J/MNRAS/520/4582ivo://CDS.VizieR/J/MNRAS/520/4582doi:10.26093/cds/vizier/bg-g8-4f6CDSPosselt B.Karastergiou A.Johnston S.Parthasarathy A.Oswald L.S.,Main R.A.Basu A.Keith M.J.Song X.Weltevrede P.Tiburzi C.,Bailes M.Buchner S.Geyer M.Kramer M.Spiewak R.,Venkatraman Krishnan V.2026-08-03T07:32:45Z2026-04-27T11:06:10ZCDS support team

CDS, Observatoire de Strasbourg, 11 rue de l'Universite, F-67000 Strasbourg, France

cds-question@unistra.frpulsarsvariable-starsinterferometryphotometryspectroscopypolarimetryradio-sourcesgalaxy-kinematicsWe present the largest single survey to date of average profiles of radio pulsars, observed and processed using the same telescope and data reduction software. Specifically, we present measurements for 1170 pulsars, observed by the Thousand Pulsar Array programme at the 64-dish SARAO MeerKAT radio telescope, in a frequency band from 856 to 1712 MHz. We provide rotation measures (RM), dispersion measures, flux densities, and polarization properties. The catalogue includes 254 new RMs that substantially increase the total number of known pulsar RMs. Our integration times typically span over 1000 individual rotations per source. We show that the radio (pseudo-) luminosity has a strong, shallow dependence on the spin-down energy, proportional to dE/dt^0.15+/-0.04^, that contradicts some previous proposals of population synthesis studies. In addition, we find a significant correlation between the steepness of the observed flux density spectra and dE/dt, and correlations of the fractional linear polarization with dE/dt, the spectral index, and the pulse width, which we discuss in the context of what is known about pulsar radio emission and how pulsars evolve with time. On the whole, we do not see significant correlations with the estimated surface magnetic field strength, and the correlations with dE/dt are much stronger than those with the characteristic age. This finding lends support to the suggestion that magnetic dipole braking may not be the dominant factor for the evolution of pulsar rotation over the lifetimes of pulsars. A public data release of the high-fidelity time-averaged pulse profiles in full polarization accompanies our catalogue.2023MNRAS.520.4582Phttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/MNRAS/520/4582CatalogResearchIsServedByTAP VizieR generic serviceIsServedByConesearch servicerelated-toJ/MNRAS/508/4249 : TPA radio pulsars with MeerKAT (Posselt+, 2021)J/MNRAS/473/4436 : Spectral properties of 441 radio pulsars (Jankowski+, 2018)J/MNRAS/391/1210 : Characteristics of energetic pulsars (Weltevrede+, 2008)J/MNRAS/386/1881 : New pulsar rotation measures (Noutsos+, 2008)J/MNRAS/273/411 : Multifrequency fluxes of 280 pulsars (Lorimer+ 1995)J/ApJS/208/17 : 2nd Fermi LAT cat. of gamma-ray pulsars (2PC) (Abdo+, 2013)B/psr : ATNF Pulsar Catalogue (Manchester+, 2005)https://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/MNRAS/520/4582https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/MNRAS/520/4582http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/MNRAS/520/4582https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/MNRAS/520/4582https://vizier.iucaa.in/viz-bin/votable?