Serena A. Cronin, Alberto D. Bolatto, Helena M. Richie, Grant P. Donnelly, Rebecca C. Levy, Karl D. Gordon, Elizabeth Tarantino, Martha L. Boyer, L Armus, Patricia A. Arens, Leindert Boogaard, Daniel A. Dale, Keaton Donaghue, Bruce T. Draine, Sara E. Duval, Kimberly Emig, David B. Fisher, Simon C. O. Glover, Brandon S. Hensley, Rodrigo Herrera-Camus, Ralf S. Klessen, T S-Y Lai, Laura Lenkić, Adam K. Leroy, Ashley E. Lieber, Ilse De Looze, Sebastian Lopez, David S. Meier, Elisabeth A.C. Mills, Karin Sandström, Evan Schneider, Kaitlyn E. Sheriff, Utsav Siwakoti, Evan D. Skillman, J.D.T. Smith, Yu-Hsuan Teng, Todd A. Thompson, Alexander G.G.M. Tielens, Sylvain Veilleux, Vicente Villanueva, Fabian Walter, Paul P. van der Werf
Abstract We present JWST MIRI and NIRCam imaging of the inner ∼5 kpc of the M82 superwind at ∼ 0 . ″ 05 − 0 . ″ 375 (∼0.9–6.5 pc) resolution. Targeted filters probe emission from polycyclic aromatic hydrocarbons (PAHs; F335M, F360M , F770W, F1130W) and continuum (F250M, F360M) The images reveal a network of cool wind filaments traced by PAHs. PAH surface brightness declines with the inverse square of distance to the midplane, suggesting that the incident radiation field from the starburst drives the observed PAH intensity out to ±2.5 kpc. The 3.3/11.3 and 3.3/7.7 μ m band ratios show uniformity with distance from the starburst, though comparisons with mid-IR dust emission models indicate a modest shift toward larger PAHs. Outside the disk, 11.3/7.7 μ m increases moderately, reflecting that PAHs become more neutral with distance from the starburst as they are exposed to a declining radiation field and ionization parameter. Overall, PAHs in the wind are consistent with standard-to-large sizes and standard-to-high ionization states. Including Spitzer and Herschel data, PAH abundance ( q PAH ) is set at ∼1% in the starburst and remains unchanging out to ±5 kpc off the disk. This flat q PAH profile suggests that PAHs are shielded from the hot wind, perhaps residing in the surface layers of cool clouds, with possible replenishment from cloud interiors and enrichment of the halo from previous bursts. In this picture, clouds are not dense enough to promote PAH growth, and they likely undergo radiative cooling and mixing with the hot phase to survive the gauntlet for at least ∼20 Myr.