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00035 #include "arts.h"
00036 #include "matpackI.h"
00037 #include "array.h"
00038 #include "auto_wsv_groups.h"
00039 #include "wsv_aux.h"
00040
00042 Array<WsvRecord> wsv_data;
00043
00044 void define_wsv_data()
00045 {
00046
00047
00048
00049 wsv_data.resize(0);
00050
00051
00052
00053
00054 wsv_data.push_back
00055 (WsvRecord
00056 ("lines",
00057 "A list of spectral line data.",
00058 ArrayOfLineRecord_));
00059
00060 wsv_data.push_back
00061 (WsvRecord
00062 ("lines_per_tg",
00063 "A list of spectral line data for each tag.\n"
00064 "Dimensions: (tag_groups.nelem()) (# of lines for this tag)",
00065 ArrayOfArrayOfLineRecord_));
00066
00067 wsv_data.push_back
00068 (WsvRecord
00069 ("tgs",
00070 "This is an array of arrays of OneTag tag definitions.\n"
00071 "It defines the available tag groups for the calculation\n"
00072 "of absorption coefficients and weighting functions.\n"
00073 "Contrary to the original Bredbeck definition, tags within a\n"
00074 "group must belong to the same species, because one VMR profile\n"
00075 "is associated with each tag group.",
00076 TagGroups_));
00077
00078 wsv_data.push_back
00079 (WsvRecord
00080 ("wfs_tgs",
00081 "This is an array of arrays of tag group definitions.\n"
00082 "It defines the tag groups for the calculation of weighting\n"
00083 "functions. The selected tag groups must be a subgroup of the\n"
00084 "tag groups defined for the absorption coefficient calculation.",
00085 TagGroups_));
00086
00087 wsv_data.push_back
00088 (WsvRecord
00089 ("wfss_tgs",
00090 "This is an array of arrays of tag group definitions.\n"
00091 "It defines the tag groups for the calculation of weighting\n"
00092 "functions. The selected tag groups must be a subgroup of the\n"
00093 "tag groups defined for the absorption coefficient calculation.",
00094 TagGroups_));
00095
00096 wsv_data.push_back
00097 (WsvRecord
00098 ("lineshape",
00099 "Lineshape specification: function, norm, cutoff. There is one entry for\n"
00100 "each abs_tag, not for each species. This means if you have several\n"
00101 "abs_tags for different isotopes or transitions of a species, you\n"
00102 "may use different lineshapes.",
00103 ArrayOfLineshapeSpec_));
00104
00105
00106
00107
00108 wsv_data.push_back
00109 (WsvRecord
00110 ("cont_description_names",
00111 "Continuum / full model absorption tag names. This variable should\n"
00112 "contain a list of tag names of continuum and full models, respectively.\n"
00113 "Associated with this WSV is the WSV\n"
00114 "`cont_description_models' which contains the specific model version of\n"
00115 "each continuum / full model absorption tag and the WSV\n"
00116 "`cont_description_parameters' which should contain the continuum / full model\n"
00117 "user defined parameters. The user defined parameters are only used when\n"
00118 "the specified model is 'user'. See also the online documentation in\n"
00119 "arts/doc/doxygen/html/continua_cc.html.\n"
00120 "\n"
00121 "The following full water vapor models are implemented:\n"
00122 "'H2O-MPM87': absorption model (line and continuum) according to \n"
00123 " H. J. Liebe,\n"
00124 " A contribution to modeling atmospheric millimeter-wave properties,\n"
00125 " Frequenz, 41, 1987, 31-36\n"
00126 " and\n"
00127 " H. J. Liebe and D. H. Layton,\n"
00128 " Millimeter-wave properties of the atmosphere:\n"
00129 " Laboratory studies and propagation modeling,\n"
00130 " U.S. Dept. of Commerce, National Telecommunications and Information\n"
