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Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters: LI. Features in the cosmic microwav...

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Zeitschriftentitel: Astronomy & Astrophysics
Personen und Körperschaften: Aghanim, N., Akrami, Y., Ashdown, M., Aumont, J., Baccigalupi, C., Ballardini, M., Banday, A. J., Barreiro, R. B., Bartolo, N., Basak, S., Benabed, K., Bersanelli, M., Bielewicz, P., Bonaldi, A., Bonavera, L., Bond, J. R., Borrill, J., Bouchet, F. R., Burigana, C., Calabrese, E., Cardoso, J.-F., Challinor, A., Chiang, H. C., Colombo, L. P. L., Combet, C., 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., Dusini, S., Efstathiou, G., Elsner, F., Enßlin, T. A., Eriksen, H. K., Fantaye, Y., Finelli, F., Forastieri, F., Frailis, M., Franceschi, E., Frolov, A., Galeotta, S., Galli, S., Ganga, K., Génova-Santos, R. T., Gerbino, M., González-Nuevo, J., Górski, K. M., Gratton, S., Gruppuso, A., Gudmundsson, J. E., Herranz, D., Hivon, E., Huang, Z., Jaffe, A. H., Jones, W. C., Keihänen, E., Keskitalo, R., Kiiveri, K., Kim, J., Kisner, T. S., Knox, L., Krachmalnicoff, N., Kunz, M., Kurki-Suonio, H., Lagache, G., Lamarre, J.-M., Lasenby, A., Lattanzi, M., Lawrence, C. R., Le Jeune, M., Levrier, F., Lewis, A., Liguori, M., Lilje, P. B., Lilley, M., Lindholm, V., López-Caniego, M., Lubin, P. M., Ma, Y.-Z., Macías-Pérez, J. F., Maggio, G., Maino, D., Mandolesi, N., Mangilli, A., Maris, M., Martin, P. G., Martínez-González, E., Matarrese, S., Mauri, N., McEwen, J. D., Meinhold, P. R., Mennella, A., Migliaccio, M., Millea, M., Miville-Deschênes, M.-A., Molinari, D., Moneti, A., Montier, L., Morgante, G., Moss, A., Narimani, A., Natoli, P., Oxborrow, C. A., Pagano, L., Paoletti, D., Partridge, B., Patanchon, G., Patrizii, L., Pettorino, V., Piacentini, F., Polastri, L., Polenta, G., Puget, J.-L., Rachen, J. P., Racine, B., Reinecke, M., Remazeilles, M., Renzi, A., Rocha, G., Rossetti, M., Roudier, G., Rubiño-Martín, J. A., Ruiz-Granados, B., Salvati, L., Sandri, M., Savelainen, M., Scott, D., Sirignano, C., Sirri, G., Stanco, L., 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., Vittorio, N., Wandelt, B. D., Wehus, I. K., White, M., Zacchei, A., Zonca, A.
In: Astronomy & Astrophysics, 607, 2017, S. A95
Format: E-Article
Sprache: Unbestimmt
veröffentlicht:
EDP Sciences
Schlagwörter:
Space and Planetary Science
Astronomy and Astrophysics
author_facet Aghanim, N.
Akrami, Y.
Ashdown, M.
Aumont, J.
Baccigalupi, C.
Ballardini, M.
Banday, A. J.
Barreiro, R. B.
Bartolo, N.
Basak, S.
Benabed, K.
Bersanelli, M.
Bielewicz, P.
Bonaldi, A.
Bonavera, L.
Bond, J. R.
Borrill, J.
Bouchet, F. R.
Burigana, C.
Calabrese, E.
Cardoso, J.-F.
Challinor, A.
Chiang, H. C.
Colombo, L. P. L.
Combet, C.
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.
Dusini, S.
Efstathiou, G.
Elsner, F.
Enßlin, T. A.
Eriksen, H. K.
Fantaye, Y.
Finelli, F.
Forastieri, F.
Frailis, M.
Franceschi, E.
Frolov, A.
Galeotta, S.
Galli, S.
Ganga, K.
Génova-Santos, R. T.
Gerbino, M.
González-Nuevo, J.
Górski, K. M.
Gratton, S.
Gruppuso, A.
Gudmundsson, J. E.
Herranz, D.
Hivon, E.
Huang, Z.
Jaffe, A. H.
Jones, W. C.
Keihänen, E.
Keskitalo, R.
Kiiveri, K.
Kim, J.
Kisner, T. S.
Knox, L.
Krachmalnicoff, N.
Kunz, M.
Kurki-Suonio, H.
Lagache, G.
Lamarre, J.-M.
Lasenby, A.
Lattanzi, M.
Lawrence, C. R.
Le Jeune, M.
Levrier, F.
Lewis, A.
Liguori, M.
Lilje, P. B.
Lilley, M.
Lindholm, V.
López-Caniego, M.
Lubin, P. M.
Ma, Y.-Z.
Macías-Pérez, J. F.
Maggio, G.
Maino, D.
Mandolesi, N.
Mangilli, A.
Maris, M.
Martin, P. G.
Martínez-González, E.
Matarrese, S.
Mauri, N.
McEwen, J. D.
Meinhold, P. R.
Mennella, A.
Migliaccio, M.
Millea, M.
Miville-Deschênes, M.-A.
Molinari, D.
Moneti, A.
Montier, L.
Morgante, G.
Moss, A.
Narimani, A.
Natoli, P.
Oxborrow, C. A.
Pagano, L.
Paoletti, D.
Partridge, B.
Patanchon, G.
Patrizii, L.
Pettorino, V.
Piacentini, F.
Polastri, L.
Polenta, G.
Puget, J.-L.
Rachen, J. P.
Racine, B.
Reinecke, M.
Remazeilles, M.
Renzi, A.
Rocha, G.
Rossetti, M.
Roudier, G.
Rubiño-Martín, J. A.
Ruiz-Granados, B.
Salvati, L.
Sandri, M.
Savelainen, M.
Scott, D.
Sirignano, C.
Sirri, G.
Stanco, L.
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.
Vittorio, N.
Wandelt, B. D.
Wehus, I. K.
White, M.
Zacchei, A.
Zonca, A.
Aghanim, N.
Akrami, Y.
Ashdown, M.
Aumont, J.
Baccigalupi, C.
Ballardini, M.
Banday, A. J.
Barreiro, R. B.
Bartolo, N.
Basak, S.
Benabed, K.
Bersanelli, M.
Bielewicz, P.
Bonaldi, A.
Bonavera, L.
Bond, J. R.
Borrill, J.
Bouchet, F. R.
Burigana, C.
Calabrese, E.
Cardoso, J.-F.
Challinor, A.
Chiang, H. C.
Colombo, L. P. L.
Combet, C.
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.
Dusini, S.
Efstathiou, G.
Elsner, F.
Enßlin, T. A.
Eriksen, H. K.
Fantaye, Y.
Finelli, F.
Forastieri, F.
Frailis, M.
Franceschi, E.
Frolov, A.
