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			<titleStmt><title level='a'>TeV Detection of the Extreme HSP Blazar RBS 1366 by VERITAS</title></titleStmt>
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				<publisher>Sissa Medialab</publisher>
				<date>08/17/2023</date>
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				<bibl> 
					<idno type="par_id">10482683</idno>
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					<author>Deivid Ribeiro</author><author>Icrc2023</author>
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			<abstract><ab><![CDATA[Extreme high-synchrotron-peak blazars (EHSPs) are postulated as the most efficient and extremeparticle accelerators in the universe but remain enigmatic as a possible new class of TeV gamma-ray blazars. Blazars are active galactic nuclei (AGNs) with jets of relativistic particles thatgenerate non-thermal emission pointed along the line-of-sight. Their spectral energy distribution(SED) are characterized by synchrotron and inverse-Compton peaks, indicating acceleration ofleptonic and possibly hadronic particle populations in the jet. EHSPs are characterized by apeak synchrotron frequency > 1017 Hz with their Compton peak expected to fall in the TeVrange. Indeed, the handful of EHSPs detected by Imaging Air Cherenkov Telescopes (IACTs)have presented challenges where some may be a high-frequency extension of the blazar sequencewhile others peaking around 10 TeV may represent a different class of TeV emitters. Detectionsof the high-energy and very-high-energy (HE; E > 100 MeV, VHE; E > 100 GeV) componentsof the Compton peak will play an important role in constraining the acceleration model derivedfrom the SED. We present the discovery of TeV emission from RBS 1366, a candidate EHSP,by the VERITAS observatory. Using HE and VHE data from the Fermi-LAT and VERITASobservatories, respectively, we characterize the detection by providing an SED and model fit inthe context of other EHSP candidates. Our work confirms the status of RBS 1366 as an EHBL.]]></ab></abstract>
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<div xmlns="http://www.tei-c.org/ns/1.0"><head n="1.">Introduction</head><p>Blazars are a subclass of active galactic nuclei with relativistic jets pointed toward the observer, emitting gamma rays in the very-high-energy (VHE; E&gt;100 GeV) or "TeV" regime. The underlying mechanisms for the emission of these gamma rays are evident in the observed spectral energy distribution (SED), which is modeled to include the underlying particle populations, and acceleration and cooling mechanisms in the jets.</p><p>It is commonly understood that the low energy and high energy peaks of the SED are produced by synchrotron and inverse Compton processes, respectively <ref type="bibr">[1]</ref>. In this synchrotron self-compton model (SSC), a population of electrons emit synchrotron radiation and then the same electron population emit gamma rays through Inverse Compton scattering the synchrotron photons.</p><p>At a redshift of &#119911; = 0.2365, RBS 1366 is an AGN in giant elliptical host galaxy with a central black hole mass of 9.31 &#177; 0.32 M &#8857; <ref type="bibr">[2]</ref>. RBS 1366 has been a prime candidate for detection and classification as an EHSP <ref type="bibr">[3]</ref><ref type="bibr">[4]</ref><ref type="bibr">[5]</ref>. It was selected for VERITAS observation based on the high synchrotron peak frequency in the Swift XRT X-ray band (&gt; 10 17 Hz), along with detection in the 20 MeV to 300 GeV Fermi-LAT band displaying a hard spectrum (and placement in the 3FHL catalog <ref type="bibr">[6]</ref>). RBS 1366 was expected to behave very much like the EHBL 1ES 0229+200 (see Table <ref type="table">1</ref> of <ref type="bibr">[5]</ref>) with a measured a redshift of z = 0.237 based on Ca II, G band, Fe I, Mg I and Na absorption <ref type="bibr">[7]</ref>. In the 1-300 GeV band, Toomey (2020) <ref type="bibr">[3]</ref> found a power law fit with normalization &#119896; = (7.20 &#177; 1.65) &#215; 10 -11 cm -2 s -1 GeV -1 and index &#120574; = 1.63 &#177; 0.08.