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Abstract: The ionizing photons produced by massive stars are key actors in galaxy evolu9on. Ionizing photon produc9on and escape is poorly understood. Improved space-based, spa9ally-resolved, mul9plexed spectroscopic capabili9es covering λ obs = 1000–3000 Å, in concert with spectroscopy from the ELTs and JWST, would lead to defini9ve answers as to how ionizing photons are produced and leaked, what popula9ons of galaxies are responsible for ionizing photon leakage, what determines whether escape is possible, and how ionizing galaxy popula9ons evolve over cosmic 9me. In-hand UV spectra of bright gravita9onally lensed galaxies demonstrate this science. This poster is an adapta1on of our Astro2020 white paper (Rigby et al.) The produc9on and escape of ionizing photons from galaxies over cosmic 9me: Demonstra9ng science for future missions using in-hand UV spectra of lensed galaxies Jane Rigby (NASA Goddard), MaO Bayliss (MIT), Danielle Berg (OSU), Rongmon Bordoloi (NCSU), John Chisholm (UCSC), Michael Florian (NASA Goddard), MaOhew Hayes (Stockholm U.), Michael Gladders (U. Chicago), Bethan James (STScI), Sangeeta Malhotra (NASA Goddard), Sally Oey (U. Michigan), John O’Meara (Keck Observatory), Emil Rivera-Thorsen (U. Oslo), K. Sharon (U. Michigan) Key Science Ques;ons: How do galaxies produce ionizing photons? How do ionizing photons escape from galaxies? Which galaxies leak ionizing photons? Which galaxies reionized the Universe? What about those galaxies permiOed ionizing photons to escape? 1. Ionizing photons are important. The Universe was re-ionized; therefore there must have been enough ionizing photons to do the job, and to keep the Universe ionized at later epochs. Studying galaxies in the epoch of reioniza9on is a key science goal for JWST, which will characterize the galaxy luminosity func9on and measure physical proper9es like densi9es and metallici9es. However, JWST will be unable to measure the ionizing fluxes of galaxies at high redshie, for a simple reason: the opacity of the intergalac9c medium prevents ionizing photons from z4 from reaching Earth. Only at redshies z4 is it possible to measure ionizing flux from galaxies (see Fig. 9 of Steidel et al. 2018). Ionizing photons are produced by main sequence and evolved massive stars. The ionizing photons ionize the H II regions, power the strong nebular emission lines that are key diagnos9cs of galaxy evolu9on, and if there are clear channels, escape their parent galaxy. The massive stars that produce the ionizing photons also produce the non-ionizing ultraviolet con9nuum, nucleosynthesize the heavier elements, and distribute those elements through a combina9on of stellar winds and supernovae winds. Aeer heroic effort, 36 galaxies have been spectroscopically iden9fied to "leak" ionizing photons, spanning redshies from z~0 to z~3 (Leitet et al. 2011; Borthakur et al. 2014; Vanzella et al. 2015, 2016, 2018; Izotov et al. 2016 a,b; Leitherer et al. 2016; Shapley et al. 2016; Bian et al. 2017; Izotov et al. 2018 a, b; Steidel et al. 2018; Rivera-Thorsen et al. 2019; Figure 1). We are just beginning to learn what kinds of galaxies might have reionized the Universe. 3. Ionizing photons can escape galaxies. How? Neutral H atoms absorb ionizing photons, which blocks their escape. To escape, ionizing photons can travel through clear channels (or highly ionized channels) in the gas, or can stream out of density-bounded H II regions that are smaller than their Strömgren radii (Figure 3). Ionizing photons from galaxy outskirts should have an easier 9me escaping (Keenan et al. 2017), and could play an outsized role. It is not understood whether escape is determined by local factors (star forma9on history, nebular geometry and ioniza9on) or large-scale factors (halo mass, galaxy mergers, environment), nor is the role of feedback understood. Do the massive stars break open their own neutral gas shells, like hatchlings, or is the neutral gas torn open by large-scale galac9c events? How important is the higher UV background at higher redshie at weakening the shells? Do numerous small “eggs” dominate ionizing photon escape, or the most luminous ones? Lyman alpha is an indirect probe of the neutral gas (Verhamme et al. 2006; Jaskot & Oey 2014; Rivera-Thorsen et al. 2017b, Yang et al. 2016, 2017). Several other indirect predictors of escape have been suggested. 