Galeotta, S.
Galli, S.
Ganga, K.
Génova-Santos, R. T.
Gerbino, M.
González-Nuevo, J.
Górski, K. M.
Gratton, S.
Gruppuso, A.
Gudmundsson, J. E.
Herranz, D.
Hivon, E.
Huang, Z.
Jaffe, A. H.
Jones, W. C.
Keihänen, E.
Keskitalo, R.
Kiiveri, K.
Kim, J.
Kisner, T. S.
Knox, L.
Krachmalnicoff, N.
Kunz, M.
Kurki-Suonio, H.
Lagache, G.
Lamarre, J.-M.
Lasenby, A.
Lattanzi, M.
Lawrence, C. R.
Le Jeune, M.
Levrier, F.
Lewis, A.
Liguori, M.
Lilje, P. B.
Lilley, M.
Lindholm, V.
López-Caniego, M.
Lubin, P. M.
Ma, Y.-Z.
Macías-Pérez, J. F.
Maggio, G.
Maino, D.
Mandolesi, N.
Mangilli, A.
Maris, M.
Martin, P. G.
Martínez-González, E.
Matarrese, S.
Mauri, N.
McEwen, J. D.
Meinhold, P. R.
Mennella, A.
Migliaccio, M.
Millea, M.
Miville-Deschênes, M.-A.
Molinari, D.
Moneti, A.
Montier, L.
Morgante, G.
Moss, A.
Narimani, A.
Natoli, P.
Oxborrow, C. A.
Pagano, L.
Paoletti, D.
Partridge, B.
Patanchon, G.
Patrizii, L.
Pettorino, V.
Piacentini, F.
Polastri, L.
Polenta, G.
Puget, J.-L.
Rachen, J. P.
Racine, B.
Reinecke, M.
Remazeilles, M.
Renzi, A.
Rocha, G.
Rossetti, M.
Roudier, G.
Rubiño-Martín, J. A.
Ruiz-Granados, B.
Salvati, L.
Sandri, M.
Savelainen, M.
Scott, D.
Sirignano, C.
Sirri, G.
Stanco, L.
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.
Vittorio, N.
Wandelt, B. D.
Wehus, I. K.
White, M.
Zacchei, A.
Zonca, A.
author Aghanim, N.
Akrami, Y.
Ashdown, M.
Aumont, J.
Baccigalupi, C.
Ballardini, M.
Banday, A. J.
Barreiro, R. B.
Bartolo, N.
Basak, S.
Benabed, K.
Bersanelli, M.
Bielewicz, P.
Bonaldi, A.
Bonavera, L.
Bond, J. R.
Borrill, J.
Bouchet, F. R.
Burigana, C.
Calabrese, E.
Cardoso, J.-F.
Challinor, A.
Chiang, H. C.
Colombo, L. P. L.
Combet, C.
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.
Dusini, S.
Efstathiou, G.
Elsner, F.
Enßlin, T. A.
Eriksen, H. K.
Fantaye, Y.
Finelli, F.
Forastieri, F.
Frailis, M.
Franceschi, E.
Frolov, A.
Galeotta, S.
Galli, S.
Ganga, K.
Génova-Santos, R. T.
Gerbino, M.
González-Nuevo, J.
Górski, K. M.
Gratton, S.
Gruppuso, A.
Gudmundsson, J. E.
Herranz, D.
Hivon, E.
Huang, Z.
Jaffe, A. H.
Jones, W. C.
Keihänen, E.
Keskitalo, R.
Kiiveri, K.
Kim, J.
Kisner, T. S.
Knox, L.
Krachmalnicoff, N.
Kunz, M.
Kurki-Suonio, H.
Lagache, G.
Lamarre, J.-M.
Lasenby, A.
Lattanzi, M.
Lawrence, C. R.
Le Jeune, M.
Levrier, F.
Lewis, A.
Liguori, M.
Lilje, P. B.
Lilley, M.
Lindholm, V.
López-Caniego, M.
Lubin, P. M.
Ma, Y.-Z.
Macías-Pérez, J. F.
Maggio, G.
Maino, D.
Mandolesi, N.
Mangilli, A.
Maris, M.
Martin, P. G.
Martínez-González, E.
Matarrese, S.
Mauri, N.
McEwen, J. D.
Meinhold, P. R.
Mennella, A.
Migliaccio, M.
Millea, M.
Miville-Deschênes, M.-A.
Molinari, D.
Moneti, A.
Montier, L.
Morgante, G.
Moss, A.
Narimani, A.
Natoli, P.
Oxborrow, C. A.
Pagano, L.
Paoletti, D.
Partridge, B.
Patanchon, G.
Patrizii, L.
Pettorino, V.
Piacentini, F.
Polastri, L.
Polenta, G.
Puget, J.-L.
Rachen, J. P.
Racine, B.
Reinecke, M.
Remazeilles, M.
Renzi, A.
Rocha, G.
Rossetti, M.
Roudier, G.
Rubiño-Martín, J. A.
Ruiz-Granados, B.
Salvati, L.
Sandri, M.
Savelainen, M.
Scott, D.
Sirignano, C.
Sirri, G.
Stanco, L.
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.
Vittorio, N.
Wandelt, B. D.
Wehus, I. K.
White, M.
Zacchei, A.
Zonca, A.
spellingShingle Aghanim, N.
Akrami, Y.
Ashdown, M.
Aumont, J.
Baccigalupi, C.
Ballardini, M.
Banday, A. J.
Barreiro, R. B.
Bartolo, N.
Basak, S.
Benabed, K.
Bersanelli, M.
Bielewicz, P.
Bonaldi, A.
Bonavera, L.
Bond, J. R.
Borrill, J.
Bouchet, F. R.
Burigana, C.
Calabrese, E.
Cardoso, J.-F.
Challinor, A.
Chiang, H. C.
Colombo, L. P. L.
Combet, C.
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.
Dusini, S.
Efstathiou, G.
Elsner, F.
Enßlin, T. A.
Eriksen, H. K.
Fantaye, Y.
Finelli, F.
Forastieri, F.
Frailis, M.
Franceschi, E.
Frolov, A.
Galeotta, S.
Galli, S.
Ganga, K.
Génova-Santos, R. T.
Gerbino, M.
González-Nuevo, J.
Górski, K. M.
Gratton, S.
Gruppuso, A.
Gudmundsson, J. E.
Herranz, D.
Hivon, E.
Huang, Z.
Jaffe, A. H.
Jones, W. C.
Keihänen, E.
Keskitalo, R.
Kiiveri, K.
Kim, J.
Kisner, T. S.
Knox, L.
Krachmalnicoff, N.
Kunz, M.
Kurki-Suonio, H.
Lagache, G.
Lamarre, J.-M.
Lasenby, A.
Lattanzi, M.
Lawrence, C. R.
Le Jeune, M.
Levrier, F.
Lewis, A.
Liguori, M.
Lilje, P. B.
Lilley, M.
Lindholm, V.
López-Caniego, M.
Lubin, P. M.