00131 " Administration, Institute for Communication Sciences,\n"
00132 " 325 Broadway, Boulder, CO 80303-3328, report 87224.\n"
00133 "'H2O-MPM89': absorption model (line and continuum) according to \n"
00134 " H. J. Liebe,\n Int. J. Infrared and Millimeter Waves, 10(6), 1989, 631\n"
00135 "'H2O-MPM93': absorption model (line and continuum) according to \n"
00136 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
00137 " Propagation modeling of moist air and suspended water/ice\n"
00138 " particles at frequencies below 1000 GHz,\n"
00139 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
00140 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21 \n"
00141 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
00142 "'H2O-CP98': absorption model (line and continuum) according to \n"
00143 " S. L. Cruz-Pol et al.,\n Radio Science, 33(5), 1319, 1998"
00144 " (ece.uprm.edu/~pol/Atmosphere.html)\n"
00145 "'H2O-PWR98': absorption model (line and continuum) according to \n"
00146 " P. W. Rosenkranz,\n "
00147 " Radio Science, 33(4), 919, 1998, Radio Science, 34(4), 1025, 1999\n"
00148 " (ftp: mesa.mit.edu/phil/lbl_rt).\n"
00149 "\n"
00150 "The following full oxygen models are implemented:\n"
00151 "'O2-MPM93': absorption model (line and continuum) according to\n"
00152 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
00153 " Propagation modeling of moist air and suspended water/ice\n"
00154 " particles at frequencies below 1000 GHz,\n"
00155 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
00156 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21\n"
00157 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
00158 "'O2-PWR93': absorption model (line and continuum) according to \n"
00159 " P. W. Rosenkranz,\n Chapter 2, in M. A. Janssen, \n"
00160 " Atmospheric Remote Sensing by Microwave Radiometry\n"
00161 " John Wiley & Sons, Inc., 1993 (mesa.mit.edu/phil/lbl_rt)\n"
00162 "\n"
00163 "The following continuum parameterizations are implemented:\n"
00164 "H2O-H2O ('H2O-SelfContStandardType'):\n"
00165 " P. W. Rosenkranz, \n"
00166 " Radio Science, Vol. 33, No 4, Pages 919-928, 1998 and \n"
00167 " Radio Science, Vol. 34, No 4, Page 1025, 1999 (mesa.mit.edu/phil/lbl_rt)\n"
00168 "H2O-air ('H2O-ForeignContStandardType'): \n"
00169 " P. W. Rosenkranz, \n"
00170 " Radio Science, Vol. 33, No 4, Pages 919-928, 1998 and \n"
00171 " Radio Science, Vol. 34, No 4, Page 1025, 1999 (mesa.mit.edu/phil/lbl_rt)\n"
00172 "H2O-air ('H2O-ContMPM93'): \n"
00173 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
00174 " Propagation modeling of moist air and suspended water/ice\n"
00175 " particles at frequencies below 1000 GHz,\n"
00176 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
00177 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21\n"
00178 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
00179 "O2-air ('O2-SelfContStandardType'):\n"
00180 " P. W. Rosenkranz,\n"
00181 " Chapter 2, in M. A. Janssen,\n"
00182 " Atmospheric Remote Sensing by Microwave Radiometry,\n"
00183 " John Wiley & Sons, Inc., 1993\n"
00184 " (mesa.mit.edu/phil/lbl_rt)\n"
00185 " and also described in \n"
00186 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
00187 " Propagation modeling of moist air and suspended water/ice\n"
00188 " particles at frequencies below 1000 GHz,\n"
00189 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
00190 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21\n"
00191 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
