Electron temperature and emission measure of HII regions in the central molecular zone (CMZ) from H40 αrecombination line and continuum emissions by ALMA CMZ Exploration Survey - ACES -
Yoshiaki Sofue, Steven N. Longmore, Daniel Walker, Adam Ginsburg, Jonathan D. Henshaw, John Bally, Ashley T. Barnes, Cara Battersby, Laura Colzi, Paul Ho, Izaskun Jimenez-serra, Elizabeth Mills, Maya A. Petkova, Mattia C. Sormani, Jennifer Wallace, Robin G. Tress, Nazar Budaiev, Rojita Buddhacharya, Christoph Federrath, Zi-xuan Feng, Pablo García, Savannah Gramze, Christian Henkel, Pei-ying Hsieh, Fengwei Xu, Katharina Immer, Dani Lipman, Dariusz C. Lis, Álvaro Sánchez-Monge, Xing Lu, Mark R. Morris, Francisco Nogueras-Lara, JÜrgen Ott, Dylan M. Paré, Jaime E. Pineda, Víctor M. Rivilla, Jairo Armijos-Abendaño, Qizhou Zhang, 6Denise Riquelme-vásquez, Howard a. Smith, Marco Donati, Q. Daniel Wang, N. Bijas
Abstract
Star formation activity in the Central Molecular Zone (CMZ) directly manifests itself as radio continuum free-free emission (Bremsstrahlung) and radio recombination line emission from HII regions surrounding newly formed massive stars. We derive the overall distribution of the HII regions and their fundamental properties: electron temperature () and emission measure (EM), and hence electron density in the form of two dimensional distribution maps over the CMZ by analyzing the ACES (ALMA CMZ Exploration Survey) 40 (99.02 GHz) recombination line and 99.6 GHz continuum emission data with synthesized beam widths of 2''.45 (0.097 pc at 8.2 kpc) and 2''.14, respectively. We apply the 'TeEM' method (--EM mapping), which creates and EM maps from input 2D maps of the continuum and integrated line intensity. The analysis covers the entire ACES field from l -0.6 to +0.8 and from b -0.2 to +0.1. The area analyzed is complete and includes previously known HII regions such as Sgr B2, Sgr B1, the Sickle, the Pistol, thermal filaments (Bridges), Sgr A HII regions, the Minispiral, and many other known HII regions. Sgr C is not included in the analysis due to the insufficient signal-to-noise ratio in the recombination line map. The mean electron temperature over the CMZ is determined to be = 5872 78 ~ (SE) ~ 3682~ (SD) K (SE:standard error of the mean, SD: pixel-to-pixel standard deviation). Some HII regions, such as Sgr B2 Main and the Minispiral, exhibit large scatter and an internal gradient of several thousand K per parsec. The EM distribution is more diverse, varying by orders of magnitude from 105 to 3× 108 within the CMZ, as well as within individual HII regions.
Create a lesson
Related papers
Rotational spectroscopy and astronomical search of propane-1-thiol (CH3CH2CH2SH) and propane-2-thiol ((CH3)2CHSH)
Wentao Song, Assimo Maris, Victor M. Rivilla et al.
CosmoDyn: a semi-analytic post-processing framework for the dynamical evolution of compact stellar systems and black holes in cosmological simulations
Pierre Boldrini, Paola Di Matteo, David Katz et al.
CNO in Giant Metal-Poor Stars
Jannat Alazzawi
The Spitzer Data Fusion - A Far-Ultraviolet to Far-Infrared Multi-Wavelength Database in Spitzer Extragalactic Survey Fields
Mattia Vaccari
Signatures of dark subhaloes in dwarf spheroidal galaxies: II. Transient and localised kinematic features
Eduardo Vitral, Jorge Penarrubia, Roeland P. van der Marel et al.
Challenging the archetypal intermittent radio galaxy J0111+3906. New insights from optical GTC/OSIRIS and radio VLA and LOFAR observations
M. Orienti, J. A. Acosta-Pulido, E. De Rubeis et al.