JADES -- The small blue bump in GN-z11: insights into the nuclear region of a galaxy at z=10.6

We report the detection of continuum excess in the rest-frame UV between 3000 {\AA} and 3550 {\AA} in the JWST/NIRSpec spectrum of GN-z11, a galaxy hosting an active galactic nucleus (AGN) at z = 10.603. The shape of the continuum excess resembles a Balmer continuum but has a break around 3546 {\AA}...

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Hauptverfasser: Ji, Xihan, Maiolino, Roberto, Ferland, Gary, D'Eugenio, Francesco, Bhatawdekar, Rachana, Charlot, Stéphane, Chevallard, Jacopo, Curti, Mirko, Curtis-Lake, Emma, Hainline, Kevin, Ji, Zhiyuan, Robertson, Brant, Del Pino, Bruno Rodríguez, Scholtz, Jan, Tacchella, Sandro, Williams, Christina C, Witstok, Joris
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creator Ji, Xihan
Maiolino, Roberto
Ferland, Gary
D'Eugenio, Francesco
Bhatawdekar, Rachana
Charlot, Stéphane
Chevallard, Jacopo
Curti, Mirko
Curtis-Lake, Emma
Hainline, Kevin
Ji, Zhiyuan
Robertson, Brant
Del Pino, Bruno Rodríguez
Scholtz, Jan
Tacchella, Sandro
Williams, Christina C
Witstok, Joris
description We report the detection of continuum excess in the rest-frame UV between 3000 {\AA} and 3550 {\AA} in the JWST/NIRSpec spectrum of GN-z11, a galaxy hosting an active galactic nucleus (AGN) at z = 10.603. The shape of the continuum excess resembles a Balmer continuum but has a break around 3546 {\AA} in the rest frame, which is 100 {\AA} bluewards to the Balmer limit at 3646 {\AA}. A Balmer continuum model alone cannot fit the spectrum, implying a different origin for the continuum excess. The absence of the Balmer jump indicates an electron temperature of $\sim 3\times 10^4$ K, which is significantly higher than the temperature of $T_{e}({\rm O^{2+}}) \approx 1.3\times 10^{4}$ K inferred from [OIII]$\lambda 4363$. The temperature difference must result from mixing of different ionized regions: the Balmer emission mainly arises from dense and hot clouds in the Broad Line Region, close to the accreting black hole, whereas the forbidden lines originate from less dense and colder gas in the host galaxy (although these ionized regions are kinematically similar in GN-z11 due to its small BH mass). We propose a potential explanation for the observed continuum excess to come from a complex of FeII emission, which shows a characteristic jump bluewards to the Balmer limit as previously seen in the spectra of many lower-redshift quasars. Through comparisons with Cloudy models, we show an Fe abundance or an overall metallicity above $\sim 1/3$ solar is likely needed. Besides the FeII emission, part of the small blue bump might also be associated with an OIII Bowen fluorescent line, a line often enhanced in dense AGN-ionized gas. Finally, the spectrum provides further evidence against Wolf-Rayet or massive stars dominating the nebular emission in GN-z11.
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The shape of the continuum excess resembles a Balmer continuum but has a break around 3546 {\AA} in the rest frame, which is 100 {\AA} bluewards to the Balmer limit at 3646 {\AA}. A Balmer continuum model alone cannot fit the spectrum, implying a different origin for the continuum excess. The absence of the Balmer jump indicates an electron temperature of $\sim 3\times 10^4$ K, which is significantly higher than the temperature of $T_{e}({\rm O^{2+}}) \approx 1.3\times 10^{4}$ K inferred from [OIII]$\lambda 4363$. The temperature difference must result from mixing of different ionized regions: the Balmer emission mainly arises from dense and hot clouds in the Broad Line Region, close to the accreting black hole, whereas the forbidden lines originate from less dense and colder gas in the host galaxy (although these ionized regions are kinematically similar in GN-z11 due to its small BH mass). We propose a potential explanation for the observed continuum excess to come from a complex of FeII emission, which shows a characteristic jump bluewards to the Balmer limit as previously seen in the spectra of many lower-redshift quasars. Through comparisons with Cloudy models, we show an Fe abundance or an overall metallicity above $\sim 1/3$ solar is likely needed. Besides the FeII emission, part of the small blue bump might also be associated with an OIII Bowen fluorescent line, a line often enhanced in dense AGN-ionized gas. 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The shape of the continuum excess resembles a Balmer continuum but has a break around 3546 {\AA} in the rest frame, which is 100 {\AA} bluewards to the Balmer limit at 3646 {\AA}. A Balmer continuum model alone cannot fit the spectrum, implying a different origin for the continuum excess. The absence of the Balmer jump indicates an electron temperature of $\sim 3\times 10^4$ K, which is significantly higher than the temperature of $T_{e}({\rm O^{2+}}) \approx 1.3\times 10^{4}$ K inferred from [OIII]$\lambda 4363$. The temperature difference must result from mixing of different ionized regions: the Balmer emission mainly arises from dense and hot clouds in the Broad Line Region, close to the accreting black hole, whereas the forbidden lines originate from less dense and colder gas in the host galaxy (although these ionized regions are kinematically similar in GN-z11 due to its small BH mass). We propose a potential explanation for the observed continuum excess to come from a complex of FeII emission, which shows a characteristic jump bluewards to the Balmer limit as previously seen in the spectra of many lower-redshift quasars. Through comparisons with Cloudy models, we show an Fe abundance or an overall metallicity above $\sim 1/3$ solar is likely needed. Besides the FeII emission, part of the small blue bump might also be associated with an OIII Bowen fluorescent line, a line often enhanced in dense AGN-ionized gas. 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The shape of the continuum excess resembles a Balmer continuum but has a break around 3546 {\AA} in the rest frame, which is 100 {\AA} bluewards to the Balmer limit at 3646 {\AA}. A Balmer continuum model alone cannot fit the spectrum, implying a different origin for the continuum excess. The absence of the Balmer jump indicates an electron temperature of $\sim 3\times 10^4$ K, which is significantly higher than the temperature of $T_{e}({\rm O^{2+}}) \approx 1.3\times 10^{4}$ K inferred from [OIII]$\lambda 4363$. The temperature difference must result from mixing of different ionized regions: the Balmer emission mainly arises from dense and hot clouds in the Broad Line Region, close to the accreting black hole, whereas the forbidden lines originate from less dense and colder gas in the host galaxy (although these ionized regions are kinematically similar in GN-z11 due to its small BH mass). We propose a potential explanation for the observed continuum excess to come from a complex of FeII emission, which shows a characteristic jump bluewards to the Balmer limit as previously seen in the spectra of many lower-redshift quasars. Through comparisons with Cloudy models, we show an Fe abundance or an overall metallicity above $\sim 1/3$ solar is likely needed. Besides the FeII emission, part of the small blue bump might also be associated with an OIII Bowen fluorescent line, a line often enhanced in dense AGN-ionized gas. Finally, the spectrum provides further evidence against Wolf-Rayet or massive stars dominating the nebular emission in GN-z11.</abstract><doi>10.48550/arxiv.2405.05772</doi><oa>free_for_read</oa></addata></record>
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title JADES -- The small blue bump in GN-z11: insights into the nuclear region of a galaxy at z=10.6
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