00192 "N2-N2 ('N2-SelfContStandardType'):\n"
00193 " The functional form of Rosenkranz but with more input parameters.\n"
00194 " P. W. Rosenkranz,\n"
00195 " Chapter 2, in M. A. Janssen,\n"
00196 " Atmospheric Remote Sensing by Microwave Radiometry,\n"
00197 " John Wiley & Sons, Inc., 1993 (mesa.mit.edu/phil/lbl_rt)\n"
00198 "N2-N2 ('N2-SelfContMPM93'):\n"
00199 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
00200 " Propagation modeling of moist air and suspended water/ice\n"
00201 " particles at frequencies below 1000 GHz,\n"
00202 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
00203 " Propagation Panel, Palma de Mallorca, Spain, 1993, May 17-21 \n"
00204 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
00205 "CO2-CO2 ('CO2-SelfContPWR93'):\n"
00206 " P. W. Rosenkranz,\n"
00207 " Chapter 2, in M. A. Janssen,\n"
00208 " Atmospheric Remote Sensing by Microwave Radiometry,\n"
00209 " John Wiley & Sons, Inc., 1993 (mesa.mit.edu/phil/lbl_rt)\n"
00210 "CO2-N2 ('CO2-ForeignContPWR93'):\n"
00211 " P. W. Rosenkranz,\n"
00212 " Chapter 2, in M. A. Janssen,\n"
00213 " Atmospheric Remote Sensing by Microwave Radiometry,\n"
00214 " John Wiley & Sons, Inc., 1993 (mesa.mit.edu/phil/lbl_rt)\n"
00215 "\n"
00216 "The following cloud absorption models are implemented:\n"
00217 "Suspended water droplet ('liquidcloud-MPM93') \n"
00218 " absorption parameterization from the MPM93 model:\n"
00219 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
00220 " Propagation modeling of moist air and suspended water/ice\n"
00221 " particles at frequencies below 1000 GHz,\n"
00222 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
00223 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21\n"
00224 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
00225 "Ice water droplet absorption ('icecloud-MPM93') \n"
00226 " parameterization from MPM93 model:\n"
00227 " H. J. Liebe and G. A. Hufford and M. G. Cotton,\n"
00228 " Propagation modeling of moist air and suspended water/ice\n"
00229 " particles at frequencies below 1000 GHz,\n"
00230 " AGARD 52nd Specialists Meeting of the Electromagnetic Wave\n"
00231 " Propagation Panel,\n Palma de Mallorca, Spain, 1993, May 17-21\n"
00232 " (ftp.its.bldrdoc.gov/pub/mpm93/)\n"
00233 "\n"
00234 "The following rain extinction model is implemented:\n"
00235 "Rain extinction parameterization ('rain-MPM93') from the\n"
00236 " MPM93 model, described in:\n"
00237 " H. J. Liebe,\n"
00238 " MPM - An Atmospheric Millimeter-Wave Propagation Model,\n"
00239 " Int. J. Infrared and Millimeter Waves, vol. 10(6),\n"
00240 " pp. 631-650, 1989;\n"
00241 " and based on:\n"
00242 " Olsen, R.L., D.V. Rogers, and D. B. Hodge,\n"
00243 " The aR^b relation in the calculation of rain attenuation,\n"
00244 " IEEE Trans. Antennas Propagat., vol. AP-26, pp. 318-329, 1978.\n"
00245 " IMPORTANT NOTE: rain-MPM93 parameterizes the EXTINCTION by rain,\n"
00246 " not just the absorption. Therefore it is not suitable for \n"
00247 " calculating thermal emission by rain!\n"
00248 " Please use rain-MPM93 only for calculation of attenuation.\n"
00249 "\n",
00250 ArrayOfString_));
00251
00252 wsv_data.push_back
00253 (WsvRecord
00254 ("cont_description_models",
00255 "Continuum / full model absorption model description parameter.\n"
00256 "See the WSV `cont_description_names' for a detailed description\n"
00257 "of the allowed continuum models. There should be one string here\n"
00258 "for each entry in `cont_description_names'.See also the online"