4. These science ques;ons can be solved, defini;vely, over cosmic ;me. 1) RedshiO 0.1<z<1.5: The ionizing UV and non-ionizing UV can only be captured from space. Crucial measurements are sub-arcs spa9ally resolved spectra, covering λ rest = 1000–3000Å at R=5000 and SNR > 15 per resoln. element, and the ionizing λ rest = 900Å region at R~100s. Cri9cal goals are to spa9ally resolve which star- forming regions are responsible for the ionizing photons, and measure proper9es of star-forming regions (Z, stellar age, SFR). Spa9ally resolving ionizing emission is the only way to directly determine the physical processes of escape and the role of feedback. Stretching the wavelength coverage as blue as possible, to measure the ionizing spectral slope, would constrain key unknowns about massive star evolu9on. 2) RedshiO 1.5<z<2.5: Mul9-object spectroscopic surveys with 20–30m ground-based ELTs will obtain the rest- frame non-ionizing UV spectra of large numbers of galaxies, at seeing-limited resolu9on, and thus characterize their massive stellar popula9ons, as well as diagnos9cs of nebular condi9ons and gas inflow and ouxlows (e.g. Shapley et al. 2003; Pezni et al. 2000; Rigby et al. 2019b). The ELTS will also cover Ly ɑ over most of this redshie range. However, the ELTs cannot measure the ionizing con9nua for any of these galaxies — this must be done from space, and would require sensi9ve, low spectral resolu9on, spa9ally resolved spectroscopy of these galaxies with a space telescope at λ rest = 900Å, which at these redshies is λ obs = 2200–3150Å. 3) RedshiO 2.5<z<3: The ELTs will capture the ionizing flux of large numbers of galaxies in the very blue op9cal (λ obs = 3200–3600Å), and their non-ionizing rest-frame UV spectra (λ rest = 1200–3000Å) in the op9cal and near-IR (λ obs = 4200–12000Å). This measurement would prove especially difficult if faint galaxies are responsible for the bulk of ionizing photon produc9on. These measurements would be seeing-limited, and therefore would lack spa9al informa9on as to which parts of galaxies leak ionizing photons. 4) RedshiOs 7<z<9: In long integra9ons, the ELTs and JWST will obtain non-ionizing rest-frame UV and rest-frame op9cal spectral diagnos9cs of galaxies at the reioniza9on epoch, including indirect predictors of ionizing escape. The inves9ga9ons discussed in the previous 3 points would provide a much deeper understanding of ionizing photon produc9on and escape for redshies 0<z<3. It would then be possible to apply this knowledge to the ELT and JWST observa9ons of the epoch of reioniza9on, to comprehensively determine which galaxies reionized the Universe. To summarize, the produc9on of ionizing photons by massive stars, and their escape from galaxies, are key unsolved issues in our understanding of galaxy evolu9on and how the Universe was reionized. Only a systema9c approach, using JWST and the ELTs at the highest redshies, using the ELTs at 1.5<z<3, and a future UV space observatory, can comprehensively measure the massive stellar popula9ons within star-forming galaxies, determine which kinds of galaxies leak ionizing photons and how to predict that escape, and apply that knowledge to finally understand which galaxies ended the dark ages by reionizing the Universe. Facilities needed Capabilities JWST Deep NIRSpec and MIRI spectra of rest-frame optical diagnostics of galaxies at reionization ELTs Multiplexed spectroscopic surveys covering λobs = 3200-12000Å Large space UV telescope (LUVOIR, HabEx) Spatially-resolved spectroscopy that covers the ionizing λrest = 900Å, λobs = 1000–3000Å, at low spectral resolution (R~100s) Large space UV telescope (LUVOIR, HabEx) Spatially-resolved spectroscopy that covers λobs = 1000–3000Å at R~5000 and SNR > 20 per resolution element Figure 1: Left panel: The gravitationally lensed Sunburst Arc at z=2.4. Right panel: Ionizing photons escape from a compact, rapidly star-forming region. Adapted from Rivera-Thorsen et al. (2019) 2. Massive stars make ionizing photons. The non-ionizing UV spectra of galaxies features a rich suite of diagnos9cs of the hot stars, namely broad He II emission, the P Cygni profiles of C IV, Si IV, and N V, and photospheric absorp9on lines (deMello et al. 2000; Crowther et al. 2016). We have demonstrated (Chisholm et al. 2019) that we can measure the age and metallicity of hot stellar popula9ons by fizng high-quality rest-frame UV spectra of z~2 lensed galaxies (Rigby et al. 2018). Different stellar popula9on synthesis models, when fizng the same high-quality spectra, differ by factors of several in the predicted ionizing photon produc9on rate and the ionizing spectral slope λ rest <900Å (Chisholm et al. 2019; Figure 2). In other words, the current unknowns about massive stellar popula9ons translate to factors-of-several uncertainty in the expected ionizing photon produc9on rates of galaxies. We need to beOer characterize the massive stellar popula9ons within star-forming galaxies, their intrinsic ionizing produc9on rate, and what determines whether those ionizing photons are trapped or can escape. Figure 2: λrest= 1000–2000Å galaxy spectra reveal the age and metallicity of the massive stellar population, by fitting stellar population synthesis (SPS) models. Current SPS models disagree by factors-of- several in the amount of ionizing radiation that should be produced by a given young stellar population. This disagreement is due to fundamental uncertainties about massive stellar evolution and spectra. From Chisholm et al. (2019), using z~2 lensed galaxy spectra from Megasaura (Rigby et al. 2018a). Figure 3: Two different scenarios for how ionizing photons could escape. Left: while most sight-lines are blocked by neutral gas along, narrow channels permit escape. Right: the ionizing photons overwhelm the small amount of gas available, such that the H II region is smaller than its Strömgren sphere (“density-bounded”), and ionizing photons can freely stream out.

