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Three‐Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Polarization Analysis

  • Authors: L. Page, G. Hinshaw, E. Komatsu, M. R. Nolta, D. N. Spergel, C. L. Bennett, C. Barnes, R. Bean, O. Doré, J. Dunkley, M. Halpern, R. S. Hill, N. Jarosik, A. Kogut, M. Limon, S. S. Meyer, N. Odegard, H. V. Peiris, G. S. Tucker, L. Verde, J. L. Weiland, E. Wollack, and E. L. Wright

Page et al. 2007 The Astrophysical Journal Supplement Series 170 335.

  • Provider: AAS Journals

Caption: Fig. 7.

Left: Angle of the magnetic field, ﹩\gamma _{M}=\gamma _{\mathrm{PA}\,}+90^{\circ }﹩, derived from the synchrotron radiation in the K‐band map (smoothed with a 4° beam) shown in Fig. 3. (We do not distinguish between ±180° in the field direction.) The predominant low Galactic latitude magnetic field direction is parallel to the Galactic plane (﹩\gamma _{M}=90^{\circ }﹩) and thus the synchrotron (and dust) polarization directions have ﹩\gamma \approx 0^{\circ }﹩. In the North Polar Spur region, the magnetic field is perpendicular to the Galactic plane corresponding to ﹩\gamma _{M}\approx 0^{\circ }﹩ or 180°. Note the large‐scale coherency of the field. Right: Predicted magnetic field direction given by a simple model of the electron distribution and the logarithmic spiral arm model (eq. [9]) for the magnetic field.

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