00259 "documentation in arts/doc/doxygen/html/continua_cc.html.\n",
00260 ArrayOfString_));
00261
00262 wsv_data.push_back
00263 (WsvRecord
00264 ("cont_description_parameters",
00265 "Continuum model parameters. See the WSV `cont_description_names'\n"
00266 "for a detailed description of the allowed continuum models. There\n"
00267 "should be one parameter vector here for each entry in\n"
00268 "`cont_description_names'. See also the online documentation in\n"
00269 "arts/doc/doxygen/html/continua_cc.html.\n",
00270 ArrayOfVector_));
00271
00272
00273
00274
00275 wsv_data.push_back
00276 (WsvRecord
00277 ("raw_ptz",
00278 "Matrix has rows:\n"
00279 "1. Pressure in Pa\n"
00280 "2. Temperature in K\n"
00281 "3. Altitude in m",
00282 Matrix_));
00283
00284 wsv_data.push_back
00285 (WsvRecord
00286 ("raw_vmrs",
00287 "The individual VMR profiles. Each species VMR profile comes with a\n"
00288 "pressure profile. The different species can hence be on different\n"
00289 "grids.\n"
00290 "The matrix has rows:\n"
00291 "1. Pressure in Pa\n"
00292 "2. VMR profile (absolute number)\n"
00293 "The array dimension is determined by the number of tag groups.",
00294 ArrayOfMatrix_));
00295
00296
00297
00298
00299 wsv_data.push_back
00300 (WsvRecord
00301 ("p_abs",
00302 "The pressure grid for the absorption coefficients [Pa]. This\n"
00303 "is the basic independent grid for the absorption calculation, both\n"
00304 "in the 1D and 2D case. Therefore it remains a vector, even in 2D.\n"
00305 "The \"raw\" atmospheric data shall be interpolated to p_abs before\n"
00306 "the absorption calculations starts.",
00307 Vector_));
00308
00309 wsv_data.push_back
00310 (WsvRecord
00311 ("f_mono",
00312 "The monochromatic frequency grid [Hz]. ",
00313 Vector_));
00314
00315
00316
00317
00318 wsv_data.push_back
00319 (WsvRecord
00320 ("t_abs",
00321 "Temperature associated with the pressures in p_abs [K]",
00322 Vector_));
00323
00324 wsv_data.push_back
00325 (WsvRecord
00326 ("z_abs",
00327 "Vertical altitudes associated with the pressures in p_abs [m]",
00328 Vector_));
00329
00330 wsv_data.push_back
00331 (WsvRecord
00332 ("h2o_abs",
00333 "The total water profile associated with the pressures in p_abs [-]",
00334 Vector_));
00335
00336 wsv_data.push_back
00337 (WsvRecord
00338 ("n2_abs",
00339 "The total nitrogen profile associated with the pressures in p_abs [-]",
00340 Vector_));
00341
00342 wsv_data.push_back
00343 (WsvRecord
00344 ("vmrs",
00345 "The VMRs (unit: absolute number) on the p_abs grid.\n"
00346 "Dimensions: [tag_groups.nelem(), p_abs.nelem()]",
00347 Matrix_));
00348
00349 wsv_data.push_back
00350 (WsvRecord
00351 ("abs",
00352 "The matrix of absorption coefficients (in units of [1/m]).\n"
00353 "Dimensions: [f_mono.nelem(), p_abs.nelem()]",
00354 Matrix_));
00355
00356 wsv_data.push_back
00357 (WsvRecord
00358 ("abs0",
00359 "A second absoprtion matrix. This matrix can be used, for example,\n"
00360 "to store absorption read from a file that shall be added to *abs*.",
00361 Matrix_));
00362
00363 wsv_data.push_back
00364 (WsvRecord
00365 ("abs_per_tg",
00366 "These are the absorption coefficients individually for each\n"
00367 "tag group. The Array contains one matrix for each tag group,\n"
00368 "the matrix format is the same as that of abs",
00369 ArrayOfMatrix_));
00370
00371 wsv_data.push_back
00372 (WsvRecord
00373 ("xsec_per_tg",
00374 "These are the cross sections individually for each tag\n"
00375 "group. The Array contains one matrix for each tag group,\n"
00376 "the matrix format is the same as that of abs",