Ma, Y.-Z.
Macías-Pérez, J. F.
Maggio, G.
Maino, D.
Mandolesi, N.
Mangilli, A.
Maris, M.
Martin, P. G.
Martínez-González, E.
Matarrese, S.
Mauri, N.
McEwen, J. D.
Meinhold, P. R.
Mennella, A.
Migliaccio, M.
Millea, M.
Miville-Deschênes, M.-A.
Molinari, D.
Moneti, A.
Montier, L.
Morgante, G.
Moss, A.
Narimani, A.
Natoli, P.
Oxborrow, C. A.
Pagano, L.
Paoletti, D.
Partridge, B.
Patanchon, G.
Patrizii, L.
Pettorino, V.
Piacentini, F.
Polastri, L.
Polenta, G.
Puget, J.-L.
Rachen, J. P.
Racine, B.
Reinecke, M.
Remazeilles, M.
Renzi, A.
Rocha, G.
Rossetti, M.
Roudier, G.
Rubiño-Martín, J. A.
Ruiz-Granados, B.
Salvati, L.
Sandri, M.
Savelainen, M.
Scott, D.
Sirignano, C.
Sirri, G.
Stanco, L.
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.
Vittorio, N.
Wandelt, B. D.
Wehus, I. K.
White, M.
Zacchei, A.
Zonca, A.
Astronomy & Astrophysics
Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
Space and Planetary Science
Astronomy and Astrophysics
author_sort aghanim, n.
spelling Aghanim, N. Akrami, Y. Ashdown, M. Aumont, J. Baccigalupi, C. Ballardini, M. Banday, A. J. Barreiro, R. B. Bartolo, N. Basak, S. Benabed, K. Bersanelli, M. Bielewicz, P. Bonaldi, A. Bonavera, L. Bond, J. R. Borrill, J. Bouchet, F. R. Burigana, C. Calabrese, E. Cardoso, J.-F. Challinor, A. Chiang, H. C. Colombo, L. P. L. Combet, C. 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. Dusini, S. Efstathiou, G. Elsner, F. Enßlin, T. A. Eriksen, H. K. Fantaye, Y. Finelli, F. Forastieri, F. Frailis, M. Franceschi, E. Frolov, A. Galeotta, S. Galli, S. Ganga, K. Génova-Santos, R. T. Gerbino, M. González-Nuevo, J. Górski, K. M. Gratton, S. Gruppuso, A. Gudmundsson, J. E. Herranz, D. Hivon, E. Huang, Z. Jaffe, A. H. Jones, W. C. Keihänen, E. Keskitalo, R. Kiiveri, K. Kim, J. Kisner, T. S. Knox, L. Krachmalnicoff, N. Kunz, M. Kurki-Suonio, H. Lagache, G. Lamarre, J.-M. Lasenby, A. Lattanzi, M. Lawrence, C. R. Le Jeune, M. Levrier, F. Lewis, A. Liguori, M. Lilje, P. B. Lilley, M. Lindholm, V. López-Caniego, M. Lubin, P. M. Ma, Y.-Z. Macías-Pérez, J. F. Maggio, G. Maino, D. Mandolesi, N. Mangilli, A. Maris, M. Martin, P. G. Martínez-González, E. Matarrese, S. Mauri, N. McEwen, J. D. Meinhold, P. R. Mennella, A. Migliaccio, M. Millea, M. Miville-Deschênes, M.-A. Molinari, D. Moneti, A. Montier, L. Morgante, G. Moss, A. Narimani, A. Natoli, P. Oxborrow, C. A. Pagano, L. Paoletti, D. Partridge, B. Patanchon, G. Patrizii, L. Pettorino, V. Piacentini, F. Polastri, L. Polenta, G. Puget, J.-L. Rachen, J. P. Racine, B. Reinecke, M. Remazeilles, M. Renzi, A. Rocha, G. Rossetti, M. Roudier, G. Rubiño-Martín, J. A. Ruiz-Granados, B. Salvati, L. Sandri, M. Savelainen, M. Scott, D. Sirignano, C. Sirri, G. Stanco, L. 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. Vittorio, N. Wandelt, B. D. Wehus, I. K. White, M. Zacchei, A. Zonca, A. 0004-6361 1432-0746 EDP Sciences Space and Planetary Science Astronomy and Astrophysics http://dx.doi.org/10.1051/0004-6361/201629504 <jats:p>The six parameters of the standard ΛCDM model have best-fit values derived from the <jats:italic>Planck</jats:italic> temperature power spectrum that are shifted somewhat from the best-fit values derived from WMAP data. These shifts are driven by features in the <jats:italic>Planck</jats:italic> temperature power spectrum at angular scales that had never before been measured to cosmic-variance level precision. We have investigated these shifts to determine whether they are within the range of expectation and to understand their origin in the data. Taking our parameter set to be the optical depth of the reionized intergalactic medium <jats:italic>τ</jats:italic>, the baryon density <jats:italic>ω</jats:italic><jats:sub>b</jats:sub>, the matter density <jats:italic>ω</jats:italic><jats:sub>m</jats:sub>, the angular size of the sound horizon <jats:italic>θ</jats:italic><jats:sub>∗</jats:sub>, the spectral index of the primordial power spectrum, <jats:italic>n</jats:italic><jats:sub>s</jats:sub>, and <jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup> (where <jats:italic>A</jats:italic><jats:sub>s</jats:sub> is the amplitude of the primordial power spectrum), we have examined the change in best-fit values between a WMAP-like large angular-scale data set (with multipole moment <jats:italic>ℓ</jats:italic> &lt; 800 in the <jats:italic>Planck</jats:italic> temperature power spectrum) and an all angular-scale data set (<jats:italic>ℓ</jats:italic> &lt; 2500<jats:italic>Planck</jats:italic> temperature power spectrum), each with a prior on <jats:italic>τ</jats:italic> of 0.07 ± 0.02. We find that the shifts, in units of the 1<jats:italic>σ</jats:italic> expected dispersion for each parameter, are { Δ<jats:italic>τ,</jats:italic>Δ<jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup>,Δ<jats:italic>n</jats:italic><jats:sub>s</jats:sub>,Δ<jats:italic>ω</jats:italic><jats:sub>m</jats:sub>,Δ<jats:italic>ω</jats:italic><jats:sub>b</jats:sub>,Δ<jats:italic>θ</jats:italic><jats:sub>∗</jats:sub> } = { −1.7,−2.2,1.2,−2.0,1.1,0.9 }, with a <jats:italic>χ</jats:italic><jats:sup>2</jats:sup> value of 8.0. We find that this <jats:italic>χ</jats:italic><jats:sup>2</jats:sup> value is exceeded in 15% of our simulated data sets, and that a parameter deviates by more than 2.2<jats:italic>σ</jats:italic> in 9% of simulated data sets, meaning that the shifts are not unusually large. Comparing <jats:italic>ℓ</jats:italic> &lt; 800 instead to <jats:italic>ℓ</jats:italic>&gt; 800, or splitting at a different multipole, yields similar results. We examined the <jats:italic>ℓ</jats:italic> &lt; 800 model residuals in the <jats:italic>ℓ</jats:italic>&gt; 800 power spectrum data and find that the features there that