Physical properties and H-ionizing-photon production rates of extreme nearby star-forming regions

ArXiv 1709.03503 (2017)

Authors:

Jacopo Chevallard, Stéphane Charlot, Peter Senchyna, Daniel P Stark, Alba Vidal-García, Anna Feltre, Julia Gutkin, Tucker Jones, Ramesh Mainali, Aida Wofford

Abstract:

Measurements of the galaxy UV luminosity function at z>6 suggest that young stars hosted in low-mass star-forming galaxies produced the bulk of hydrogen-ionizing photons necessary to reionize the intergalactic medium (IGM) by redshift z~6. Whether star-forming galaxies dominated cosmic reionization, however, also depends on their stellar populations and interstellar medium properties, which set, among other things, the production rate of H-ionizing photons, $\xi_\text{ion}^\star$, and the fraction of these escaping into the IGM. Given the difficulty of constraining with existing observatories the physical properties of z>6 galaxies, in this work we focus on a sample of ten nearby objects showing UV spectral features comparable to those observed at z>6. We use the new-generation Beagle tool to model the UV-to-optical photometry and UV/optical emission lines of these Local 'analogues' of high-redshift galaxies, finding that our relatively simple, yet fully self-consistent, physical model can successfully reproduce the different observables considered. Our galaxies span a broad range of metallicities and are characterised by high ionization parameters, low dust attenuation, and very young stellar populations. Through our analysis, we derive a novel diagnostic of the production rate of H-ionizing photons per unit UV luminosity, $\xi_\text{ion}^\star$, based on the equivalent width of the bright $[\text{OIII}] \lambda 4959,5007$ doublet, which does not require measurements of H-recombination lines. This new diagnostic can be used to estimate $\xi_\text{ion}^\star$ from future direct measurements of the $[\text{OIII}] \lambda 4959,5007$ line using JWST/NIRSpec (out to z~9.5), and by exploiting the contamination by $\text{H}\beta + [\text{OIII}] \lambda 4959,5007$ of photometric observations of distant galaxies, for instance from existing Spitzer/IRAC data and from future ones with JWST/NIRCam.

Gamma-ray and X-ray emission from the Galactic Centre: hints on the nuclear star cluster formation history

(2017)

Authors:

Manuel Arca-Sedda, Bence Kocsis, Timothy Brandt

The KMOS Cluster Survey (KCS). I. The fundamental plane and the formation ages of cluster galaxies at redshift 1.4 < Z < 1.6

Astrophysical Journal American Astronomical Society 846:2 (2017) 1-25

Authors:

A Beifiori, JT Mendel, JCC Chan, RP Saglia, R Bender, Michele Cappellari, Roger L Davies, A Galametz, Ryan CW Houghton, Laura J Prichard, R Smith, John P Stott, DJ Wilman, Ian J Lewis, R Sharples, M Wegner

Abstract:

The American Astronomical Society. All rights reserved. We present the analysis of the fundamental plane (FP) for a sample of 19 massive red-sequence galaxies (M· > ×4 10 10 M·) in three known overdensities at 1.39 1.61 < < z from the K-band Multi-object Spectrograph (KMOS) Cluster Survey, a guaranteed-time program with spectroscopy from the KMOS at the VLT and imaging from the Hubble Space Telescope. As expected, we find that the FP zero-point in B band evolves with redshift, from the value 0.443 of Coma to -0.10±0.09, -0.19±0.05, and -0.29±0.12 for our clusters at z = 1.39, z = 1.46, and z = 1.61, respectively. For the most massive galaxies (log 1 M M· > 1) in our sample, we translate the FP zero-point evolution into a mass-to-light-ratio M/L evolution, finding D log 0.46 0.10 M L z B = - (D log )0.52 0.07 M L z B = -to(D log ) 0.55 0.10 M L z B = - respectively. We assess the potential contribution of the galaxy structural and stellar velocity dispersion evolution to the evolution of the FP zero-point and find it to be ∼6%-35% of the FP zero-point evolution. The rate of M/L evolution is consistent with galaxies evolving passively. Using single stellar population models, we find an average age of 2.33- +0.51 0.86 Gyr for the log 1 M M· > 1 galaxies in our massive and virialized cluster at z = 1.39,1.59- +0.62 1.40 Gyr in a massive but not virialized cluster at z = 1.46, and 1.20- +0.47 1.03 Gyr in a protocluster at z = 1.61. After accounting for the difference in the age of the universe between redshifts, the ages of the galaxies in the three overdensities are consistent within the errors, with possibly a weak suggestion that galaxies in the most evolved structure are older.

Review: Far-Infrared Instrumentation and Technology Development for the Next Decade

(2017)

Authors:

Duncan Farrah, Kimberly Ennico Smith, David Ardila, Charles M Bradford, Michael Dipirro, Carl Ferkinhoff, Jason Glenn, Paul Goldsmith, David Leisawitz, Thomas Nikola, Naseem Rangwala, Stephen A Rinehart, Johannes Staguhn, Michael Zemcov, Jonas Zmuidzinas, James Bartlett, Sean Carey, William J Fischer, Julia Kamenetzky, Jeyhan Kartaltepe, Mark Lacy, Dariusz C Lis, Lisa Locke, Enrique Lopez-Rodriguez, Meredith MacGregor, Elisabeth Mills, S Harvey Moseley, Eric J Murphy, Alan Rhodes, Matt Richter, Dimitra Rigopoulou, David Sanders, Ravi Sankrit, Giorgio Savini, John-David Smith, Sabrina Stierwalt

Cosmic ray acceleration by relativistic shocks: Limits and estimates

Monthly Notices of the Royal Astronomical Society Oxford University Press (2017)

Authors:

AR Bell, AT Araudo, James H Matthews, Katherine M Blundell

Abstract:

We examine limits to the energy to which cosmic rays can be accelerated by relativistic shocks, showing that acceleration of light ions as high as 100 EeV is unlikely. The implication of our estimates is that if ultra-high energy cosmic rays are accelerated by shocks, then those shocks are probably not relativistic.