00377 ArrayOfMatrix_));
00378
00379
00380
00381
00382 wsv_data.push_back
00383 (WsvRecord
00384 ("hse",
00385 "This vector holds the parameters for calculating hydrostatic \n"
00386 "equilibrium (HSE). The length of the vector is either 1 or 5, where\n"
00387 "the values are: \n "
00388 " 1: On/off flag. 0 = ignore HSE, 1 = consider HSE.\n "
00389 " 2: The pressure of the reference point [Pa]. \n "
00390 " 3: The altitude of the reference point [m]. \n "
00391 " 4: Gravitational acceleration at the geoid surface [m/s2]. \n "
00392 " 5: Number of iterations of the calculations.\n"
00393 "If the on/off flag is set to 1, the length of the vector must be 5,\n"
00394 "while if the flag is 0 a length of 1 is OK.\n"
00395 "See the function hseCalc for some more details.",
00396 Vector_));
00397
00398
00399
00400
00401
00402 wsv_data.push_back
00403 (WsvRecord
00404 ("emission",
00405 "Boolean to include emssion in the calculation of spectra.\n"
00406 "If this variable is set to 0 (zero) pure transmission calculations \n"
00407 "will be simulated and, for example, yCalc will give optical \n"
00408 "thicknesses instead of radiation intensities.",
00409 Index_));
00410
00411 wsv_data.push_back
00412 (WsvRecord
00413 ("za_pencil",
00414 "Pencil beam zenith angle grid [deg]. \n"
00415 "The observation direction is specified by the angle between zenith \n"
00416 "and the LOS.",
00417 Vector_));
00418
00419 wsv_data.push_back
00420 (WsvRecord
00421 ("z_tan",
00422 "Tangent altitude for each spectrum [m].\n"
00423 "These tangent altitudes include the effect of refraction (if set). \n"
00424 "In the case of a ground intersection, a geometrical prolongation \n"
00425 "below the ground is applied to determine the tangent altitude. \n"
00426 "For upward observations where there are no tangent altitudes, \n"
00427 "*z_tan* is set to 999 km. \n"
00428 "It should be noted that the LOS calculations take *za_pencil* as \n"
00429 "input, not *z_tan*. However, *za_pencil* can be calculated from \n"
00430 "*z_tan* by the function *zaFromZtan*. ",
00431 Vector_));
00432
00433 wsv_data.push_back
00434 (WsvRecord
00435 ("z_plat",
00436 "Vertical altitude, above the geoid, of the observation platform [m].",
00437 Numeric_));
00438
00439 wsv_data.push_back
00440 (WsvRecord
00441 ("l_step",
00442 "The maximum length, along the LOS, between the points of LOS [m].\n"
00443 "The final step length will in most cases equal the selected length.\n"
00444 "There are two rare exceptions:\n"
00445 " 1. Downward observations from within the atmosphere, where the step\n"
00446 " length is adjusted downwards to get an integer number of steps\n"
00447 " between the sensor and the tangent or ground point.\n"
00448 " 2. Limb sounding and the distance from the tangent point to the\n"
00449 " atmospheric limit (the highest absorption altitude) is smaller\n"
00450 " than the selected length. The length is then adjusted to this\n"
00451 " distance",
00452 Numeric_));
00453
00454 wsv_data.push_back
00455 (WsvRecord
00456 ("refr",
00457 "Boolean for inclusion of refraction (0=no refraction, 1=refraction).",
00458 Index_));
00459
00460 wsv_data.push_back
00461 (WsvRecord
00462 ("refr_lfac",
00463 "This factor determines the step length used during the ray tracing \n"
00464 "performed when considering refraction. \n"
00465 "The step length applied is *l_step* divided by *refr_lfac*. \n"
00466 "Accordingly, this factor gives how many ray tracing steps that are \n"
00467 "performed for each step of the LOS.",