The produc9on and escape of ionizing photons from galaxies ... · This poster is an adapta1on of our Astro2020 white paper (Rigby et al.) ... et al. 2016, 2017). Several other indirect

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Page 1: The produc9on and escape of ionizing photons from galaxies ... · This poster is an adapta1on of our Astro2020 white paper (Rigby et al.) ... et al. 2016, 2017). Several other indirect

Abstract:Theionizingphotonsproducedbymassivestarsarekeyactorsingalaxyevolu9on.Ionizingphotonproduc9onandescapeispoorlyunderstood.Improvedspace-based,spa9ally-resolved,mul9plexedspectroscopiccapabili9escoveringλobs=1000–3000Å,inconcertwithspectroscopyfromtheELTsandJWST,wouldleadtodefini9veanswersastohowionizingphotonsareproducedandleaked,whatpopula9onsofgalaxiesareresponsibleforionizingphotonleakage,whatdetermineswhetherescapeispossible,andhowionizinggalaxypopula9onsevolveovercosmic9me.In-handUVspectraofbrightgravita9onallylensedgalaxiesdemonstratethisscience.Thisposterisanadapta1onofourAstro2020whitepaper(Rigbyetal.)

Theproduc9onandescapeofionizingphotonsfromgalaxiesovercosmic9me:Demonstra9ngscienceforfuturemissionsusingin-handUVspectraoflensedgalaxiesJaneRigby(NASAGoddard),MaOBayliss(MIT),DanielleBerg(OSU),RongmonBordoloi(NCSU),JohnChisholm(UCSC),MichaelFlorian(NASAGoddard),MaOhewHayes(StockholmU.),MichaelGladders(U.Chicago),BethanJames(STScI),SangeetaMalhotra(NASAGoddard),SallyOey(U.Michigan),JohnO’Meara(KeckObservatory),EmilRivera-Thorsen(U.Oslo),K.Sharon(U.Michigan)

KeyScienceQues;ons:• Howdogalaxiesproduceionizingphotons?

• Howdoionizingphotonsescapefromgalaxies?

• Whichgalaxiesleakionizingphotons?WhichgalaxiesreionizedtheUniverse?

• WhataboutthosegalaxiespermiOedionizingphotonstoescape?

1.Ionizingphotonsareimportant. TheUniversewasre-ionized;thereforetheremusthavebeenenoughionizingphotonstodothejob,andtokeeptheUniverseionizedatlaterepochs.Studyinggalaxiesintheepochofreioniza9onisakeysciencegoalforJWST,whichwillcharacterizethegalaxyluminosityfunc9onandmeasurephysicalproper9eslikedensi9esandmetallici9es.However,JWSTwillbeunabletomeasuretheionizingfluxesofgalaxiesathighredshie,forasimplereason:theopacityoftheintergalac9cmediumpreventsionizingphotonsfromz⪅4fromreachingEarth.Onlyatredshiesz⪅4isitpossibletomeasureionizingfluxfromgalaxies(seeFig.9ofSteideletal.2018).

