Planckintermediate results
Authors:   Planck Collaboration, Akrami Y. , Ashdown M. , Aumont J. , Baccigalupi C. , Ballardini M. , Banday A. J. , Barreiro R. B. , Bartolo N. , Basak S. , Benabed K. , Bernard J.-P. , Bersanelli M. , Bielewicz P. , Bonavera L. , Bond J. R. , Borrill J. , Bouchet F. R. , Boulanger F. , Bucher M. , Burigana C. , Butler R. C. , Calabrese E. , Cardoso J.-F. , Carron J. , Chiang H. C. , Colombo L. P. L. , Comis B. , Couchot F. , Coulais A. , Crill B. P. , Curto A. , Cuttaia F. , de Bernardis P. , de Rosa A. , de Zotti G. , Delabrouille J. , Di Valentino E. , Dickinson C. , Diego J. M. , Doré O. , Ducout A. , Dupac X. , Elsner F. , Enßlin T. A. , Eriksen H. K. , Falgarone E. , Fantaye Y. , Finelli F. , Frailis M. , Fraisse A. A. , Franceschi E. , Frolov A. , Galeotta S. , Galli S. , Ganga K. , Génova-Santos R. T. , Gerbino M. , González-Nuevo J. , Górski K. M. , Gruppuso A. , Gudmundsson J. E. , Hansen F. K. , Helou G. , Henrot-Versillé S. , Herranz D. , Hivon E. , Jaffe A. H. , Jones W. C. , Keihänen E. , Keskitalo R. , Kiiveri K. , Kim J. , Kisner T. S. , Krachmalnicoff N. , Kunz M. , Kurki-Suonio H. , Lagache G. , Lamarre J.-M. , Lasenby A. , Lattanzi M. , Lawrence C. R. , Le Jeune M. , Lellouch E. , Levrier F. , Liguori M. , Lilje P. B. , Lindholm V. , López-Caniego M. , Ma Y.-Z. , Macías-Pérez J. F. , Maggio G. , Maino D. , Mandolesi N. , Maris M. , Martin P. G. , Martínez-González E. , Matarrese S. , Mauri N. , McEwen J. D. , Melchiorri A. , Mennella A. , Migliaccio M. , Miville-Deschênes M.-A. , Molinari D. , Moneti A. , Montier L. , Moreno R. , Morgante G. , Natoli P. , Oxborrow C. A. , Paoletti D. , Partridge B. , Patanchon G. , Patrizii L. , Perdereau O. , Piacentini F. , Plaszczynski S. , Polenta G. , Rachen J. P. , Racine B. , Reinecke M. , Remazeilles M. , Renzi A. , Rocha G. , Romelli E. , Rosset C. , Roudier G. , Rubiño-Martín J. A. , Ruiz-Granados B. , Salvati L. , Sandri M. , Savelainen M. , Scott D. , Sirri G. , Spencer L. D. , Suur-Uski A.-S. , Tauber J. A. , Tavagnacco D. , Tenti M. , Toffolatti L. , Tomasi M. , Tristram M. , Trombetti T. , Valiviita J. , Van Tent F. , Vielva P. , Villa F. , Wehus I. K. , Zacchei A. 
Published: April 2017

Measurements of flux density are described for five planets, Mars, Jupiter, Saturn, Uranus, and Neptune, across the sixPlanckHigh Frequency Instrument frequency bands (100–857 GHz) and these are then compared with models and existing data. In our analysis, we have also included estimates of the brightness of Jupiter and Saturn at the three frequencies of thePlanckLow Frequency Instrument (30, 44, and 70 GHz). The results provide constraints on the intrinsic brightness and the brightness time-variability of these planets. The majority of the planet flux density estimates are limited by systematic errors, but still yield better than 1% measurements in many cases. Applying data fromPlanckHFI, theWilkinsonMicrowave Anisotropy Probe (WMAP), and the Atacama Cosmology Telescope (ACT) to a model that incorporates contributions from Saturn’s rings to the planet’s total flux density suggests a best fit value for the spectral index of Saturn’s ring system ofβring= 2.30 ± 0.03 over the 30–1000 GHz frequency range. Estimates of the polarization amplitude of the planets have also been made in the four bands that have polarization-sensitive detectors (100–353 GHz); this analysis provides a 95% confidence level upper limit on Mars’s polarization of 1.8, 1.7, 1.2, and 1.7% at 100, 143, 217, and 353 GHz, respectively. The average ratio between thePlanck-HFI measurements and the adopted model predictions for all five planets (excluding Jupiter observations for 353 GHz) is 1.004, 1.002, 1.021, and 1.033 for 100, 143, 217, and 353 GHz, respectively. Model predictions for planet thermodynamic temperatures are therefore consistent with the absolute calibration ofPlanck-HFI detectors at about the three-percent level. We compare our measurements with published results from recent cosmic microwave background experiments. In particular, we observe that the flux densities measured byPlanckHFI and WMAP agree to within 2%. These results allow experiments operating in the mm-wavelength range to cross-calibrate againstPlanckand improve models of radiative transport used in planetary science.