
"ArrayOfIndex" )));
4280 "The sensor positions associated with *y*.\n"
4282 "Definition of positions matches *sensor_pos* (such as first column\n"
4283 "holds the radius). Data are provided for each element of *y*,\n"
4284 "following y_f, and the number of rows equals the length of *y*.\n"
4286 "Usage: Output from radiative transfer calculations considering\n"
4287 " sensor response.\n"
4289 "Unit: [ degrees, degrees ]\n"
4291 GROUP(
"Matrix" )));
4298 "Unit for spectral values returned by radiative transfer methods.\n"
4300 "The basic unit is determined by the definition of background\n"
4301 "radiation and atmospheric and surface source terms. The standard\n"
4302 "choices give radiances in unit of [W/m2/Hz/sr]. This variable\n"
4303 "allows conversion to other units.\n"
4305 "Please note that there is no way for ARTS to check the actual unit\n"
4306 "of a spectral value. In principle, the unit can differ between the\n"
4307 "elements. The user must makes sure that any unit conversion is\n"
4308 "applied correctly, and in accordance with the calibration of the\n"
4309 "instrument of concern. Note especially that the brightness\n"
4310 "temperature of pure Stokes elements is obtained with a common power\n"
4311 "reference. In short, the ratio is Q/I is not changed by the\n"
4312 "conversion (beside a non-linear effect for PlanckBT). This in\n"
4313 "contrast to Iv and other single \"measurement\" single polarisation\n"
4314 "componenets, where a Tb of e.g. Iv=200K corresponds to half of the\n"
4315 "power for I=200K (total power). See further the documentation.\n"
4316 "See *y_pol* for defined polarisation componenets.\n"
4318 "Possible choices are:\n"
4319 " \"1\" : No conversion.\n"
4320 " \"RJBT\" : Conversion to Rayleigh-Jean brightness temperature.\n"
4321 " \"PlanckBT\" : Conversion to Planck brightness temperature.\n"
4322 " \"W/(m^2 m sr)\" : Conversion to [W/(m^2 m sr)] (radiance per wavelength unit).\n"
4323 " \"W/(m^2 m-1 sr)\": Conversion to [W/(m^2 m-1 sr)] (radiance per wavenumber unit).\n"
4325 "Usage: Set by the user.\n"
4327 GROUP(
"String" )));
4334 "The measurement vector for a single measurement block.\n"
4336 "Exactly as *y*, but holds data only for a single measurement block.\n"
4338 "Usage: Used internally.\n"
4340 GROUP(
"Vector" )));
4347 "Batch of spectra.\n"
4349 "Each column of *ybatch* corresponds to a spectrum vector *y*. \n"
4350 "See further *ybatchCalc*.\n"
4352 "Usage: Most commonly produced by *ybatch*.\n"
4354 "Unit: Undefined. Possibilities include: K, W/(m^2 Hz sr) and\n "
4355 " optical thickness.\n"
4357 "Dimensions: (length(y), number of batch cases)\n"
4359 GROUP(
"Matrix" )));
4363 (
NAME(
"ybatch_calc_agenda" ),
4368 GROUP(
"Agenda" )));
4372 (
NAME(
"ybatch_index" ),
4375 "Index of batch case.\n"
4377 "See further *ybatchCalc*.\n"
4379 "Usage: Set by *ybatchCalc*, for communication with\n"
4380 " *ybatch_calc_agenda*.\n"
4386 (
NAME(
"ybatch_jacobians" ),
4389 "All the Jacobians associated with ybatch.\n"
4391 "The batch index here is the array dimension.\n"
4393 "Usage: Most commonly produced by *ybatch*.\n"
4395 "Unit: Depends on unit of y and on Jacobian type.\n"
4397 "Dimensions: [number of batch cases] \n"
4399 " number of retrieval quantities and grids)\n"
4401 GROUP(
"ArrayOfMatrix" )));
4405 (
NAME(
"ybatch_n" ),
4408 "Number of batch cases for *ybatchCalc*.\n"
4410 "See further *ybatchCalc*.\n"
4412 "Usage: Input to *ybatchCalc*.\n"
4418 (
NAME(
"ybatch_start" ),
4421 "Start index for *ybatchCalc*.\n"
4423 "This is set to a default of zero in *general.arts*.\n"
4425 "See further *ybatchCalc*.\n"