Ionizingphotonsareproducedbymainsequenceandevolvedmassivestars.TheionizingphotonsionizetheHIIregions,powerthestrongnebularemissionlinesthatarekeydiagnos9csofgalaxyevolu9on,andifthereareclearchannels,escapetheirparentgalaxy.Themassivestarsthatproducetheionizingphotonsalsoproducethenon-ionizingultravioletcon9nuum,nucleosynthesizetheheavierelements,anddistributethoseelementsthroughacombina9onofstellarwindsandsupernovaewinds. Aeerheroiceffort,36galaxieshavebeenspectroscopicallyiden9fiedto"leak"ionizingphotons,spanningredshiesfromz~0toz~3(Leitetetal.2011;Borthakuretal.2014;Vanzellaetal.2015,

2016,2018;Izotovetal.2016a,b;Leithereretal.2016;Shapleyetal.2016;Bianetal.2017;Izotovetal.2018a,b;Steideletal.2018;Rivera-Thorsenetal.2019;Figure1).WearejustbeginningtolearnwhatkindsofgalaxiesmighthavereionizedtheUniverse.

3.Ionizingphotonscanescapegalaxies.How?NeutralHatomsabsorbionizingphotons,whichblockstheirescape.Toescape,ionizingphotonscantravelthroughclearchannels(orhighlyionizedchannels)inthegas,orcanstreamoutofdensity-boundedHIIregionsthataresmallerthantheirStrömgrenradii(Figure3).Ionizingphotonsfromgalaxyoutskirtsshouldhaveaneasier9meescaping(Keenanetal.2017),andcouldplayanoutsizedrole.Itisnotunderstoodwhetherescapeisdeterminedbylocalfactors(star

forma9onhistory,nebulargeometryandioniza9on)orlarge-scalefactors(halomass,galaxymergers,environment),noristheroleoffeedbackunderstood.Dothemassivestarsbreakopentheirownneutralgasshells,likehatchlings,oristheneutralgastornopenbylarge-scalegalac9cevents?HowimportantisthehigherUVbackgroundathigherredshieatweakeningtheshells?Donumeroussmall“eggs”dominateionizingphotonescape,orthemostluminousones? Lymanalphaisanindirectprobeoftheneutralgas(Verhammeetal.2006;Jaskot&Oey2014;Rivera-Thorsenetal.2017b,Yangetal.2016,2017).Severalotherindirectpredictorsofescapehavebeensuggested.

4.Thesescienceques;onscanbesolved,defini;vely,overcosmic;me.1)RedshiO0.1<z<1.5:TheionizingUVandnon-ionizingUVcanonlybecapturedfromspace.Crucialmeasurementsaresub-arcsspa9allyresolvedspectra,coveringλrest=1000–3000ÅatR=5000andSNR>15perresoln.element,andtheionizingλrest=900ÅregionatR~100s.Cri9calgoalsaretospa9allyresolvewhichstar-formingregionsareresponsiblefortheionizingphotons,andmeasureproper9esofstar-formingregions(Z,stellarage,SFR).Spa9allyresolvingionizingemissionistheonlywaytodirectlydeterminethephysicalprocessesofescapeandtheroleoffeedback.Stretchingthewavelengthcoverageasblueaspossible,tomeasuretheionizingspectralslope,wouldconstrainkeyunknownsaboutmassivestarevolu9on.

2)RedshiO1.5<z<2.5:Mul9-objectspectroscopicsurveyswith20–30mground-basedELTswillobtaintherest-framenon-ionizingUVspectraoflargenumbersofgalaxies,atseeing-limitedresolu9on,andthuscharacterizetheirmassivestellarpopula9ons,aswellasdiagnos9csofnebularcondi9onsandgasinflowandouxlows(e.g.Shapleyetal.2003;Peznietal.2000;Rigbyetal.2019b).TheELTSwillalsocoverLyɑovermostofthisredshierange.However,theELTscannotmeasuretheionizingcon9nuaforanyofthesegalaxies—thismustbedonefromspace,andwouldrequiresensi9ve,lowspectralresolu9on,spa9allyresolvedspectroscopyofthesegalaxieswithaspacetelescopeatλrest=900Å,whichattheseredshiesisλobs=2200–3150Å.

3)RedshiO2.5<z<3:TheELTswillcapturetheionizingfluxoflargenumbersofgalaxiesintheveryblueop9cal(λobs=3200–3600Å),andtheirnon-ionizingrest-frameUVspectra(λrest=1200–3000Å)intheop9calandnear-IR(λobs=4200–12000Å).Thismeasurementwouldproveespeciallydifficultiffaintgalaxiesareresponsibleforthebulkofionizingphotonproduc9on.Thesemeasurementswouldbeseeing-limited,andthereforewouldlackspa9alinforma9onastowhichpartsofgalaxiesleakionizingphotons.