-source=J/MNRAS/520/4582http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/MNRAS/520/4582GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapCone search capability for table J/MNRAS/520/4582/table1 (The general properties of the TPA pulsars and their census observations)https://vizier.cds.unistra.fr/viz-bin/conesearch/J/MNRAS/520/4582/table1?https://vizier.iucaa.in/viz-bin/conesearch/J/MNRAS/520/4582/table1?http://vizieridia.saao.ac.za/viz-bin/conesearch/J/MNRAS/520/4582/table1?GETtext/xml+votable180.050000true8.537125-7.36552780.0055555555555555565/7203 7294 7381 7383 7555 7561 7564 7648-7649 7651 7654 7675 7678 10419 10556-10557 6/426 781 4163 4227 4403 4556 4584 4608 8192 8277 8539 8644 8676 8714 8964 9240 12441 12500 12513 12526 12539 12565 12586 12719 12747 12754 12847 12870 12911-12912 12939 12960-12961 12964 12967 12970-12971 12974 12987 12990-12991 12993 13088 13191 13316 14336 14339 14341-14342 14345-14346 14352 14355 14360 16676 16996 17247 17378 17450 17532 18421 18830 19421 19438 20096 20166 20171 20574 20767 20883 21016 21171 21455 21504 21515 21519 21957 22058 22071 22118 22174 22205-22206 22255 22271 22426 22442 22594 22765 22917 22996 23620 23622 23640 23646 23727 23830 23952 23994 24040 24262 24360 24708 24717 25114 25251 25732 25763 26520 26656 27554 28108 28135 28226 28692 28711 28716 28724-28725 28730 28735 28749 28771 28806-28809 28816 28818 28825-28826 28830-28833 28843 28847 28849 28851 28860 28864 28869 28872 28878-28879 28886 28890 28896 28900-28901 28913 28915 28919 28921 28945-28946 29055 29063 29079 29082 29089-29090 29096-29098 29100-29101 29103 29106 29108 29112-29113 29115 29118 29135 29145 29157 29162 29165 29172 29174 29180 29205 29261 29267-29269 29303 29334 29340 29369 29383 29387 29390 29422 29436 29441 29447 29458-29459 29461 29465 29477 29483 29487 29495 29504-29505 29510-29511 29516 29518 29521-29523 29528-29530 29538 29541 29550-29551 29556 29559-29560 29569 29591 29615 29617 29625 29639 29652-29653 29675 29680 29692 29696 29727 29746 29768 29789 29833 29840 29846 29860 29862-29863 29865 29883 29897 29929 29961 30102 30119 30127 30208 30210-30211 30215 30217-30219 30227 30234 30240-30242 30252-30253 30260 30264-30265 30267-30269 30273 30280-30281 30298 30300 30303 30306 30309 30311 30313-30317 30319 30322 30325-30326 30328 30330-30333 30335 30338-30339 30347-30349 30357 30359 30361-30362 30364 30368 30370 30394 30400-30401 30407 30409 30412-30414 30416-30418 30420 30422-30425 30428-30430 30449 30451-30453 30457 30461 30493 30501 30506 30517 30521 30525 30541 30548 30564 30572 30577 30579 30582 30591 30600-30601 30603 30609-30610 30613 30622 30624 30631 30641 30643-30646 30651-30652 30657 30662 30664 30669 30671 30675 30682-30683 30689-30691 30693-30694 30696-30697 30705 30708 30711 30716 30719 30781 30784 30871 30941 31031 31049 31058 31078 31244 31251 31344 31591 31623 31717 31745 31751 31775 31809 31811 31829 31842 31851 31859 31864 31870 31873 31898 31933 32007 32010 32014 32024 32027 32029 32039-32040 32048 32058 32069 32077 32079-32080 32085-32087 32116 32121 32127 32140 32161 32194 32218 32452 32546 32548 32824 32888 33030 33047 33073 33075-33076 33089 33095 33098-33099 33112-33113 33127 33137 33145 33294 33299 33306 33325 33328 33333 33730 34107 34393 34680 35229 35691 35925 36540 36946 36948 36952 37062 37082 37175 37193-37194 37203 37207 37210 37215 37224 37227 37229 37232 37235 37240 37244 37260 37317 37322 37331-37332 37338-37339 37341 37351 37360-37361 37364-37365 37374-37375 37638 37643 37646 37651 37658 37701 37704 37714 37717 37721 37726 37744-37746 37758 37787 37801 37828 37830 37848 37858 37863-37864 37873-37874 37876 37884 37892 37895 37898 37900-37901 37903-37905 37908-37910 37915 37919 37921 37923-37924 37929-37931 37933 37937 37946 37948 37953 37957-37958 37963 37967 37976 37984 37990 38017-38018 38020 38040 38048-38049 38060 38068 38081 38102 38113 38152 38179 38193 38250 38402 38406 38425 38428 38436 38550 38568 38586 38597 38711 38756 38891 38935 38975 39216 39235 39243 39247 39250 39269 