00468 Index_));
00469
00470 wsv_data.push_back
00471 (WsvRecord
00472 ("refr_model",
00473 "A string giving what parameterization to use for the calculation of \n"
00474 "refractive index. See *refrCalc* for existing choices.",
00475 String_));
00476
00477 wsv_data.push_back
00478 (WsvRecord
00479 ("refr_index",
00480 "The refractive index at the pressure levels in p_abs [-].\n",
00481 Vector_));
00482
00483 wsv_data.push_back
00484 (WsvRecord
00485 ("r_geoid",
00486 "The local curvature radius of the geoid along the LOS [m].",
00487 Numeric_));
00488
00489 wsv_data.push_back
00490 (WsvRecord
00491 ("z_ground",
00492 "The vertical altitude above the geoid of the ground [m].",
00493 Numeric_));
00494
00495 wsv_data.push_back
00496 (WsvRecord
00497 ("t_ground",
00498 "The physical temperature of the ground [K].",
00499 Numeric_));
00500
00501 wsv_data.push_back
00502 (WsvRecord
00503 ("e_ground",
00504 "The ground emission factor for the frequencies in f_mono [0-1].",
00505 Vector_));
00506
00507 wsv_data.push_back
00508 (WsvRecord
00509 ("los",
00510 "Structure to define the line of sight (LOS). See los.h for \n"
00511 "definition of the structure.",
00512 Los_));
00513
00514 wsv_data.push_back
00515 (WsvRecord
00516 ("source",
00517 "Mean source function between the points of the LOS.",
00518 ArrayOfMatrix_));
00519
00520 wsv_data.push_back
00521 (WsvRecord
00522 ("trans",
00523 "The transmissions between the points of the LOS [-].",
00524 ArrayOfMatrix_));
00525
00526 wsv_data.push_back
00527 (WsvRecord
00528 ("y_space",
00529 "Radiation entering the atmosphere at the top of the atmosphere, \n"
00530 "typically cosmic background radiation. This variable is most easily \n"
00531 "set by the function *y_spaceStd*.",
00532 Vector_));
00533
00534 wsv_data.push_back
00535 (WsvRecord
00536 ("y",
00537 "The working set of spectra. \n"
00538 "The spectra from the different zenith angles are appended to form *y*.",
00539 Vector_));
00540
00541 wsv_data.push_back
00542 (WsvRecord
00543 ("y0",
00544 "A reference spectrum. This variable can be used e.g. to save a copy\n"
00545 "of *y* or to compare the spectra before and after some operation(s).",
00546 Vector_));
00547
00548 wsv_data.push_back
00549 (WsvRecord
00550 ("h",
00551 "The H matrix.\n"
00552 "\n"
00553 "Can be used to apply the sensor model to monochromatic pencil beam\n"
00554 "spectra and weighting functions. \n",
00555 Matrix_));
00556
00557
00558
00559
00560 wsv_data.push_back
00561 (WsvRecord
00562 ("absloswfs",
00563 "Line of sight weighting functions. \n"
00564 "See AUG for definition of this quantity. ",
00565 ArrayOfMatrix_));
00566
00567 wsv_data.push_back
00568 (WsvRecord
00569 ("k_grid",
00570 "Retrieval grid to be used in calculation of weighting functions (WFs)\n"
00571 "For example, *k_grid* is the pressure altitude grid for species WFs. \n"
00572 "Not all WFs need 'k_grid* as input.",
00573 Vector_));
00574
00575 wsv_data.push_back
00576 (WsvRecord
00577 ("k",
00578 "The weighting functions (WFs) for a single retrieval/error group.",
00579 Matrix_));
00580
00581 wsv_data.push_back
00582 (WsvRecord
00583 ("k_names",
00584 "Names of the retrieval identies in *k*.",
00585 ArrayOfString_));
00586
00587 wsv_data.push_back
00588 (WsvRecord
00589 ("k_aux",
00590 "Auxiliary data for *k*. The number of rows of this matrix equals the\n"
00591 "length of the state vector for the retrieval group (the number of\n"
00592 "columns of k).\n"
00593 "The columns hold different quantities:\n"
00594 " Col 1: retrieval grid (or correspondingly)\n"
