Ionization, excitation, and abundance ratios in z~2-3 star-forming galaxies with KBSS-MOSFIRE

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Ionization, excitation, and abundance ratios in z~2-3 star-forming galaxies with KBSS-MOSFIRE Allison Strom (Caltech) Chuck Steidel (Caltech), Gwen Rudie (Carnegie), Naveen Reddy (UC Riverside) Ryan Trainor (UC Berkeley), Rachel Theios (Caltech)

The Keck Baryonic Structure Survey (KBSS) Specifically designed to investigate IGM/CGM and galaxies Centered on 15 of the brightest quasars in the sky (total area = 0.24 deg 2 ) Spectroscopic observations: 2354 with rest-uv spectra (LRIS) 1097 with rest-optical spectra 732 galaxies with z 2-2.7 have at least one MOSFIRE spectrum 275 galaxies with good detections of all strong diagnostic emission lines 2

Typical z~2-3 star-forming galaxies in the KBSS median stellar mass: 10 10 M median SFR: 25 M /yr median E(B-V): 0.29 ( 2 at Hα) electron density: ~200-300 cm -3 3

The [NII]-BPT diagram at z~2-3 with KBSS Strom et al. (in prep.) 4

The [NII]-BPT diagram at z~2-3 with KBSS Strom et al. (in prep.) Sanders et al. (2015) MOSDEF 4

The [SII]-BPT diagram at z~2-3 with KBSS Strom et al. (in prep.) 5

The [SII]-BPT diagram at z~2-3 with KBSS Strom et al. (in prep.) Sanders et al. (2015) MOSDEF 5

What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) [OIII]/Hβ [NII]/Hα 6

What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) higher electron density [OIII]/Hβ [NII]/Hα 6

What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) higher electron density [OIII]/Hβ [NII]/Hα 6

What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) higher electron density enhanced N/O ratios [OIII]/Hβ [NII]/Hα 6

What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) higher electron density enhanced N/O ratios [OIII]/Hβ [NII]/Hα 6

What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) higher electron density enhanced N/O ratios harder ionizing radiation [OIII]/Hβ [NII]/Hα 6

What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) higher electron density enhanced N/O ratios harder ionizing radiation [OIII]/Hβ [NII]/Hα 6

What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) [OIII]/Hβ higher electron density enhanced N/O ratios harder ionizing radiation larger ionization parameter [NII]/Hα 6

What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) [OIII]/Hβ higher electron density enhanced N/O ratios harder ionizing radiation larger ionization parameter [NII]/Hα 6

The properties of offset galaxies provide clues Strom et al. (in prep.) close detections close limits ([NII]/[SII]) offset detections offset limits ([NII]/[SII]) 7

High-z galaxies show similar N/O ratios Strom et al. (in prep.) Steidel, Rudie, Strom et al. (2014) 8

High-z galaxies show similar N/O ratios Strom et al. (in prep.) Steidel, Rudie, Strom et al. (2014) WISP Masters et al. (2014) 8

High-z galaxies show similar N/O ratios Strom et al. (in prep.) Steidel, Rudie, Strom et al. (2014) WISP Masters et al. (2014) fit to all KBSS galaxies 8

Rest-UV observations of KBSS require harder EUV Steidel, Strom, et al. (in prep.) 9

Harder EUV spectra naturally reproduce observations Strom et al. (in prep.) 10

Maiolino et al. (2008) O32 vs. R23: a look at only O and H Strom et al. (in prep.) 247 galaxies dust-corrected 11

O32 vs. R23: a look at only O and H Maiolino et al. (2008) Strom et al. (in prep.) 247 galaxies dust-corrected 11

The most offset galaxies have the highest Γ Γ= n γ /nh 12

The most offset galaxies have the highest Γ log Γ -2.9 Γ= n γ /nh 12

The most offset galaxies have the highest Γ log Γ -2.9 log Γ -3.1 Γ= n γ /nh 12

What are the physical reasons for the differences and similarities? 13

What are the physical reasons for the differences and similarities? 1. similar N/O ratios as seen at z~0: No significant difference between z~2 and z~0 is observed as a function of metallicity. 13

What are the physical reasons for the differences and similarities? 1. similar N/O ratios as seen at z~0: No significant difference between z~2 and z~0 is observed as a function of metallicity. 2. harder ionizing radiation: The same stellar population and photoionization models used to reproduce the KBSS [NII]-BPT locus also match the parameter space occupied by KBSS galaxies in the [SII]-BPT and O32-R23 diagrams. 13

What are the physical reasons for the differences and similarities? 1. similar N/O ratios as seen at z~0: No significant difference between z~2 and z~0 is observed as a function of metallicity. 2. harder ionizing radiation: The same stellar population and photoionization models used to reproduce the KBSS [NII]-BPT locus also match the parameter space occupied by KBSS galaxies in the [SII]-BPT and O32-R23 diagrams. 3. (slightly) larger ionization parameters: High-z galaxies appear to have uniformly higher O32 with the most offset galaxies exhibiting the most extreme values, which imply higher ionization parameters. 13

14