- Main
Planck intermediate results
- Ade, PAR;
- Aghanim, N;
- Ashdown, M;
- Aumont, J;
- Baccigalupi, C;
- Banday, AJ;
- Barreiro, RB;
- Bartolo, N;
- Basak, S;
- Battaner, E;
- Benabed, K;
- Benoit-Lévy, A;
- Bernard, J-P;
- Bersanelli, M;
- Bielewicz, P;
- Bock, JJ;
- Bonaldi, A;
- Bonavera, L;
- Bond, JR;
- Borrill, J;
- Bouchet, FR;
- Boulanger, F;
- Burigana, C;
- Butler, RC;
- Calabrese, E;
- Cardoso, J-F;
- Catalano, A;
- Chiang, HC;
- Christensen, PR;
- Clements, DL;
- Colombi, S;
- Colombo, LPL;
- Combet, C;
- Crill, BP;
- Curto, A;
- Cuttaia, F;
- Danese, L;
- Davis, RJ;
- de Bernardis, P;
- de Zotti, G;
- Delabrouille, J;
- Dickinson, C;
- Diego, JM;
- Doré, O;
- Ducout, A;
- Dupac, X;
- Elsner, F;
- Enßlin, TA;
- Eriksen, HK;
- Finelli, F;
- Forni, O;
- Frailis, M;
- Fraisse, AA;
- Franceschi, E;
- Galeotta, S;
- Galli, S;
- Ganga, K;
- Ghosh, T;
- Giard, M;
- Giraud-Héraud, Y;
- Gjerløw, E;
- González-Nuevo, J;
- Górski, KM;
- Gruppuso, A;
- Gudmundsson, JE;
- Harrison, DL;
- Hernández-Monteagudo, C;
- Herranz, D;
- Hildebrandt, SR;
- Hornstrup, A;
- Hovest, W;
- Hurier, G;
- Jaffe, AH;
- Jones, WC;
- Keihänen, E;
- Keskitalo, R;
- Kisner, TS;
- Knoche, J;
- Knox, L;
- Kunz, M;
- Kurki-Suonio, H;
- Lagache, G;
- Lähteenmäki, A;
- Lamarre, J-M;
- Lasenby, A;
- Lattanzi, M;
- Leonardi, R;
- Levrier, F;
- Lilje, PB;
- Linden-Vørnle, M;
- López-Caniego, M;
- Lubin, PM;
- Macías-Pérez, JF;
- Maffei, B;
- Maggio, G;
- Maino, D;
- Mandolesi, N;
- Mangilli, A;
- Maris, M;
- Martin, PG;
- Martínez-González, E;
- Masi, S;
- Matarrese, S;
- Meinhold, PR;
- Melchiorri, A;
- Mennella, A;
- Migliaccio, M;
- Mitra, S;
- Miville-Deschênes, M-A;
- Moneti, A;
- Montier, L;
- Morgante, G;
- Mortlock, D;
- Moss, A;
- Munshi, D;
- Murphy, JA;
- Naselsky, P;
- Nati, F;
- Natoli, P;
- Netterfield, CB;
- Nørgaard-Nielsen, HU;
- Novikov, D;
- Novikov, I;
- Pagano, L;
- Pajot, F;
- Paoletti, D;
- Pasian, F;
- Patanchon, G;
- Perdereau, O;
- Perotto, L;
- Pettorino, V;
- Piacentini, F;
- Piat, M;
- Pierpaoli, E;
- Pointecouteau, E;
- Polenta, G;
- Pratt, GW;
- Rachen, JP;
- Reinecke, M;
- Remazeilles, M;
- Renault, C;
- Renzi, A;
- Ristorcelli, I;
- Rocha, G;
- Rosset, C;
- Rossetti, M;
- Roudier, G;
- Rubiño-Martín, JA;
- Rusholme, B;
- Sandri, M;
- Santos, D;
- Savelainen, M;
- Savini, G;
- Scott, D;
- Spencer, LD;
- Stolyarov, V;
- Stompor, R;
- Sudiwala, R;
- Sunyaev, R;
- Sutton, D;
- Suur-Uski, A-S;
- Sygnet, J-F;
- Tauber, JA;
- Terenzi, L;
- Toffolatti, L;
- Tomasi, M;
- Tristram, M;
- Tucci, M;
- Tuovinen, J;
- Valenziano, L;
- Valiviita, J;
- Van Tent, B;
- Vielva, P;
- Villa, F;
- Wade, LA;
- Wandelt, BD;
- Wehus, IK;
- Yvon, D;
- Zacchei, A;
- Zonca, A
Published Web Location
https://doi.org/10.1051/0004-6361/201527932Abstract
The secondary cosmic microwave background (CMB) B-modes stem from the post-decoupling distortion of the polarization E-modes due to the gravitational lensing effect of large-scale structures. These lensing-induced B-modes constitute both a valuable probe of the dark matter distribution and an important contaminant for the extraction of the primary CMB B-modes from inflation. Planck provides accurate nearly all-sky measurements of both the polarization E-modes and the integrated mass distribution via the reconstruction of the CMB lensing potential. By combining these two data products, we have produced an all-sky template map of the lensing-induced B-modes using a real-space algorithm that minimizes the impact of sky masks. The cross-correlation of this template with an observed (primordial and secondary) B-mode map can be used to measure the lensing B-mode power spectrum at multipoles up to 2000. In particular, when cross-correlating with the B-mode contribution directly derived from the Planck polarization maps, we obtain lensing-induced B-mode power spectrum measurement at a significance level of 12σ, which agrees with the theoretical expectation derived from the Planck best-fit Λ cold dark matter model. This unique nearly all-sky secondary B-mode template, which includes the lensing-induced information from intermediate to small (10 ≤ l ≤ 1000) angular scales, is delivered as part of the Planck 2015 public data release. It will be particularly useful for experiments searching for primordial B-modes, such as BICEP2/Keck Array or LiteBIRD, since it will enable an estimate to be made of the lensing-induced contribution to the measured total CMB B-modes.
Many UC-authored scholarly publications are freely available on this site because of the UC's open access policies. Let us know how this access is important for you.