</p><p>It is notable that a VERITAS upper limit has been reported <ref type="bibr">[5,</ref><ref type="bibr">8]</ref>, anticipating that a detection of this source with an accompanying spectrum would enable further EHSP characterization. A differential upper limit of 1.7 &#215; 10 -11 cm -1 s -1 erg -1 at 327 GeV was calculated for this source by VERITAS based on 10 hours of observations in 2016 <ref type="bibr">[8]</ref>.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="2.">Methods</head></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="2.1">Fermi-LAT</head><p>The Large Area Telescope (LAT) on board the Fermi satellite has operated since 2008 <ref type="bibr">[9]</ref>. It is sensitive to photons between &#8764;20 MeV and &#8764;1 TeV and has an &#8764;60&#176;field of view, enabling it to survey the entire sky in about 3 hours.</p><p>RBS 1366 was observed from 2008 to 2023, where the data was fit with a power law as the base spectral model. The Fermi-LAT 4FGL catalog defines this source as J1417.9+2543 located at 14 &#8462; 17 &#119898; 58.6 &#119904; , 25 &#8226; 43 &#8242; 26 &#8242;&#8242; .</p><p>The publicly available Fermi-LAT data were analyzed using with the Fermitools suite of tools provided by the Fermi Science Support Center (FSSC). Using the Fermipy analysis package <ref type="bibr">[10]</ref>1, the data were prepared for a binned likelihood analysis in which a spatial spectral model is fit over the energy bins. The data were selected using the SOURCE class of events, which are optimized for point-source analysis, within an angle of 15&#176;from the analysis target position. A 90&#176;zenith angle cut was applied to remove any external background events due to the effect of the Earth. The standard background models were applied to the test model, incorporating an isotropic</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>PoS(ICRC2023)659</head></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>VERITAS Detection of RBS 1366</head><p>Deivid Ribeiro background and a galactic diffuse emission model without any modifications (&#119892;&#119897;&#119897;_&#119894;&#119890;&#119898;_&#119907;07 and &#119894;&#119904;&#119900;_&#119875;8&#119877;3_&#119878;&#119874;&#119880; &#119877;&#119862;&#119864;_&#119881;2_&#119907;1). The standard 4FGL catalog was then queried for sources within the field of view and their default model parameters <ref type="bibr">[11]</ref>. With the improvements to Fermi-LAT low-energy sensitivity in PASS8 reconstruction, the energy range was expanded to 100 MeV -1 TeV.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="2.2">VERITAS</head><p>The Very Energetic Radiation Imaging Telescope Array System (VERITAS) is an Imaging Atmospheric Cherenkov Telescope (IACT) array consisting of four 12 m telescopes separated by approximately 100 m, at the Fred Lawrence Whipple Observatory (FLWO) in southern Arizona, USA <ref type="bibr">[12,</ref><ref type="bibr">13]</ref>. The observatory is sensitive to photons within the energy range &#8765;100 GeV to &#8765;30 TeV, with the ability to detect 1% of the emission of the Crab Nebula in 25 hours (at 5&#120590;). The instrument has an angular resolution (68% containment) of &#8765;0.1&#176;at 1 TeV, an energy resolution of &#8765;15% at 1 TeV, and 3.5&#176;field of view.</p><p>VERITAS observed RBS 1366 for 56 hr between 2008 and 2021, under dark sky conditions. The data in this paper were taken using "wobble" pointing mode, where the source is offset from the center of the camera by 0.5&#176;. This mode creates space for a radially symmetric "off" region to be used for background estimation in the same field of view, saving time from targeted background observations that contain the same data observing conditions.</p><p>The data were processed with standard VERITAS calibration and reconstruction pipelines, and then cross-checked with a separate analysis chain <ref type="bibr">[14,</ref><ref type="bibr">15]</ref>. Specifically, we used an Image Template Method (ITM) to improve event angular and energy reconstruction <ref type="bibr">[16]</ref>, where analysis cuts are determined with a set of a priori data-selection cuts optimized on sources with a soft power law index (from 2.5 to 3).