4)RedshiOs7<z<9:Inlongintegra9ons,theELTsandJWSTwillobtainnon-ionizingrest-frameUVandrest-frameop9calspectraldiagnos9csofgalaxiesatthereioniza9onepoch,includingindirectpredictorsofionizingescape.Theinves9ga9onsdiscussedintheprevious3pointswouldprovideamuchdeeperunderstandingofionizingphotonproduc9onandescapeforredshies0<z<3.ItwouldthenbepossibletoapplythisknowledgetotheELTandJWSTobserva9onsoftheepochofreioniza9on,tocomprehensivelydeterminewhichgalaxiesreionizedtheUniverse.

Tosummarize,theproduc9onofionizingphotonsbymassivestars,andtheirescapefromgalaxies,arekeyunsolvedissuesinourunderstandingofgalaxyevolu9onandhowtheUniversewasreionized.Onlyasystema9capproach,usingJWSTandtheELTsatthehighestredshies,usingtheELTsat1.5<z<3,andafutureUVspaceobservatory,cancomprehensivelymeasurethemassivestellarpopula9onswithinstar-forminggalaxies,determinewhichkindsofgalaxiesleakionizingphotonsandhowtopredictthatescape,andapplythatknowledgetofinallyunderstandwhichgalaxiesendedthedarkagesbyreionizingtheUniverse.

Facilities needed Capabilities

JWST Deep NIRSpec and MIRI spectra of rest-frame optical diagnostics of galaxies at reionization

ELTs Multiplexed spectroscopic surveys covering λobs = 3200-12000Å

Large space UV telescope (LUVOIR, HabEx) Spatially-resolved spectroscopy that covers the ionizing λrest = 900Å, λobs = 1000–3000Å, at low spectral resolution (R~100s)

Large space UV telescope (LUVOIR, HabEx) Spatially-resolved spectroscopy that covers λobs = 1000–3000Å at R~5000 and SNR > 20 per resolution element

Figure 1:  Left panel: The gravitationally lensed Sunburst Arc at z=2.4.  Right panel: Ionizing photons escape from a compact, rapidly star-forming region.  Adapted from Rivera-Thorsen et al. (2019)

2.Massivestarsmakeionizingphotons. Thenon-ionizingUVspectraofgalaxiesfeatures

arichsuiteofdiagnos9csofthehotstars,namelybroadHeIIemission,thePCygniprofilesofCIV,SiIV,andNV,andphotosphericabsorp9onlines(deMelloetal.2000;Crowtheretal.2016).

Wehavedemonstrated(Chisholmetal.2019)thatwecanmeasuretheageandmetallicityofhotstellarpopula9onsbyfiznghigh-qualityrest-frameUVspectraofz~2lensedgalaxies(Rigbyetal.2018). Differentstellarpopula9onsynthesismodels,whenfizngthesamehigh-qualityspectra,differbyfactorsofseveralinthepredictedionizingphotonproduc9onrateandtheionizingspectralslopeλrest<900Å(Chisholmetal.2019;Figure2).Inotherwords,thecurrentunknownsaboutmassivestellarpopula9onstranslatetofactors-of-severaluncertaintyintheexpectedionizingphotonproduc9onratesofgalaxies.WeneedtobeOercharacterizethemassivestellarpopula9onswithinstar-forminggalaxies,theirintrinsicionizingproduc9onrate,andwhatdetermineswhetherthoseionizingphotonsaretrappedorcanescape.

Figure 2:   λrest= 1000–2000Å galaxy spectra reveal the age and metallicity of the massive stellar population, by fitting stellar population synthesis (SPS) models.  Current SPS models disagree by factors-of-several in the amount of ionizing radiation that should be produced by a given young stellar population. This disagreement is due to fundamental uncertainties about massive stellar evolution and spectra. From Chisholm et al. (2019), using z~2 lensed galaxy spectra from Megasaura (Rigby et al. 2018a).

Figure 3: Two different scenarios for how ionizing photons could escape.  Left: while most sight-lines are blocked by neutral gas along, narrow channels permit escape.  Right: the ionizing photons overwhelm the small amount of gas available, such that the H II region is smaller than its Strömgren sphere (“density-bounded”), and ionizing photons can freely stream out.