Using precise full-sky observations from Planck, and applying several methods of component separation, we identify and characterise the emission from the Galactic "haze" at microwave wavelengths. The haze is a distinct component of diffuse Galactic emission, roughly centered on the Galactic centre, and extends to vertical bar b vertical bar similar to 35-50 degrees in Galactic latitude and vertical bar l vertical bar similar to 15-20 degrees in longitude. By combining the Planck data with observations from the Wilkinson Microwave Anisotropy Probe, we were able to determine the spectrum of this emission to high accuracy, unhindered by the strong systematic biases present in previous analyses. The derived spectrum is consistent with power-law emission with a spectral index of -2.56 +/- 0.05, thus excluding free-free emission as the source and instead favouring hard-spectrum synchrotron radiation from an electron population with a spectrum (number density per energy) dN/dE proportional to E-2.1. At Galactic latitudes vertical bar b vertical bar < 30 degrees, the microwave haze morphology is consistent with that of the Fermi gamma-ray "haze" or "bubbles", while at b similar to -50 degrees we have identified an edge in the microwave haze that is spatially coincident with the edge in the gamma-ray bubbles. Taken together, this indicates that we have a multi-wavelength view of a distinct component of our Galaxy. Given both the very hard spectrum and the extended nature of the emission, it is highly unlikely that the haze electrons result from supernova shocks in the Galactic disk. Instead, a new astrophysical mechanism for cosmic-ray acceleration in the inner Galaxy is implied.

Planck intermediate results IX. Detection of the Galactic haze with Planck

MANDOLESI, Nazzareno;NATOLI, Paolo;
2013

Abstract

Using precise full-sky observations from Planck, and applying several methods of component separation, we identify and characterise the emission from the Galactic "haze" at microwave wavelengths. The haze is a distinct component of diffuse Galactic emission, roughly centered on the Galactic centre, and extends to vertical bar b vertical bar similar to 35-50 degrees in Galactic latitude and vertical bar l vertical bar similar to 15-20 degrees in longitude. By combining the Planck data with observations from the Wilkinson Microwave Anisotropy Probe, we were able to determine the spectrum of this emission to high accuracy, unhindered by the strong systematic biases present in previous analyses. The derived spectrum is consistent with power-law emission with a spectral index of -2.56 +/- 0.05, thus excluding free-free emission as the source and instead favouring hard-spectrum synchrotron radiation from an electron population with a spectrum (number density per energy) dN/dE proportional to E-2.1. At Galactic latitudes vertical bar b vertical bar < 30 degrees, the microwave haze morphology is consistent with that of the Fermi gamma-ray "haze" or "bubbles", while at b similar to -50 degrees we have identified an edge in the microwave haze that is spatially coincident with the edge in the gamma-ray bubbles. Taken together, this indicates that we have a multi-wavelength view of a distinct component of our Galaxy. Given both the very hard spectrum and the extended nature of the emission, it is highly unlikely that the haze electrons result from supernova shocks in the Galactic disk. Instead, a new astrophysical mechanism for cosmic-ray acceleration in the inner Galaxy is implied.
2013
P. A., R.; N., Aghanim; M., Arnaud; M., Ashdown; F., Atrio Barandela; J., Aumont; C., Baccigalupi; A., Balbi; A. J., Banday; R. B., Barreiro; J. G., Bartlett; E., Battaner; K., Benabed; A., Benoit; J. . ., P.; M., Bersanelli; A., Bonaldi; J. R., Bond; J., Borrill; F. R., Bouchet; C., Burigana; P., Cabella; J. . ., F.; A., Catalano; L., Cayon; R. . . R., L. . . Y.; P. R., Christensen; D. L., Clements; L. P., L.; A., Coulais; B. P., Crill; F., Cuttaia; L., Danese; O., D'Arcangelo; R. J., Davis; P. d., Bernardis; A. d., Rosa; G. d., Zotti; J., Delabrouille; C., Dickinson; J. M., Diego; G., Dobler; H., Dole; S., Donzelli; O., Dore; U., Doerl; M., Douspis; X., Dupac; G., Efstathiou; T. A., Ensslin; H. K., Eriksen; F., Finelli; O., Forni; M., Frailis; E., Franceschi; S., Galeotta; K., Ganga; M., Giard; G., Giardino; J., Gonzalez Nuevo; K. M., Gorski; S., Gratton; A., Gregorio; A., Gruppuso; F. K., Hansen; D., Harrison; G., Helou; S., Henrot Versille; C., Hernandez Monteagudo; S. R., Hildebrandt; M., Hobson; W. A., Holmes; A., Hornstrup; W., Hovest; K. M., Huffenberger; T. R., Jaffe; T., Jagemann; J., Jewell; W. C., Jones; M., Juvela; E., Keihaecn; J., Knoche; L., Knox; M., Kunz; H., Kurki Suonio; G., Lagache; A., Lahteenmaki; J. . ., M.; A., Lasenby; C. R., Lawrence; S., Leach; R., Leonardi; P. B., Lilje; M., Linden Vornle; M., Lopez Caniego; P. M., Lubin; J. F., Macias Perez; B., Maffei; D., Maino; Mandolesi, Nazzareno; M., Maris; D. J., Marshall; P. G., Martin; E., Martinez Gonzalez; S., Masi; M., Massardi; S., Matarrese; F., Matthai; P., Mazzotta; P. R., Meinhold; A., Melchiorri; L., Mendes; A., Mennella; S., Mitra; A., Moneti; L., Montier; G., Morgante; D., Munshi; J. A., Murphy; P., Naselsky; Natoli, Paolo; H. U., Norgaard Nielsen; F., Noviello; D., Novikov; S., Osborne; F., Pajot; R., Paladini; D., Paoletti; B., Partridge; T. J., Pearson; O., Perdereau; F., Perrotta; F., Piacentini; M., Piat; E., Pierpaoli; D., Pietrobon; S., Plaszczynski; E., Pointecouteau; G., Polenta; N., Ponthieu; L., Popa; T., Poutanen; G. W., Pratt; S., Prunet; J. . ., L.; J. P., Rachen; R., Rebolo; M., Reinecke; C., Renault; S., Ricciardi; T., Riller; I., Ristorcelli; G., Rocha; C., Rosset; J. A., Rubino Martin; B., Rusholme; M., Sandri; G., Savini; B. M., Schaefer; D., Scott; G. F., Smoot; L., Spencer; F., Stivoli; R., Sudiwala; A. . . S., J. . . F.; J. A., Tauber; L., Terenzi; L., Toffolatti; M., Tomasi; M., Tristram; M., Tuerler; G., Umana; L., Valenziano; B. V., Tent; P., Vielva; F., Villa; N., Vittorio; L. A., Wade; B. D., Wandelt; M., White; D., Yvon; A., Zacchei; A., Zonca
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11392/2284440
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