39272 39275 39280 39294 39299 39311 39342 39364 39367-39369 39389 39395 39414 39473 39789 39886 39907 39921 39925 39977 39992 40016 40104 40124 40127 40238 40366 40432 40667 40680 41118 41143 41212 41258 41271 41343 41365 41373 41386 41400-41401 41431 41436 41442 41454-41455 41457 41460 41464 41466 41468 41485 41535 41539-41540 41549 41561 41567 41569 41578 41583-41585 41593-41595 41597 41607 41615 41619 41625 41628 41630 41632 41642 41647 41650 41653-41657 41660 41665 41672-41674 41681-41686 41689 41695-41697 41701 41704 41710-41713 41719 41727 41736 41743-41744 41747 41753 41755-41758 41762 41765-41766 41768-41769 41771 41773 41778 41781-41782 41789 41793 41798-41800 41802-41806 41809 41811 41814-41816 41818-41821 41828-41830 41833 41840 41844 41857 41859 41865 41870-41871 41894 41909 41916 41939 41949 42019 42038 42070 42076 42092 42094 42124 42126 42143 42146-42147 42150 42155 42157 42159 42162 42165 42169 42171-42173 42178 42185 42187 42189 42193-42194 42196 42206 42208-42209 42213-42214 42216 42218 42220 42223 42232-42233 42236 42269 42284 42288 42296 42300-42301 42306 42328 42341 42346 42351 42353-42354 42356-42357 42366-42368 42371 42374 42378-42380 42382-42386 42389 42391 42396-42398 42401 42405 42414 42420 42422 42424-42425 42429 42432-42433 42435 42438 42442 42445 42450-42451 42456-42457 42468 42472 42477 42481 42487 42496 42499 42503-42504 42510 42513 42515 42524 42528-42529 42531 42533 42551 42560-42562 42576-42577 42583 42585 42592 42595 42612 42635 42640 42651-42652 42654 42658 42674 42676 42709 42726 42757 42763 42772 42821 42825 42829 42832 42834 42914 42937 42951 43012-43013 43017 43019-43020 43022 43024-43025 43040 43044 43060 43065 43073 43075 43080 43107 43110 43113 43122 43125 43137 43140 43144 43149 43169 43182 43195-43196 43219 43223 43245 43253 43261 43272-43273 43304 43366 43460 43546 43571 43671 43747 43820 43882 43992 44308 44316 44923 45198 45219 45285 45478 46095 46787 47010 47022 47244 47275 47484 47649 47759 47803 47885 47975 47998 48025 48080 48158 48609 48928 49129https://cdsarc.cds.unistra.fr/viz-bin/moc/J/MNRAS/520/4582?format=asciiRadiodefaultJ/MNRAS/520/4582/table1The general properties of the TPA pulsars and their census observationsrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintPSRPulsar name designation as JHHMM+/-DDMM (PSRJ)meta.id;meta.maincharprimarySimbadNameSimbad column added by the CDSmeta.idcharnullableATNFDisplay the ATNF pulsar catalogue from Manchester et al. 2005AJ....129.1993M, Cat. B/psrmeta.ref.urlintnullablePRotation period of the pulsar (P)stime.periodfloatlogdE/dt? The logarithm of the spin-down energy loss rate (logEdot)1e-07Wphys.energyfloatnullableMJDThe modified Julian date of the census pulsar observation (MJD)dtime.epochfloattobsThe TPA census observing time corrected from radio frequency interference RFI (t_obs_)stime.expointtnom? The nominal optimal observing lengths t_nom_ according to Song et al. (2021MNRAS.505.4456S) (t_norm_)stime.expointnullableRMSIJ/MNRAS/520/4582/table2The 254 newly measured RMs and uncertainties explained in section 3.2recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintPSRPulsar name designation as JHHMM+/-DDMM (PSRJ)meta.id;meta.maincharRMRotation measure as explained in sections 2.3 and 3 (RM)rad.m**-2phys.polarization.rotMeasurefloate_RMThe 1{sigma} estimated error of RM ({sigma}_RM_)rad.m**-2stat.errorfloatJ/MNRAS/520/4582/table5Properties of the TPA census of pulsars used for weighted PL-fits to derive spectral indicesnutThe frequency of the frequency-averaged at which the continuum-equivalent fluxes Ft are obtained ({nu}_t_)MHzem.freq;em.radio.750-1500MHzintnu6? The frequency of channel 6 processed with PTUSE at which the continuum-equivalent fluxes Fch6 are obtained ({nu}_6_)MHzem.freq;em.radio.750-1500MHzintnullableFch6? The continuum-equivalent flux measured in the frequency channel 6 {nu}_6_ (F_ch6_)mJyphot.flux.density;em.radio.750-1500MHzdoublenullablerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintFtThe continuum-equivalent flux measured in the frequency-averaged total power profile (F_t_)mJyphot.flux.density;em.radio.750-1500MHzdoublee_FtThe 1{sigma} estimated error of Ft ({sigma}_Ft_)mJystat.errorfloatlogL? The calculated pseudo-luminosity in MeerKAT L-band in same way as equation 2 of section 2.4 (logL_L_)log(1e-07W)phys.luminosityfloatnullablenu1? The frequency of channel 1 processed with PTUSE at which the continuum-equivalent fluxes Fch1 are obtained ({nu}_1_)MHzem.freq;em.radio.750-1500MHzintnullableFch1? The continuum-equivalent flux measured in the frequency channel 1 {nu}_1_ (F_ch1_)mJyphot.flux.density;em.radio.750-1500MHzdoublenullablee_Fch1? The 1{sigma} estimated error of Fch1 ({sigma}_Fch1_)mJystat.errorfloatnullablenu2? The frequency of channel 2 processed with PTUSE at which the continuum-equivalent fluxes Fch2 are obtained ({nu}_2_)MHzem.freq;em.radio.750-1500MHzintnullableFch2? The continuum-equivalent flux measured in the frequency channel 2 {nu}_2_ (F_ch2_)mJyphot.flux.density;em.radio.750-1500MHzdoublenullablee_Fch2? The 1{sigma} estimated error of Fch2 ({sigma}_Fch2_)mJystat.errorfloatnullablenu3? The frequency of channel 3 processed with PTUSE at which the continuum-equivalent fluxes Fch3 are obtained ({nu}_3_)MHzem.freq;em.radio.750-1500MHzintnullableFch3? The continuum-equivalent flux measured in the frequency channel 3 {nu}_3_ (F_ch3_)mJyphot.flux.density;em.radio.750-1500MHzdoublenullablee_Fch3? The 1{sigma} estimated error of Fch3 ({sigma}_Fch3_)mJystat.errorfloatnullablenu4? The frequency of channel 4 processed with PTUSE at which the continuum-equivalent fluxes Fch4 are obtained ({nu}_4_)MHzem.freq;em.radio.750-1500MHzintnullableFch4? The continuum-equivalent flux measured in the frequency channel 4 {nu}_4_ (F_ch4_)mJyphot.flux.density;em.radio.750-1500MHzdoublenullablee_Fch4? The 1{sigma} estimated error of Fch4 ({sigma}_Fch4_)mJystat.errorfloatnullablenu5? The frequency of channel 5 processed with PTUSE at which the continuum-equivalent fluxes Fch5 are obtained ({nu}_5_)MHzem.freq;em.radio.750-1500MHzintnullableFch5? The continuum-equivalent flux measured in the frequency channel 5 {nu}_5_ (F_ch5_)mJyphot.flux.density;em.radio.750-1500MHzdoublenullablee_Fch5? The 1{sigma} estimated error of Fch5 ({sigma}_Fch5_)mJystat.errorfloatnullablee_Fch6? The 1{sigma} estimated error of Fch6 ({sigma}_Fch6_)mJystat.errorfloatnullablenu7? The frequency of channel 7 processed with PTUSE at which the continuum-equivalent fluxes Fch7 are obtained ({nu}_7_)MHzem.freq;em.radio.750-1500MHzintnullableFch7? The continuum-equivalent flux measured in the frequency channel 7 {nu}_7_ (F_ch7_)mJyphot.flux.density;em.radio.750-1500MHzdoublenullablee_Fch7? The 1{sigma} estimated error of Fch7 ({sigma}_Fch7_)mJystat.errorfloatnullablenu8? The frequency of channel 8 processed with PTUSE at which the continuum-equivalent fluxes Fch8 are obtained ({nu}_8_)MHzem.freq;em.radio.1500-3000MHzintnullableFch8? The continuum-equivalent flux measured in the frequency channel 8 {nu}_8_ (F_ch8_)mJyphot.flux.density;em.radio.1500-3000MHzdoublenullablee_Fch8? The 1{sigma} estimated error of Fch8 ({sigma}_Fch8_)mJystat.errorfloatnullableSI? The spectral index derived from our weighted