00595 " Col 2: a priori values",
00596 Matrix_));
00597
00598 wsv_data.push_back
00599 (WsvRecord
00600 ("kx",
00601 "The state weighting function matrix.",
00602 Matrix_));
00603
00604 wsv_data.push_back
00605 (WsvRecord
00606 ("kx_names",
00607 "Names of the retrieval identities in *kx*.",
00608 ArrayOfString_));
00609
00610 wsv_data.push_back
00611 (WsvRecord
00612 ("kx_lengths",
00613 "The length of the state vector for each retrieval identity in *kx*.",
00614 ArrayOfIndex_));
00615
00616 wsv_data.push_back
00617 (WsvRecord
00618 ("kx_aux",
00619 "Auxiliary data for *kx*. As *k_aux* but with the data of the \n"
00620 "different retrieval groups appended vertically.",
00621 Matrix_));
00622
00623 wsv_data.push_back
00624 (WsvRecord
00625 ("kb",
00626 "The model parameters weighting function matrix.",
00627 Matrix_));
00628
00629 wsv_data.push_back
00630 (WsvRecord
00631 ("kb_names",
00632 "Names of the model parameter identities in *kb*.",
00633 ArrayOfString_));
00634
00635 wsv_data.push_back
00636 (WsvRecord
00637 ("kb_lengths",
00638 "The length of the model vector for each retrieval identity in *kb*.",
00639 ArrayOfIndex_));
00640
00641 wsv_data.push_back
00642 (WsvRecord
00643 ("kb_aux",
00644 "Auxiliary data for *kb*. As *k_aux* but with the data of the \n"
00645 "different forward model groups appended vertically.",
00646 Matrix_));
00647
00648 wsv_data.push_back
00649 (WsvRecord
00650 ("S_S",
00651 "Stores the accuracy of the spectroscopic parameters read from catalog\n"
00652 "This are necessary for the the spectroscopic error analysis\n"
00653 "number columns = 2; first keeps the absolute error, second the error in percents\n"
00654 "number lines equal of spectroscopic parameters investigated (the number of\n"
00655 "columns of k).",
00656 Matrix_));
00657
00658
00659
00660
00661
00662
00663
00664
00665
00666
00667
00668
00669
00670 wsv_data.push_back
00671 (WsvRecord
00672 ("batchname",
00673 "Default basename for batch data.",
00674 String_));
00675
00676 wsv_data.push_back
00677 (WsvRecord
00678 ("ybatch",
00679 "A batch of spectra.\n"
00680 "The spectra are stored as columns in a matrix",
00681 Matrix_));
00682
00683 wsv_data.push_back
00684 (WsvRecord
00685 ("absbatch",
00686 "A batch of absorption coefficients.\n"
00687 "FIXME",
00688 ArrayOfMatrix_));
00689
00690 wsv_data.push_back
00691 (WsvRecord
00692 ("jacbatch",
00693 "A batch of jacobian matrices.\n"
00694 "FIXME",
00695 ArrayOfMatrix_));
00696
00697
00698 wsv_data.push_back
00699 (WsvRecord
00700 ("radiosonde_data",
00701 "An array of Matrix holding data for many radiosonde launches. The\n"
00702 "dimension of the Array is the number of radiosonde launches. Each\n"
00703 "Matrix within the Array has dimension nx4, where n is the number of\n"
00704 "pressure levels. The columns of the Matrix are:\n"
00705 "\n"
00706 "pressure [Pa] temperature [K] altitude [m] VMR [1]",
00707 ArrayOfMatrix_));
00708
00709
00710
00711
00712 wsv_data.push_back
00713 (WsvRecord
00714 ("coolrate",
00715 "Cooling rate matrix, in unit of K/s/Hz."
00716 "Dimensions: [f_mono.nelem(), z_crates.nelem()]",
00717 Matrix_));
00718
00719 wsv_data.push_back
00720 (WsvRecord
00721 ("p_coolrate",
00722 "Pressures for which to calculate cooling rates.",
00723 Vector_));
00724
00725
00726
00727
00728 wsv_data.push_back
00729 (WsvRecord
00730 ("method_list",
00731 "A list of methods. See \"arts -d MethodListDefine\"\n"
00732 "for an explanation what a method list is.",
00733 ArrayOfIndex_));
00734
00735 }