</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="3.">Results</head></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="3.1">Fermi-LAT</head><p>Using the Fermi-LAT data from this work, RBS 1366 (as 4FGL J1417+2543) was detected with a test statistic TS=353.9 (&#8764; 18&#120590;) over an observation period of 14.5 years in the energy range from 100 GeV to 1 TeV. The source was fit to a power law model &#119889;&#119899;/&#119889;&#119864; = (4.13 &#177; 0.76 &#215; 10 -15 ) (&#119864;/10.4 GeV) -1.6&#177;0.1 MeV -1 cm -2 s -1 . The spectrum is shown in the left of Figure <ref type="figure">1</ref>.</p><p>RBS 1366 was also tested for time variability by constructing a light curve over the entire observing period in 6 month bins, integrating over the same energy range of 100 GeV to 1 TeV. The light curve is binned into periods determined by the Bayesian Blocks algorithm where a false alarm rate of &#119901;0 = 0.0027 (equivalent to 3 sigma) is used to compute the prior of the number of bins, yielding 3 bins of relative stability, see Figure <ref type="figure">2</ref> <ref type="bibr">[17]</ref>. This is consistent with the 4FGL catalog entry for RBS 1366, where the variability index is measured to be 17.4 (an index above 24.72 over 12 intervals indicates &lt;1% chance of being a steady source <ref type="bibr">[18]</ref>).</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>PoS(ICRC2023)659</head><p>VERITAS Detection of RBS 1366  <ref type="bibr">[19]</ref>, for redshift z=0.237 <ref type="bibr">[7]</ref>. For low significance bins (TS&lt;1), the Rolke upper limit is derived for a power law of index 2.5, and is not included in the overall fit of the larger energy range <ref type="bibr">[20]</ref>.</p><note type="other">Deivid Ribeiro</note></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="3.2">VERITAS</head><p>VERITAS has detected RBS 1366 at a significance of 6.5 sigma or standard deviation, with an exposure of 56.8 hours. A summary of the detection is shown in Table <ref type="table">1</ref>. The observed spectrum was fit to a power law model, shown in Figure <ref type="figure">1</ref>.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>Table 1:</head><p>Summary of VERITAS detection. The quality-selected live time, number of gamma-ray-like events in the on-and off-source regions, the normalization for the larger off-source region, the observed excess of gamma-rays and the corresponding statistical significance are shown. For each observation epoch, the integral flux corresponding to the observed excess is given. The flux is reported above the observation threshold of 200 GeV, and is also given in percentage of Crab Nebula flux above the same threshold.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>Epoch</head><p>T On Off Norm Excess Significance Flux (&gt;200 GeV) Crab [hr]</p><p>[&#120590;] [10 -12 cm -2 s -1 ] % 2008-2022 57 3006 29180 0.0909 353 6.53 1.7 &#177; 0.5 0.5</p><p>An effective energy threshold of &#8764;200 GeV is calculated. The spectrum is fit between 200 GeV and 2 TeV where the photon count in each bin is above 10 excess counts and the significance is above 1&#120590;, since this source is weakly detected. Upper limit points were calculated to a confidence limit of 99%. The spectrum is fit with a power law, where upper limits are not included. The power law fit gives (2.39 &#215; 10 -12 &#177; 5.2 &#215; 10 -13 ) &#215; (&#119864;/400 GeV) (-2.7&#177;0.5) TeV -1 cm -1 s -1 .</p><p>VHE photons are absorbed by the extragalactic background light (EBL) throughout the universe; the flux must be corrected to account for this effect. This absorption is energy and redshift dependent. Deabsorption is applied to the flux using the model of <ref type="bibr">[19]</ref>. After deabsorbing the spectrum from the EBL, the power law fit is (7.49 &#215; 10 -12 &#177; 1.7 &#215; 10 -12 ) &#215; (&#119864;/400 GeV) (-1.1&#177;0.6) TeV -1 cm -1 s -1 . Although these flux points are harder than the overlapping Fermi-LAT data, they are consistent within error. Both observed and EBL deabsorbed spectral points are shown in Figure <ref type="figure">1</ref>.