- Main
Planck intermediate results
- Ade, PAR;
- Aghanim, N;
- Arnaud, M;
- Ashdown, M;
- Aubourg, E;
- Aumont, J;
- Baccigalupi, C;
- Banday, AJ;
- Barreiro, RB;
- Bartolo, N;
- Battaner, E;
- Benabed, K;
- Benoit-Lévy, A;
- Bersanelli, M;
- Bielewicz, P;
- Bock, JJ;
- Bonaldi, A;
- Bonavera, L;
- Bond, JR;
- Borrill, J;
- Bouchet, FR;
- Burigana, C;
- Calabrese, E;
- Cardoso, J-F;
- Catalano, A;
- Chamballu, A;
- Chiang, HC;
- Christensen, PR;
- Clements, DL;
- Colombo, LPL;
- Combet, C;
- Crill, BP;
- Curto, A;
- Cuttaia, F;
- Danese, L;
- Davies, RD;
- Davis, RJ;
- de Bernardis, P;
- de Zotti, G;
- Delabrouille, J;
- Dickinson, C;
- Diego, JM;
- Dolag, K;
- Donzelli, S;
- Doré, O;
- Douspis, M;
- Ducout, A;
- Dupac, X;
- Efstathiou, G;
- Elsner, F;
- Enßlin, TA;
- Eriksen, HK;
- Finelli, F;
- Forni, O;
- Frailis, M;
- Fraisse, AA;
- Franceschi, E;
- Frejsel, A;
- Galeotta, S;
- Galli, S;
- Ganga, K;
- Génova-Santos, RT;
- Giard, M;
- Gjerløw, E;
- González-Nuevo, J;
- Górski, KM;
- Gregorio, A;
- Gruppuso, A;
- Hansen, FK;
- Harrison, DL;
- Henrot-Versillé, S;
- Hernández-Monteagudo, C;
- Herranz, D;
- Hildebrandt, SR;
- Hivon, E;
- Hobson, M;
- Hornstrup, A;
- Huffenberger, KM;
- Hurier, G;
- Jaffe, AH;
- Jaffe, TR;
- Jones, WC;
- Juvela, M;
- Keihänen, E;
- Keskitalo, R;
- Kitaura, F;
- Kneissl, R;
- Knoche, J;
- Kunz, M;
- Kurki-Suonio, H;
- Lagache, G;
- Lamarre, J-M;
- Lasenby, A;
- Lattanzi, M;
- Lawrence, CR;
- Leonardi, R;
- León-Tavares, J;
- Levrier, F;
- Liguori, M;
- Lilje, PB;
- Linden-Vørnle, M;
- López-Caniego, M;
- Lubin, PM;
- Ma, Y-Z;
- Macías-Pérez, JF;
- Maffei, B;
- Maino, D;
- Mak, DSY;
- Mandolesi, N;
- Mangilli, A;
- Maris, M;
- Martin, PG;
- Martínez-González, E;
- Masi, S;
- Matarrese, S;
- McGehee, P;
- Melchiorri, A;
- Mennella, A;
- Migliaccio, M;
- Miville-Deschênes, M-A;
- Moneti, A;
- Montier, L;
- Morgante, G;
- Mortlock, D;
- Munshi, D;
- Murphy, JA;
- Naselsky, P;
- Nati, F;
- Natoli, P;
- Noviello, F;
- Novikov, D;
- Novikov, I;
- Oxborrow, CA;
- Pagano, L;
- Pajot, F;
- Paoletti, D;
- Perdereau, O;
- Perotto, L;
- Pettorino, V;
- Piacentini, F;
- Piat, M;
- Pierpaoli, E;
- Pointecouteau, E;
- Polenta, G;
- Ponthieu, N;
- Pratt, GW;
- Puget, J-L;
- Puisieux, S;
- Rachen, JP;
- Racine, B;
- Reach, WT;
- 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;
- Sudiwala, R;
- Sunyaev, R;
- Sutton, D;
- Suur-Uski, A-S;
- Sygnet, J-F;
- Tauber, JA;
- Terenzi, L;
- Toffolatti, L;
- Tomasi, M;
- Tucci, M;
- Valenziano, L;
- Valiviita, J;
- Van Tent, B;
- Vielva, P;
- Villa, F;
- Wade, LA;
- Wandelt, BD;
- Wang, W;
- Wehus, IK;
- Yvon, D;
- Zacchei, A;
- Zonca, A
- et al.
Published Web Location
https://doi.org/10.1051/0004-6361/201526328Abstract
By looking at the kinetic Sunyaev-Zeldovich effect (kSZ) in Planck nominal mission data, we present a significant detection of baryons participating in large-scale bulk flows around central galaxies (CGs) at redshift z ≈ 0.1. We estimate the pairwise momentum of the kSZ temperature fluctuations at the positions of the Central Galaxy Catalogue (CGC) samples extracted from Sloan Digital Sky Survey (SDSS-DR7) data. For the foreground-cleaned SEVEM, SMICA, NILC, and COMMANDER maps, we find 1.8-2.5σ detections of the kSZ signal, which are consistent with the kSZ evidence found in individual Planck raw frequency maps, although lower than found in the WMAP-9yr W-band (3.3σ). We further reconstruct the peculiar velocity field from the CG density field, and compute for the first time the cross-correlation function between kSZ temperature fluctuations and estimates of CG radial peculiar velocities. This correlation function yields a 3.0-3.7σ detection of the peculiar motion of extended gas on Mpc scales in flows correlated up to distances of 80-100 h-1 Mpc. Both the pairwise momentum estimates and the kSZ temperature-velocity field correlation find evidence for kSZ signatures out to apertures of 8 arcmin and beyond, corresponding to a physical radius of >1 Mpc, more than twice the mean virial radius of halos. This is consistent with the predictions from hydrodynamical simulations that most of the baryons are outside the virialized halos. We fit a simple model, in which the temperature-velocity cross-correlation is proportional to the signal seen in a semi-analytic model built upon N-body simulations, and interpret the proportionality constant as an effective optical depth to Thomson scattering. We find τT = (1.4 ± 0.5) × 10-4; the simplest interpretation of this measurement is that much of the gas is in a diffuse phase, which contributes little signal to X-ray or thermal Sunyaev-Zeldovich observations.
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