4427 "Usage: Input to *ybatchCalc*.\n"
4433 (
NAME(
"z_field" ),
4436 "The field of geometrical altitudes.\n"
4438 "This variable gives the geometrical altitude, above the geoid, of\n"
4439 "each crossing of the pressure, latitude and longitude grids. For 1D\n"
4440 "cases the altitudes give the geometrical position of the pressure\n"
4443 "For each geographical position (lat,lon), the values must be sorted\n"
4444 "in increasing order, with no repetitions. Otherwise the altitudes\n"
4445 "can be set to arbitrary values. Hydrostatic equilibrium is not\n"
4446 "applied automatically. If hydrostatic equilibrium applies, *z_field*\n"
4447 "must be set by a method ensuring that this criterium is fulfilled.\n"
4449 "The radius (from the coordinate centre) for a point between the grid\n"
4450 "crossings is obtained by a (multi-)linear interpolation of the sum\n"
4451 "of *r_geoid* and *z_field*.\n"
4453 "See further the ARTS user guide (AUG). Use the index to find where\n"
4454 "this variable is discussed. The variable is listed as a subentry to\n"
4455 "\"workspace variables\".\n"
4457 "Usage: Output of *AtmFieldsCalc*\n"
4461 "Dimensions: [ p_grid, lat_grid, lon_grid ]\n"
4463 GROUP(
"Tensor3" )));
4476 (
NAME(
"z_field_raw" ),
4479 "Raw data for geometrical altitudes.\n"
4481 "This variable gives the geometrical altitudes as stored in the \n"
4482 "database for atmospheric scenarios.\n"
4484 "See further the ARTS user guide (AUG). Use the index to find where\n"
4485 "this variable is discussed. The variable is listed as a subentry to\n"
4486 "\"workspace variables\".\n"
4488 "Usage: Set by the user by choosing a climatology.\n"
4492 "Size GriddedField3 \n "
4496 " [N_p, N_lat, N_lon] \n"
4498 GROUP(
"GriddedField3" )));
4502 (
NAME(
"z_hse_accuracy" ),
4505 "Minimum accuracy for calculation of hydrostatic equilibrium.\n"
4507 "Usage: Set by the user.\n"
4511 GROUP(
"Numeric" )));
4515 (
NAME(
"z_surface" ),
4518 "The surface altitude.\n"
4520 "This variable defines the shape of the surface, by giving the\n"
4521 "geometrical altitude above the geiod for each crossing of the \n"
4522 "latitude and longitude grids. Any shape of the surface is accepted.\n"
4523 "No gap between the surface and the lowermost pressure level is \n"
4526 "The radius (from the coordinate centre) for a point between the grid\n"
4527 "crossings is obtained by a linear (1D) or bi-linear (2D) \n"
4528 "interpolation of the sum of *r_geoid* and *z_surface*. With other \n"
4529 "words, the radius for the surface is assumed to vary linear along \n"
4530 "the latitudes and longitudes in *lat_grid* and *lon_grid*.\n"
4532 "See further the ARTS user guide (AUG). Use the index to find where\n"
4533 "this variable is discussed. The variable is listed as a subentry to\n"
4534 "\"workspace variables\".\n"
4536 "Usage: Set by user.\n"
4540 "Dimensions: [ lat_grid, lon_grid ]\n"
4542 GROUP(
"Matrix" )));
static Array< WsvRecord > wsv_data
This file contains the definition of Array.
The implementation for String, the ARTS string class.
static void define_wsv_data()
Propagation path structure and functions.
This class contains all static information for one workspace variable.
This file contains the declaration and partly the implementation of the workspace class.
my_basic_string< char > String
The String type for ARTS.
static map< String, Index > WsvMap
Header file for sparse matrices.
Index get_wsv_id(const String &name)
Get index of WSV.
INDEX Index
The type to use for all integer numbers and indices.
Auxiliary header stuff related to workspace variable groups.
The global header file for ARTS.