drive these shifts are a set of oscillations across a broad range of angular scales. Although they partly appear similar to the effects of enhanced gravitational lensing, the shifts in ΛCDM parameters that arise in response to these features correspond to model spectrum changes that are predominantly due to non-lensing effects; the only exception is <jats:italic>τ</jats:italic>, which, at fixed <jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup>, affects the <jats:italic>ℓ</jats:italic>&gt; 800 temperature power spectrum solely through the associated change in <jats:italic>A</jats:italic><jats:sub>s</jats:sub> and the impact of that on the lensing potential power spectrum. We also ask, “what is it about the power spectrum at <jats:italic>ℓ</jats:italic> &lt; 800 that leads to somewhat different best-fit parameters than come from the full <jats:italic>ℓ</jats:italic> range?” We find that if we discard the data at <jats:italic>ℓ</jats:italic> &lt; 30, where there is a roughly 2<jats:italic>σ</jats:italic> downward fluctuation in power relative to the model that best fits the full <jats:italic>ℓ</jats:italic> range, the <jats:italic>ℓ</jats:italic> &lt; 800 best-fit parameters shift significantly towards the <jats:italic>ℓ</jats:italic> &lt; 2500 best-fit parameters. In contrast, including <jats:italic>ℓ</jats:italic> &lt; 30, this previously noted “low-<jats:italic>ℓ</jats:italic> deficit” drives <jats:italic>n</jats:italic><jats:sub>s</jats:sub> up and impacts parameters correlated with <jats:italic>n</jats:italic><jats:sub>s</jats:sub>, such as <jats:italic>ω</jats:italic><jats:sub>m</jats:sub> and <jats:italic>H</jats:italic><jats:sub>0</jats:sub>. As expected, the <jats:italic>ℓ</jats:italic> &lt; 30 data have a much greater impact on the <jats:italic>ℓ</jats:italic> &lt; 800 best fit than on the <jats:italic>ℓ</jats:italic> &lt; 2500 best fit. So although the shifts are not very significant, we find that they can be understood through the combined effects of an oscillatory-like set of high-<jats:italic>ℓ</jats:italic> residuals and the deficit in low-<jats:italic>ℓ</jats:italic> power, excursions consistent with sample variance that happen to map onto changes in cosmological parameters. Finally, we examine agreement between <jats:italic>Planck</jats:italic><jats:italic>TT</jats:italic> data and two other CMB data sets, namely the <jats:italic>Planck</jats:italic> lensing reconstruction and the <jats:italic>TT</jats:italic> power spectrum measured by the South Pole Telescope, again finding a lack of convincing evidence of any significant deviations in parameters, suggesting that current CMB data sets give an internally consistent picture of the ΛCDM model.</jats:p> LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters <i>Planck </i>intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters Astronomy & Astrophysics
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match_str aghanim2017planckintermediateresultslifeaturesinthecosmicmicrowavebackgroundtemperaturepowerspectrumandshiftsincosmologicalparameterslifeaturesinthecosmicmicrowavebackgroundtemperaturepowerspectrumandshiftsincosmologicalparameters
publishDateSort 2017
publisher EDP Sciences
recordtype ai
record_format ai
series Astronomy & Astrophysics
source_id 49
title_sub LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_unstemmed Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_full Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_fullStr Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_full_unstemmed Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_short Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_sort <i>planck </i>intermediate results : li. features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
topic Space and Planetary Science
Astronomy and Astrophysics
url http://dx.doi.org/10.1051/0004-6361/201629504
publishDate 2017
physical A95
description <jats:p>The six parameters of the standard ΛCDM model have best-fit values derived from the <jats:italic>Planck</jats:italic> temperature power spectrum that are shifted somewhat from the best-fit values derived from WMAP data. These shifts are driven by features in the <jats:italic>Planck</jats:italic> temperature power spectrum at angular scales that had never before been measured to cosmic-variance level precision. We have investigated these shifts to determine whether they are within the range of expectation and to understand their origin in the data. Taking our parameter set to be the optical depth of the reionized intergalactic medium <jats:italic>τ</jats:italic>, the baryon density <jats:italic>ω</jats:italic><jats:sub>b</jats:sub>, the matter density <jats:italic>ω</jats:italic><jats:sub>m</jats:sub>, the angular size of the sound horizon <jats:italic>θ</jats:italic><jats:sub>∗</jats:sub>, the spectral index of the primordial power spectrum, <jats:italic>n</jats:italic><jats:sub>s</jats:sub>, and <jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup> (where <jats:italic>A</jats:italic><jats:sub>s</jats:sub> is the amplitude of the primordial power spectrum), we have examined the change in best-fit values between a WMAP-like large angular-scale data set (with multipole moment <jats:italic>ℓ</jats:italic> &lt; 800 in the <jats:italic>Planck</jats:italic> temperature power spectrum) and an all angular-scale data set (<jats:italic>ℓ</jats:italic> &lt; 2500<jats:italic>Planck</jats:italic> temperature power spectrum), each with a prior on <jats:italic>τ</jats:italic> of 0.07 ± 0.02. We find that the shifts, in units of the 1<jats:italic>σ</jats:italic> expected dispersion for each parameter, are { Δ<jats:italic>τ,</jats:italic>Δ<jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup>,Δ<jats:italic>n</jats:italic><jats:sub>s</jats:sub>,Δ<jats:italic>ω</jats:italic><jats:sub>m</jats:sub>,Δ<jats:italic>ω</jats:italic><jats:sub>b</jats:sub>,Δ<jats:italic>θ</jats:italic><jats:sub>∗</jats:sub> } = { −1.7,−2.2,1.2,−2.0,1.1,0.9 }, with a <jats:italic>χ</jats:italic><jats:sup>2</jats:sup> value of 8.0. We find that this <jats:italic>χ</jats:italic><jats:sup>2</jats:sup> value is exceeded in 15% of our simulated data sets, and that a parameter deviates by more than 2.2<jats:italic>σ</jats:italic> in 9% of simulated data sets, meaning that the shifts are not unusually large. Comparing <jats:italic>ℓ</jats:italic> &lt; 800 instead to <jats:italic>ℓ</jats:italic>&gt; 800, or splitting at a different multipole, yields similar results. We examined the <jats:italic>ℓ</jats:italic> &lt; 800 model residuals in the <jats:italic>ℓ</jats:italic>&gt; 800 power spectrum data and find that the features there that drive these shifts are a set of oscillations across a broad range of angular scales. Although they partly appear similar to the effects of enhanced gravitational lensing, the shifts in ΛCDM parameters that arise in response to these features correspond to model spectrum changes that are predominantly due to non-lensing effects; the only exception is <jats:italic>τ</jats:italic>, which, at fixed <jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup>, affects the <jats:italic>ℓ</jats:italic>&gt; 800 temperature power spectrum solely through the associated change in <jats:italic>A</jats:italic><jats:sub>s</jats:sub> and the impact of that on the lensing potential power spectrum. We also ask, “what is it about the power spectrum at <jats:italic>ℓ</jats:italic> &lt; 800 that leads to somewhat different best-fit parameters than come from the full <jats:italic>ℓ</jats:italic> range?” We find that if we discard the data at <jats:italic>ℓ</jats:italic> &lt; 30, where there is a roughly 2<jats:italic>σ</jats:italic> downward fluctuation in power relative to the model that best fits the full <jats:italic>ℓ</jats:italic> range, the <jats:italic>ℓ</jats:italic> &lt; 800 best-fit parameters shift significantly towards the <jats:italic>ℓ</jats:italic> &lt; 2500 best-fit parameters. In contrast, including <jats:italic>ℓ</jats:italic> &lt; 30, this previously noted “low-<jats:italic>ℓ</jats:italic> deficit” drives <jats:italic>n</jats:italic><jats:sub>s</jats:sub> up and impacts parameters correlated with <jats:italic>n</jats:italic><jats:sub>s</jats:sub>, such as <jats:italic>ω</jats:italic><jats:sub>m</jats:sub> and <jats:italic>H</jats:italic><jats:sub>0</jats:sub>. As expected, the <jats:italic>ℓ</jats:italic> &lt; 30 data have a much greater impact on the <jats:italic>ℓ</jats:italic> &lt; 800 best fit than on the <jats:italic>ℓ</jats:italic> &lt; 2500 best fit. So although the shifts are not very significant, we find that they can be understood through the combined effects of an oscillatory-like set of high-<jats:italic>ℓ</jats:italic> residuals and the deficit in low-<jats:italic>ℓ</jats:italic> power, excursions consistent with sample variance that happen to map onto changes in cosmological parameters. Finally, we examine agreement between <jats:italic>Planck</jats:italic><jats:italic>TT</jats:italic> data and two other CMB data sets, namely the <jats:italic>Planck</jats:italic> lensing reconstruction and the <jats:italic>TT</jats:italic> power spectrum measured by the South Pole Telescope, again finding a lack of convincing evidence of any significant deviations in parameters, suggesting that current CMB data sets give an internally consistent picture of the ΛCDM model.</jats:p>
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author Aghanim, N., Akrami, Y., Ashdown, M., Aumont, J., Baccigalupi, C., Ballardini, M., Banday, A. J., Barreiro, R. B., Bartolo, N., Basak, S., Benabed, K., Bersanelli, M., Bielewicz, P., Bonaldi, A., Bonavera, L., Bond, J. R., Borrill, J., Bouchet, F. R., Burigana, C., Calabrese, E., Cardoso, J.-F., Challinor, A., Chiang, H. C., Colombo, L. P. L., Combet, C., 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., Dusini, S., Efstathiou, G., Elsner, F., Enßlin, T. A., Eriksen, H. K., Fantaye, Y., Finelli, F., Forastieri, F., Frailis, M., Franceschi, E., Frolov, A., Galeotta, S., Galli, S., Ganga, K., Génova-Santos, R. T., Gerbino, M., González-Nuevo, J., Górski, K. M., Gratton, S., Gruppuso, A., Gudmundsson, J. E., Herranz, D., Hivon, E., Huang, Z., Jaffe, A. H., Jones, W. C., Keihänen, E., Keskitalo, R., Kiiveri, K., Kim, J., Kisner, T. S., Knox, L., Krachmalnicoff, N., Kunz, M., Kurki-Suonio, H., Lagache, G., Lamarre, J.-M., Lasenby, A., Lattanzi, M., Lawrence, C. R., Le Jeune, M., Levrier, F., Lewis, A., Liguori, M., Lilje, P. B., Lilley, M., Lindholm, V., López-Caniego, M., Lubin, P. M., Ma, Y.-Z., Macías-Pérez, J. F., Maggio, G., Maino, D., Mandolesi, N., Mangilli, A., Maris, M., Martin, P. G., Martínez-González, E., Matarrese, S., Mauri, N., McEwen, J. D., Meinhold, P. R., Mennella, A., Migliaccio, M., Millea, M., Miville-Deschênes, M.-A., Molinari, D., Moneti, A., Montier, L., Morgante, G., Moss, A., Narimani, A., Natoli, P., Oxborrow, C. A., Pagano, L., Paoletti, D., Partridge, B., Patanchon, G., Patrizii, L., Pettorino, V., Piacentini, F., Polastri, L., Polenta, G., Puget, J.-L., Rachen, J. P., Racine, B., Reinecke, M., Remazeilles, M., Renzi, A., Rocha, G., Rossetti, M., Roudier, G., Rubiño-Martín, J. A., Ruiz-Granados, B., Salvati, L., Sandri, M., Savelainen, M., Scott, D., Sirignano, C., Sirri, G., Stanco, L., 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., Vittorio, N., Wandelt, B. D., Wehus, I. K., White, M., Zacchei, A., Zonca, A.
