Aghanim, N; Akrami, Y; Ashdown, Mark Andrew; Aumont, J; Baccigalupi, C; Ballardini, M; Banday, AJ; Barreiro, RB; Bartolo, N; Basak, S; Benabed, K; Bersanelli, M; Bielewicz, P; Bonaldi, A; Bonavera, L; Bond, JR; Borrill, J; Bouchet, FR; Burigana, C; Calabrese, E; Cardoso, JF; Challinor, Anthony David; Chiang, HC; Colombo, LPL; Combet, C; Crill, BP; Curto, A; Cuttaia, F; De Bernardis, P; De Rosa, A; De Zotti, G; Delabrouille, J; Di Valentino, E; Dickinson, C; Diego, JM; Doré, O; Ducout, A; Dupac, X; Dusini, S; Efstathiou, George Petros; Elsner, F; Enßlin, TA; Eriksen, HK; Fantaye, Y; Finelli, F; Forastieri, F; Frailis, M; Franceschi, E; Frolov, A; Galeotta, S; Galli, S; Ganga, K; Génova-Santos, RT; Gerbino, M; González-Nuevo, J; Górski, KM; Gratton, S; Gruppuso, A; Gudmundsson, JE; Herranz, D; Hivon, E
The six parameters of the standard ΛCDM model have best-fit values derived from the Planck temperature power spectrum that are shifted somewhat from the best-fit values derived from WMAP data. These shifts are driven by ...