PL-fits (SI)spect.index;meta.modelledfloatnullablee_SI? The 1{sigma} estimated error of SI ({sigma}_SI_)stat.errorfloatnullablemSI? The pseudo-modulation index defined in equation 3 of section 2.4 and indicating the scatter around the PL-fit (m_SI_)spect.index;meta.modelledfloatnullablePSRPulsar name designation as JHHMM+/-DDMM (PSRJ)meta.id;meta.maincharJ/MNRAS/520/4582/table6The polarization fraction measurements in frequency-averaged and set of the 8 frequency channels data of the TPA census pulsars with well determined RMe_L/I3? The 1{sigma} estimated error of L/I3 (ch3delfracLPtrueI)stat.errorfloatnullablee_V/I7? The 1{sigma} estimated error of V/I7 (ch7delfracVI)stat.errorfloatnullablerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintPSRPulsar name designation as JHHMM+/-DDMM (PSRJ)meta.id;meta.maincharL/ItThe debiased linear polarization fraction LFP for the frequency-averaged data (TfracLPtrueI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloate_L/ItThe 1{sigma} estimated error of L/It (TdelfracLPtrueI) (1)stat.errorfloatL*/ItThe debiased vector-added linear polarization L*PF fraction for the frequency-averaged data (TfracLPvecI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloate_L*/ItThe 1{sigma} estimated error of L*/It (TdelfracLPvecI) (1)stat.errorfloatV/ItThe debiased circular polarization fraction CPF for the frequency-averaged data (TfracVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloate_V/ItThe 1{sigma} estimated error of V/It (TdelfracVI) (1)stat.errorfloatVabs/ItThe debiased absolute circular polarization fraction aCPF for the frequency-averaged data (TfracabsVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatLP30t? Percentage fraction of the pulse that have linear polarization LP above 30 per cent for the frequency-averaged data (PFLP30)%stat.fit.paramintnullablee_LP30t[]? Lower 1{sigma} statistical uncertainty of LP30t (PFLP30_minusSigma) (2)%stat.errorintnullableE_LP30t? Upper 1{sigma} statistical uncertainty of LP30t (PFLP30_plusSigma) (2)%stat.error;stat.maxintnullableLP60t? Percentage fraction of the pulse that have linear polarization LP above 60 per cent for the frequency-averaged data (PFLP60)%stat.fit.paramintnullablee_LP60t[]? Lower 1{sigma} statistical uncertainty of LP60t (PFLP60_minusSigma) (2)%stat.errorintnullableE_LP60t? Upper 1{sigma} statistical uncertainty of LP60t (PFLP60_plusSigma) (2)%stat.error;stat.maxintnullableLP90t? Percentage fraction of the pulse that have linear polarization LP above 90 per cent for the frequency-averaged data (PFLP90)%stat.fit.paramintnullablee_LP90t[]? Lower 1{sigma} statistical uncertainty of LP90t (PFLP90_minusSigma) (2)%stat.errorintnullableE_LP90t? Upper 1{sigma} statistical uncertainty of LP90t (PFLP90_plusSigma) (2)%stat.error;stat.maxintnullableaCP10? Percentage fraction of the pulse that have absolute circular polarization aCP above 10 per cent for the frequency-averaged data (PFaCP10)%stat.fit.paramintnullablee_aCP10[]? Lower 1{sigma} statistical uncertainty of aCP10 (PFaCP10_minusSigma) (2)%stat.errorintnullableE_aCP10? Upper 1{sigma} statistical uncertainty of aCP10 (PFaCP10_plusSigma) (2)%stat.error;stat.maxintnullableaCP25? Percentage fraction of the pulse that have absolute circular polarization aCP above 25 per cent for the frequency-averaged data (PFaCP25)%stat.fit.paramintnullablee_aCP25[]? Lower 1{sigma} statistical uncertainty of aCP25 (PFaCP25_minusSigma) (2)%stat.errorintnullableE_aCP25? Upper 1{sigma} statistical uncertainty of aCP25 (PFaCP25_plusSigma) (2)%stat.error;stat.maxintnullableaCP40? Percentage fraction of the pulse that