Ionization, excitation, and abundance ratios in z~2-3 star-forming galaxies with KBSS-MOSFIRE
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1 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)
2 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 have at least one MOSFIRE spectrum 275 galaxies with good detections of all strong diagnostic emission lines 2
3 Typical z~2-3 star-forming galaxies in the KBSS median stellar mass: M median SFR: 25 M /yr median E(B-V): 0.29 ( 2 at Hα) electron density: ~ cm -3 3
4 The [NII]-BPT diagram at z~2-3 with KBSS Strom et al. (in prep.) 4
5 The [NII]-BPT diagram at z~2-3 with KBSS Strom et al. (in prep.) Sanders et al. (2015) MOSDEF 4
6 The [SII]-BPT diagram at z~2-3 with KBSS Strom et al. (in prep.) 5
7 The [SII]-BPT diagram at z~2-3 with KBSS Strom et al. (in prep.) Sanders et al. (2015) MOSDEF 5
8 What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) [OIII]/Hβ [NII]/Hα 6
9 What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) higher electron density [OIII]/Hβ [NII]/Hα 6
10 What causes the [NII]-BPT offset and no change elsewhere? adapted from Kewley et al. (2013) higher electron density [OIII]/Hβ [NII]/Hα 6
11 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
12 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
13 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
14 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
15 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
16 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
17 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
18 High-z galaxies show similar N/O ratios Strom et al. (in prep.) Steidel, Rudie, Strom et al. (2014) 8
19 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
20 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
21 Rest-UV observations of KBSS require harder EUV Steidel, Strom, et al. (in prep.) 9
22 Harder EUV spectra naturally reproduce observations Strom et al. (in prep.) 10
23 Maiolino et al. (2008) O32 vs. R23: a look at only O and H Strom et al. (in prep.) 247 galaxies dust-corrected 11
24 O32 vs. R23: a look at only O and H Maiolino et al. (2008) Strom et al. (in prep.) 247 galaxies dust-corrected 11
25 The most offset galaxies have the highest Γ Γ= n γ /nh 12
26 The most offset galaxies have the highest Γ log Γ -2.9 Γ= n γ /nh 12
27 The most offset galaxies have the highest Γ log Γ -2.9 log Γ -3.1 Γ= n γ /nh 12
28 What are the physical reasons for the differences and similarities? 13
29 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
30 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
31 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
32 14
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