author_facet Aghanim, N., Akrami, Y., Ashdown, M., Aumont, J., Baccigalupi, C., Ballardini, M., Banday, A. J., Barreiro, R. B., Bartolo, N., Basak, S., Benabed, K., Bersanelli, M., Bielewicz, P., Bonaldi, A., Bonavera, L., Bond, J. R., Borrill, J., Bouchet, F. R., Burigana, C., Calabrese, E., Cardoso, J.-F., Challinor, A., Chiang, H. C., Colombo, L. P. L., Combet, C., 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., Dusini, S., Efstathiou, G., Elsner, F., Enßlin, T. A., Eriksen, H. K., Fantaye, Y., Finelli, F., Forastieri, F., Frailis, M., Franceschi, E., Frolov, A., Galeotta, S., Galli, S., Ganga, K., Génova-Santos, R. T., Gerbino, M., González-Nuevo, J., Górski, K. M., Gratton, S., Gruppuso, A., Gudmundsson, J. E., Herranz, D., Hivon, E., Huang, Z., Jaffe, A. H., Jones, W. C., Keihänen, E., Keskitalo, R., Kiiveri, K., Kim, J., Kisner, T. S., Knox, L., Krachmalnicoff, N., Kunz, M., Kurki-Suonio, H., Lagache, G., Lamarre, J.-M., Lasenby, A., Lattanzi, M., Lawrence, C. R., Le Jeune, M., Levrier, F., Lewis, A., Liguori, M., Lilje, P. B., Lilley, M., Lindholm, V., López-Caniego, M., Lubin, P. M., Ma, Y.-Z., Macías-Pérez, J. F., Maggio, G., Maino, D., Mandolesi, N., Mangilli, A., Maris, M., Martin, P. G., Martínez-González, E., Matarrese, S., Mauri, N., McEwen, J. D., Meinhold, P. R., Mennella, A., Migliaccio, M., Millea, M., Miville-Deschênes, M.-A., Molinari, D., Moneti, A., Montier, L., Morgante, G., Moss, A., Narimani, A., Natoli, P., Oxborrow, C. A., Pagano, L., Paoletti, D., Partridge, B., Patanchon, G., Patrizii, L., Pettorino, V., Piacentini, F., Polastri, L., Polenta, G., Puget, J.-L., Rachen, J. P., Racine, B., Reinecke, M., Remazeilles, M., Renzi, A., Rocha, G., Rossetti, M., Roudier, G., Rubiño-Martín, J. A., Ruiz-Granados, B., Salvati, L., Sandri, M., Savelainen, M., Scott, D., Sirignano, C., Sirri, G., Stanco, L., 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., Vittorio, N., Wandelt, B. D., Wehus, I. K., White, M., Zacchei, A., Zonca, A., Aghanim, N., Akrami, Y., Ashdown, M., Aumont, J., Baccigalupi, C., Ballardini, M., Banday, A. J., Barreiro, R. B., Bartolo, N., Basak, S., Benabed, K., Bersanelli, M., Bielewicz, P., Bonaldi, A., Bonavera, L., Bond, J. R., Borrill, J., Bouchet, F. R., Burigana, C., Calabrese, E., Cardoso, J.-F., Challinor, A., Chiang, H. C., Colombo, L. P. L., Combet, C., 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., Dusini, S., Efstathiou, G., Elsner, F., Enßlin, T. A., Eriksen, H. K., Fantaye, Y., Finelli, F., Forastieri, F., Frailis, M., Franceschi, E., Frolov, A., Galeotta, S., Galli, S., Ganga, K., Génova-Santos, R. T., Gerbino, M., González-Nuevo, J., Górski, K. M., Gratton, S., Gruppuso, A., Gudmundsson, J. E., Herranz, D., Hivon, E., Huang, Z., Jaffe, A. H., Jones, W. C., Keihänen, E., Keskitalo, R., Kiiveri, K., Kim, J., Kisner, T. S., Knox, L., Krachmalnicoff, N., Kunz, M., Kurki-Suonio, H., Lagache, G., Lamarre, J.-M., Lasenby, A., Lattanzi, M., Lawrence, C. R., Le Jeune, M., Levrier, F., Lewis, A., Liguori, M., Lilje, P. B., Lilley, M., Lindholm, V., López-Caniego, M., Lubin, P. M., Ma, Y.-Z., Macías-Pérez, J. F., Maggio, G., Maino, D., Mandolesi, N., Mangilli, A., Maris, M., Martin, P. G., Martínez-González, E., Matarrese, S., Mauri, N., McEwen, J. D., Meinhold, P. R., Mennella, A., Migliaccio, M., Millea, M., Miville-Deschênes, M.-A., Molinari, D., Moneti, A., Montier, L., Morgante, G., Moss, A., Narimani, A., Natoli, P., Oxborrow, C. A., Pagano, L., Paoletti, D., Partridge, B., Patanchon, G., Patrizii, L., Pettorino, V., Piacentini, F., Polastri, L., Polenta, G., Puget, J.-L., Rachen, J. P., Racine, B., Reinecke, M., Remazeilles, M., Renzi, A., Rocha, G., Rossetti, M., Roudier, G., Rubiño-Martín, J. A., Ruiz-Granados, B., Salvati, L., Sandri, M., Savelainen, M., Scott, D., Sirignano, C., Sirri, G., Stanco, L., 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., Vittorio, N., Wandelt, B. D., Wehus, I. K., White, M., Zacchei, A., Zonca, A.
author_sort aghanim, n.
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container_title Astronomy & Astrophysics
container_volume 607
description <jats:p>The six parameters of the standard ΛCDM model have best-fit values derived from the <jats:italic>Planck</jats:italic> temperature power spectrum that are shifted somewhat from the best-fit values derived from WMAP data. These shifts are driven by features in the <jats:italic>Planck</jats:italic> temperature power spectrum at angular scales that had never before been measured to cosmic-variance level precision. We have investigated these shifts to determine whether they are within the range of expectation and to understand their origin in the data. Taking our parameter set to be the optical depth of the reionized intergalactic medium <jats:italic>τ</jats:italic>, the baryon density <jats:italic>ω</jats:italic><jats:sub>b</jats:sub>, the matter density <jats:italic>ω</jats:italic><jats:sub>m</jats:sub>, the angular size of the sound horizon <jats:italic>θ</jats:italic><jats:sub>∗</jats:sub>, the spectral index of the primordial power spectrum, <jats:italic>n</jats:italic><jats:sub>s</jats:sub>, and <jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup> (where <jats:italic>A</jats:italic><jats:sub>s</jats:sub> is the amplitude of the primordial power spectrum), we have examined the change in best-fit values between a WMAP-like large angular-scale data set (with multipole moment <jats:italic>ℓ</jats:italic> &lt; 800 in the <jats:italic>Planck</jats:italic> temperature power spectrum) and an all angular-scale data set (<jats:italic>ℓ</jats:italic> &lt; 2500<jats:italic>Planck</jats:italic> temperature power spectrum), each with a prior on <jats:italic>τ</jats:italic> of 0.07 ± 0.02. We find that the shifts, in units of the 1<jats:italic>σ</jats:italic> expected dispersion for each parameter, are { Δ<jats:italic>τ,</jats:italic>Δ<jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup>,Δ<jats:italic>n</jats:italic><jats:sub>s</jats:sub>,Δ<jats:italic>ω</jats:italic><jats:sub>m</jats:sub>,Δ<jats:italic>ω</jats:italic><jats:sub>b</jats:sub>,Δ<jats:italic>θ</jats:italic><jats:sub>∗</jats:sub> } = { −1.7,−2.2,1.2,−2.0,1.1,0.9 }, with a <jats:italic>χ</jats:italic><jats:sup>2</jats:sup> value of 8.0. We find that this <jats:italic>χ</jats:italic><jats:sup>2</jats:sup> value is exceeded in 15% of our simulated data sets, and that a parameter deviates by more than 2.2<jats:italic>σ</jats:italic> in 9% of simulated data sets, meaning that the shifts are not unusually large. Comparing <jats:italic>ℓ</jats:italic> &lt; 800 instead to <jats:italic>ℓ</jats:italic>&gt; 800, or splitting at a different multipole, yields similar results. We examined the <jats:italic>ℓ</jats:italic> &lt; 800 model residuals in the <jats:italic>ℓ</jats:italic>&gt; 800 power spectrum data and find that the features there that drive these shifts are a set of oscillations across a broad range of angular scales. Although they partly appear similar to the effects of enhanced gravitational lensing, the shifts in ΛCDM parameters that arise in response to these features correspond to model spectrum changes that are predominantly due to non-lensing effects; the only exception is <jats:italic>τ</jats:italic>, which, at fixed <jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup>, affects the <jats:italic>ℓ</jats:italic>&gt; 800 temperature power spectrum solely through the associated change in <jats:italic>A</jats:italic><jats:sub>s</jats:sub> and the impact of that on the lensing potential power spectrum. We also ask, “what is it about the power spectrum at <jats:italic>ℓ</jats:italic> &lt; 800 that leads to somewhat different best-fit parameters than come from the full <jats:italic>ℓ</jats:italic> range?” We find that if we discard the data at <jats:italic>ℓ</jats:italic> &lt; 30, where there is a roughly 2<jats:italic>σ</jats:italic> downward fluctuation in power relative to the model that best fits the full <jats:italic>ℓ</jats:italic> range, the <jats:italic>ℓ</jats:italic> &lt; 800 best-fit parameters shift significantly towards the <jats:italic>ℓ</jats:italic> &lt; 2500 best-fit parameters. In contrast, including <jats:italic>ℓ</jats:italic> &lt; 30, this previously noted “low-<jats:italic>ℓ</jats:italic> deficit” drives <jats:italic>n</jats:italic><jats:sub>s</jats:sub> up and impacts parameters correlated with <jats:italic>n</jats:italic><jats:sub>s</jats:sub>, such as <jats:italic>ω</jats:italic><jats:sub>m</jats:sub> and <jats:italic>H</jats:italic><jats:sub>0</jats:sub>. As expected, the <jats:italic>ℓ</jats:italic> &lt; 30 data have a much greater impact on the <jats:italic>ℓ</jats:italic> &lt; 800 best fit than on the <jats:italic>ℓ</jats:italic> &lt; 2500 best fit. So although the shifts are not very significant, we find that they can be understood through the combined effects of an oscillatory-like set of high-<jats:italic>ℓ</jats:italic> residuals and the deficit in low-<jats:italic>ℓ</jats:italic> power, excursions consistent with sample variance that happen to map onto changes in cosmological parameters. Finally, we examine agreement between <jats:italic>Planck</jats:italic><jats:italic>TT</jats:italic> data and two other CMB data sets, namely the <jats:italic>Planck</jats:italic> lensing reconstruction and the <jats:italic>TT</jats:italic> power spectrum measured by the South Pole Telescope, again finding a lack of convincing evidence of any significant deviations in parameters, suggesting that current CMB data sets give an internally consistent picture of the ΛCDM model.</jats:p>
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spelling Aghanim, N. Akrami, Y. Ashdown, M. Aumont, J. Baccigalupi, C. Ballardini, M. Banday, A. J. Barreiro, R. B. Bartolo, N. Basak, S. Benabed, K. Bersanelli, M. Bielewicz, P. Bonaldi, A. Bonavera, L. Bond, J. R. Borrill, J. Bouchet, F. R. Burigana, C. Calabrese, E. Cardoso, J.-F. Challinor, A. Chiang, H. C. Colombo, L. P. L. Combet, C. 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. Dusini, S. Efstathiou, G. Elsner, F. Enßlin, T. A. Eriksen, H. K. Fantaye, Y. Finelli, F. Forastieri, F. Frailis, M. Franceschi, E. Frolov, A. Galeotta, S. Galli, S. Ganga, K. Génova-Santos, R. T. Gerbino, M. González-Nuevo, J. Górski, K. M. Gratton, S. Gruppuso, A. Gudmundsson, J. E. Herranz, D. Hivon, E. Huang, Z. Jaffe, A. H. Jones, W. C. Keihänen, E. Keskitalo, R. Kiiveri, K. Kim, J. Kisner, T. S. Knox, L. Krachmalnicoff, N. Kunz, M. Kurki-Suonio, H. Lagache, G. Lamarre, J.-M. Lasenby, A. Lattanzi, M. Lawrence, C. R. Le Jeune, M. Levrier, F. Lewis, A. Liguori, M. Lilje, P. B. Lilley, M. Lindholm, V. López-Caniego, M. Lubin, P. M. Ma, Y.-Z. Macías-Pérez, J. F. Maggio, G. Maino, D. Mandolesi, N. Mangilli, A. Maris, M. Martin, P. G. Martínez-González, E. Matarrese, S. Mauri, N. McEwen, J. D. Meinhold, P. R. Mennella, A. Migliaccio, M. Millea, M. Miville-Deschênes, M.-A. Molinari, D. Moneti, A. Montier, L. Morgante, G. Moss, A. Narimani, A. Natoli, P. Oxborrow, C. A. Pagano, L. Paoletti, D. Partridge, B. Patanchon, G. Patrizii, L. Pettorino, V. Piacentini, F. Polastri, L. Polenta, G. Puget, J.-L. Rachen, J. P. Racine, B. Reinecke, M. Remazeilles, M. Renzi, A. Rocha, G. Rossetti, M. Roudier, G. Rubiño-Martín, J. A. Ruiz-Granados, B. Salvati, L. Sandri, M. Savelainen, M. Scott, D. Sirignano, C. Sirri, G. Stanco, L. 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. Vittorio, N. Wandelt, B. D. Wehus, I. K. White, M. Zacchei, A. Zonca, A. 0004-6361 1432-0746 EDP Sciences Space and Planetary Science Astronomy and Astrophysics http://dx.doi.org/10.1051/0004-6361/201629504 <jats:p>The six parameters of the standard ΛCDM model have best-fit values derived from the <jats:italic>Planck</jats:italic> temperature power spectrum that are shifted somewhat from the best-fit values derived from WMAP data. These shifts are driven by features in the <jats:italic>Planck</jats:italic> temperature power spectrum at angular scales that had never before been measured to cosmic-variance level precision. We have investigated these shifts to determine whether they are within the range of expectation and to understand their origin in the data. Taking our parameter set to be the optical depth of the reionized intergalactic medium <jats:italic>τ</jats:italic>, the baryon density <jats:italic>ω</jats:italic><jats:sub>b</jats:sub>, the matter density <jats:italic>ω</jats:italic><jats:sub>m</jats:sub>, the angular size of the sound horizon <jats:italic>θ</jats:italic><jats:sub>∗</jats:sub>, the spectral index of the primordial power spectrum, <jats:italic>n</jats:italic><jats:sub>s</jats:sub>, and <jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup> (where <jats:italic>A</jats:italic><jats:sub>s</jats:sub> is the amplitude of the primordial power spectrum), we have examined the change in best-fit values between a WMAP-like large angular-scale data set (with multipole moment <jats:italic>ℓ</jats:italic> &lt; 800 in the <jats:italic>Planck</jats:italic> temperature power spectrum) and an all angular-scale data set (<jats:italic>ℓ</jats:italic> &lt; 2500<jats:italic>Planck</jats:italic> temperature power spectrum), each with a prior on <jats:italic>τ</jats:italic> of 0.07 ± 0.02. We find that the shifts, in units of the 1<jats:italic>σ</jats:italic> expected dispersion for each parameter, are { Δ<jats:italic>τ,</jats:italic>Δ<jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup>,Δ<jats:italic>n</jats:italic><jats:sub>s</jats:sub>,Δ<jats:italic>ω</jats:italic><jats:sub>m</jats:sub>,Δ<jats:italic>ω</jats:italic><jats:sub>b</jats:sub>,Δ<jats:italic>θ</jats:italic><jats:sub>∗</jats:sub> } = { −1.7,−2.2,1.2,−2.0,1.1,0.9 }, with a <jats:italic>χ</jats:italic><jats:sup>2</jats:sup> value of 8.0. We find that this <jats:italic>χ</jats:italic><jats:sup>2</jats:sup> value is exceeded in 15% of our simulated data sets, and that a parameter deviates by more than 2.2<jats:italic>σ</jats:italic> in 9% of simulated data sets, meaning that the shifts are not unusually large. Comparing <jats:italic>ℓ</jats:italic> &lt; 800 instead to <jats:italic>ℓ</jats:italic>&gt; 800, or splitting at a different multipole, yields similar results. We examined the <jats:italic>ℓ</jats:italic> &lt; 800 model residuals in the <jats:italic>ℓ</jats:italic>&gt; 800 power spectrum data and find that the features there that drive these shifts are a set of oscillations across a broad range of angular scales. Although they partly appear similar to the effects of enhanced gravitational lensing, the shifts in ΛCDM parameters that arise in response to these features correspond to model spectrum changes that are predominantly due to non-lensing effects; the only exception is <jats:italic>τ</jats:italic>, which, at fixed <jats:italic>A</jats:italic><jats:sub>s</jats:sub>e<jats:sup>− 2<jats:italic>τ</jats:italic></jats:sup>, affects the <jats:italic>ℓ</jats:italic>&gt; 800 temperature power spectrum solely through the associated change in <jats:italic>A</jats:italic><jats:sub>s</jats:sub> and the impact of that on the lensing potential power spectrum. We also ask, “what is it about the power spectrum at <jats:italic>ℓ</jats:italic> &lt; 800 that leads to somewhat different best-fit parameters than come from the full <jats:italic>ℓ</jats:italic> range?” We find that if we discard the data at <jats:italic>ℓ</jats:italic> &lt; 30, where there is a roughly 2<jats:italic>σ</jats:italic> downward fluctuation in power relative to the model that best fits the full <jats:italic>ℓ</jats:italic> range, the <jats:italic>ℓ</jats:italic> &lt; 800 best-fit parameters shift significantly towards the <jats:italic>ℓ</jats:italic> &lt; 2500 best-fit parameters. In contrast, including <jats:italic>ℓ</jats:italic> &lt; 30, this previously noted “low-<jats:italic>ℓ</jats:italic> deficit” drives <jats:italic>n</jats:italic><jats:sub>s</jats:sub> up and impacts parameters correlated with <jats:italic>n</jats:italic><jats:sub>s</jats:sub>, such as <jats:italic>ω</jats:italic><jats:sub>m</jats:sub> and <jats:italic>H</jats:italic><jats:sub>0</jats:sub>. As expected, the <jats:italic>ℓ</jats:italic> &lt; 30 data have a much greater impact on the <jats:italic>ℓ</jats:italic> &lt; 800 best fit than on the <jats:italic>ℓ</jats:italic> &lt; 2500 best fit. So although the shifts are not very significant, we find that they can be understood through the combined effects of an oscillatory-like set of high-<jats:italic>ℓ</jats:italic> residuals and the deficit in low-<jats:italic>ℓ</jats:italic> power, excursions consistent with sample variance that happen to map onto changes in cosmological parameters. Finally, we examine agreement between <jats:italic>Planck</jats:italic><jats:italic>TT</jats:italic> data and two other CMB data sets, namely the <jats:italic>Planck</jats:italic> lensing reconstruction and the <jats:italic>TT</jats:italic> power spectrum measured by the South Pole Telescope, again finding a lack of convincing evidence of any significant deviations in parameters, suggesting that current CMB data sets give an internally consistent picture of the ΛCDM model.</jats:p> LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters <i>Planck </i>intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters Astronomy & Astrophysics
spellingShingle Aghanim, N., Akrami, Y., Ashdown, M., Aumont, J., Baccigalupi, C., Ballardini, M., Banday, A. J., Barreiro, R. B., Bartolo, N., Basak, S., Benabed, K., Bersanelli, M., Bielewicz, P., Bonaldi, A., Bonavera, L., Bond, J. R., Borrill, J., Bouchet, F. R., Burigana, C., Calabrese, E., Cardoso, J.-F., Challinor, A., Chiang, H. C., Colombo, L. P. L., Combet, C., 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., Dusini, S., Efstathiou, G., Elsner, F., Enßlin, T. A., Eriksen, H. K., Fantaye, Y., Finelli, F., Forastieri, F., Frailis, M., Franceschi, E., Frolov, A., Galeotta, S., Galli, S., Ganga, K., Génova-Santos, R. T., Gerbino, M., González-Nuevo, J., Górski, K. M., Gratton, S., Gruppuso, A., Gudmundsson, J. E., Herranz, D., Hivon, E., Huang, Z., Jaffe, A. H., Jones, W. C., Keihänen, E., Keskitalo, R., Kiiveri, K., Kim, J., Kisner, T. S., Knox, L., Krachmalnicoff, N., Kunz, M., Kurki-Suonio, H., Lagache, G., Lamarre, J.-M., Lasenby, A., Lattanzi, M., Lawrence, C. R., Le Jeune, M., Levrier, F., Lewis, A., Liguori, M., Lilje, P. B., Lilley, M., Lindholm, V., López-Caniego, M., Lubin, P. M., Ma, Y.-Z., Macías-Pérez, J. F., Maggio, G., Maino, D., Mandolesi, N., Mangilli, A., Maris, M., Martin, P. G., Martínez-González, E., Matarrese, S., Mauri, N., McEwen, J. D., Meinhold, P. R., Mennella, A., Migliaccio, M., Millea, M., Miville-Deschênes, M.-A., Molinari, D., Moneti, A., Montier, L., Morgante, G., Moss, A., Narimani, A., Natoli, P., Oxborrow, C. A., Pagano, L., Paoletti, D., Partridge, B., Patanchon, G., Patrizii, L., Pettorino, V., Piacentini, F., Polastri, L., Polenta, G., Puget, J.-L., Rachen, J. P., Racine, B., Reinecke, M., Remazeilles, M., Renzi, A., Rocha, G., Rossetti, M., Roudier, G., Rubiño-Martín, J. A., Ruiz-Granados, B., Salvati, L., Sandri, M., Savelainen, M., Scott, D., Sirignano, C., Sirri, G., Stanco, L., 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., Vittorio, N., Wandelt, B. D., Wehus, I. K., White, M., Zacchei, A., Zonca, A., Astronomy & Astrophysics, Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters, Space and Planetary Science, Astronomy and Astrophysics
title Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_full Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_fullStr Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_full_unstemmed Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_short Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_sort <i>planck </i>intermediate results : li. features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_sub LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
title_unstemmed Planck intermediate results : LI. Features in the cosmic microwave background temperature power spectrum and shifts in cosmological parameters
topic Space and Planetary Science, Astronomy and Astrophysics
url http://dx.doi.org/10.1051/0004-6361/201629504