have absolute circular polarization aCP above 40 per cent for the frequency-averaged data (PFaCP40)%stat.fit.paramintnullablee_aCP40[]? Lower 1{sigma} statistical uncertainty of aCP40 (PFaCP40_minusSigma) (2)%stat.errorintnullableE_aCP40? Upper 1{sigma} statistical uncertainty of aCP40 (PFaCP40_plusSigma) (2)%stat.error;stat.maxintnullableL/I1? The debiased linear polarization fraction LFP for the frequency channel 1 (ch1fracLPtrueI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L/I1? The 1{sigma} estimated error of L/I1 (ch1delfracLPtrueI)stat.errorfloatnullableL*/I1? The debiased vector-added linear polarization L*PF fraction for the frequency channel 1 (ch1fracLPvecI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L*/I1? The 1{sigma} estimated error of L*/I1 (ch1delfracLPvecI)stat.errorfloatnullableV/I1? The debiased circular polarization fraction CPF for the frequency channel 1 (ch1fracVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_V/I1? The 1{sigma} estimated error of V/I1 (ch1delfracVI)stat.errorfloatnullableVabs/I1? The debiased absolute circular polarization fraction aCPF for the frequency channel 1 (ch1fracabsVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullableL/I2? The debiased linear polarization fraction LFP for the frequency channel 2 (ch2fracLPtrueI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L/I2? The 1{sigma} estimated error of L/I2 (ch2delfracLPtrueI)stat.errorfloatnullableL*/I2? The debiased vector-added linear polarization L*PF fraction for the frequency channel 2 (ch2fracLPvecI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L*/I2? The 1{sigma} estimated error of L*/I2 (ch2delfracLPvecI)stat.errorfloatnullableV/I2? The debiased circular polarization fraction CPF for the frequency channel 2 (ch2fracVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_V/I2? The 1{sigma} estimated error of V/I2 (ch2delfracVI)stat.errorfloatnullableVabs/I2? The debiased absolute circular polarization fraction aCPF for the frequency channel 2 (ch2fracabsVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullableL/I3? The debiased linear polarization fraction LFP for the frequency channel 3 (ch3fracLPtrueI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullableL*/I3? The debiased vector-added linear polarization L*PF fraction for the frequency channel 3 (ch3fracLPvecI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L*/I3? The 1{sigma} estimated error of L*/I3 (ch3delfracLPvecI)stat.errorfloatnullableV/I3? The debiased circular polarization fraction CPF for the frequency channel 3 (ch3fracVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_V/I3? The 1{sigma} estimated error of V/I3 (ch3delfracVI)stat.errorfloatnullableVabs/I3? The debiased absolute circular polarization fraction aCPF for the frequency channel 3 (ch3fracabsVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullableL/I4? The debiased linear polarization fraction LFP for the frequency channel 4 (ch4fracLPtrueI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L/I4? The 1{sigma} estimated error of L/I4 (ch4delfracLPtrueI)stat.errorfloatnullableL*/I4? The debiased vector-added linear polarization L*PF fraction for the frequency channel 4 (ch4fracLPvecI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L*/I4? The 1{sigma} estimated error of L*/I4 (ch4delfracLPvecI)stat.errorfloatnullableV/I4? The debiased circular polarization fraction CPF for the frequency channel 4 (ch4fracVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_V/I4? The 1{sigma} estimated error of V/I4 (ch4delfracVI)stat.errorfloatnullableVabs/I4? The debiased absolute