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>PoS(ICRC2023)659</head><p>VERITAS Detection of RBS 1366  Parameter Value Uncertainty Unit Index 1.62 0.05 Amplitude 9.0 1.4 10 -12 cm -2 s -1 TeV -1 Reference 0.4 -TeV</p><note type="other">Deivid Ribeiro</note><p>The combined HE and VHE spectral fit is shown in Figure <ref type="figure">3</ref>. Although the VERITAS flux point are hardened by the lowest energy point at 200 GeV, the combined power law fit is consistent within error with a &#120594; 2 statistic of 13.49 (ndof=12). These fit results are summarized in Table <ref type="table">2</ref>.</p><p>In addition to the VERITAS SED, a light curve was also computed over 30 day bins, integrating above 300 GeV. This is shown in Figure <ref type="figure">2</ref> along with the corresponding Fermi-LAT light curve.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="4.">Discussion &amp; Conclusion</head><p>The source exhibited a hard HE+VHE spectrum (index &lt; 2) after correcting for EBL absorption. With a synchrotron peak at log frequency of 17.7 &#177; 0.2 (&#8764;2 keV), a redshift of 0.237, and the known hardness of the Fermi-LAT power law, the evidence already points toward an EHSP classification. The combined HE+VHE fit in this work supports this classification and merits investigation into the subclassification posited by <ref type="bibr">[5]</ref>. The power law index 1.62 &#177; 0.05 on the combined EBLdeabsorbed HE+VHE spectrum in Figure <ref type="figure">3</ref> gives a VHE gamma-ray slope (&#119878; = 2 -&#120574; where &#120574; is power law index) of &#119878; = 0.38, which places RBS 1366 similar to other blazars such as 1ES</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>PoS(ICRC2023)659</head><p>VERITAS Detection of RBS 1366 1101-232, 1ES 0347-121 and 3FGL J0710+5808, which were labeled as Hard-TeV EHBLs in <ref type="bibr">[5]</ref>]. A full multi-wavelength-SED will enable a complete classification in a future study.</p><note type="other">Deivid Ribeiro</note><p>The HE-VHE luminosity of RBS 1366 appears to peak above an energy of &#8764; 1 TeV, where it reaches an intrinsic luminosity of 3 &#215; 10 44 erg/s (assumed to be isotropic). However, since the turnover of the Compton component is not yet evident, we are not able to claim that the Compton component is not dominant over the synchrotron component, which peaks at a log frequency of 17.7 &#177; 0.2 (&#8764;2 keV) with a luminosity of &#8764; 10 45 erg/s <ref type="bibr">[5]</ref>. A more sensitive observation from the Cherenkov Telescope Array (CTA), a next generation IACT observatory, in the future may yield a more comprehensive estimation of the Compton peak with improved sensitivity above 1 TeV <ref type="bibr">[21,</ref><ref type="bibr">22]</ref>.</p><p>A basic estimate of the relativistic boosting in the SSC model fit to available published data is very high, between &#120575; &#8764; 50 -100, implying a significantly efficient acceleration that is common to EHSPs. This indicates the emission region is probably in the jet where the emission region is in the range of 10 17 cm and the magnetic field is very weak. While variability has been noted in the optical band <ref type="bibr">[8]</ref>, the lack of variability in the HE-VHE band is expected for the rising end of the Compton peak seen here.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head>PoS(ICRC2023)659</head><p>VERITAS Detection of RBS 1366 The observational circumstances above all support the conclusion that RBS 1366 is an EHSP now detected in the TeV energy range. Figure <ref type="figure">4</ref> is a reproduction of the index versus synchrotron peak frequency plot sampling the other TeV detection EHSPs in <ref type="bibr">[5]</ref>, which cluster into Hard-TeV and HBL-like blazars. Using the results presented in this work, RBS 1366 may be classified as a Hard-TeV EHSP. A complete study using a full multi-wavelength SED to confirm the Hard-TeV EHSP classification is underway.</p><note type="other">Deivid Ribeiro</note></div><note xmlns="http://www.tei-c.org/ns/1.0" place="foot" xml:id="foot_0"><p>1https://fermipy.readthedocs.io/en/latest/ ; v1.2</p></note>
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