circular polarization fraction aCPF for the frequency channel 4 (ch4fracabsVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullableL/I5? The debiased linear polarization fraction LFP for the frequency channel 5 (ch5fracLPtrueI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L/I5? The 1{sigma} estimated error of L/I5 (ch5delfracLPtrueI)stat.errorfloatnullableL*/I5? The debiased vector-added linear polarization L*PF fraction for the frequency channel 5 (ch5fracLPvecI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L*/I5? The 1{sigma} estimated error of L*/I5 (ch5delfracLPvecI)stat.errorfloatnullableV/I5? The debiased circular polarization fraction CPF for the frequency channel 5 (ch5fracVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_V/I5? The 1{sigma} estimated error of V/I5 (ch5delfracVI)stat.errorfloatnullableVabs/I5? The debiased absolute circular polarization fraction aCPF for the frequency channel 5 (ch5fracabsVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullableL/I6? The debiased linear polarization fraction LFP for the frequency channel 6 (ch6fracLPtrueI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L/I6? The 1{sigma} estimated error of L/I6 (ch6delfracLPtrueI)stat.errorfloatnullableL*/I6? The debiased vector-added linear polarization L*PF fraction for the frequency channel 6 (ch6fracLPvecI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L*/I6? The 1{sigma} estimated error of L*/I6 (ch6delfracLPvecI)stat.errorfloatnullableV/I6? The debiased circular polarization fraction CPF for the frequency channel 6 (ch6fracVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_V/I6? The 1{sigma} estimated error of V/I6 (ch6delfracVI)stat.errorfloatnullableVabs/I6? The debiased absolute circular polarization fraction aCPF for the frequency channel 6 (ch6fracabsVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullableL/I7? The debiased linear polarization fraction LFP for the frequency channel 7 (ch7fracLPtrueI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L/I7? The 1{sigma} estimated error of L/I7 (ch7delfracLPtrueI)stat.errorfloatnullableL*/I7? The debiased vector-added linear polarization L*PF fraction for the frequency channel 7 (ch7fracLPvecI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullablee_L*/I7? The 1{sigma} estimated error of L*/I7 (ch7delfracLPvecI)stat.errorfloatnullableV/I7? The debiased circular polarization fraction CPF for the frequency channel 7 (ch7fracVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullableVabs/I7? The debiased absolute circular polarization fraction aCPF for the frequency channel 7 (ch7fracabsVI)phot.flux.density;arith.ratio;em.radio.750-1500MHzfloatnullableL/I8? The debiased linear polarization fraction LFP for the frequency channel 8 (ch8fracLPtrueI)phot.flux.density;arith.ratio;em.radio.1500-3000MHzfloatnullablee_L/I8? The 1{sigma} estimated error of L/I8 (ch8delfracLPtrueI)stat.errorfloatnullableL*/I8? The debiased vector-added linear polarization L*PF fraction for the frequency channel 8 (ch8fracLPvecI)phot.flux.density;arith.ratio;em.radio.1500-3000MHzfloatnullablee_L*/I8? The 1{sigma} estimated error of L*/I8 (ch8delfracLPvecI)stat.errorfloatnullableV/I8? The debiased circular polarization fraction CPF for the frequency channel 8 (ch8fracVI)phot.flux.density;arith.ratio;em.radio.1500-3000MHzfloatnullablee_V/I8? The 1{sigma} estimated error of V/I8 (ch8delfracVI)stat.errorfloatnullableVabs/I8? The debiased absolute circular polarization fraction aCPF for the frequency channel 8 (ch8fracabsVI)phot.flux.density;arith.ratio;em.radio.1500-3000MHzfloatnullable