The large gamma-ray flare of the flat-spectrum radio quasar PKS 0346−27

Aims. In this paper, we characterize the first γ-ray flaring episode of the flat-spectrum radio quasar PKS 0346−27 (z = 0.991), as revealed by Fermi-LAT monitoring data, and the concurrent multi-wavelength variability observed from radio through X-rays. Methods. We studied the longand short-term flux and spectral variability from PKS 0346−27 by producing γ-ray light curves with different time binning. We complement the Fermi-LAT data with multi-wavelength observations from the Atacama Large Millimeter Array (radio mm-band), the Rapid Eye Mount telescope (near-infrared) and Swift (optical-UV and X-rays). This quasi-simultaneous multi-wavelength coverage allowed us to construct time-resolved spectral energy distributions (SEDs) of PKS 0346−27 and compare the broadband spectral properties of the source between different activity states using a one-zone leptonic emission model. Results. PKS 0346−27 entered an elevated γ-ray activity state starting from the beginning of 2018. The high-state continued throughout the year, displaying the highest fluxes in May 2018. We find evidence of short-time scale variability down to approximately 1.5 h, which constrains the γ-ray emission region to be compact. The extended flaring period was characterized by a persistently harder spectrum with respect to the quiescent state, indicating changes in the broadband spectral properties of the source. This was confirmed by the multi-wavelength observations, which show a shift in the position of the two SED peaks by approximately two orders of magnitude in energy and peak flux value. As a result, the non-thermal jet emission completely outshines the thermal contribution from the dust torus and accretion disk during the high state. The broadband SED of PKS 0346−27 transitions from a typical LowSynchrotron-Peaked (LSP) to the Intermediate-Synchrotron-Peaked (ISP) class, a behavior previously observed in other flaring γ-ray sources. Our one-zone leptonic emission model of the high-state SEDs constrains the γ-ray emission region to have a lower magnetic field, larger radius, and higher maximum electron Lorentz factors with respect to the quiescent SED. Finally, we note that the bright and hard γ-ray spectrum observed during the peak of flaring activity in May 2018 implies that PKS 0346−27 could be a promising target for future ground-based Cherenkov observatories such as the Cherenkov Telescope Array (CTA). The CTA could detect such a flare in the low-energy tail of its energy range during a high state such as the one observed in May 2018.


Introduction
Radio-loud active galactic nuclei (AGN) are the most common astrophysical source class in the γ-ray sky. Their relativistic jets produced by the central black hole emit bright nonthermal radiation across a wide range of wavelengths and energies, from radio to TeV. The vast majority of γ-ray detected AGN are blazars, that is sources where the relativistic jet is aligned at a small angle with the observer's line of sight, leading to strong relativistic Doppler boosting and beaming effects. Blazars have historically been divided into two subclasses: flatspectrum radio quasars (FSRQs), showing strong broad emission lines in their optical spectra, and BL Lacertae objects (BL Lacs), which typically have weak or absent optical spectral features. There is also evidence that flat-spectrum radio-loud Tables of the measured fluxes are only available at the CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/627/ A140 narrow-line Seyfert 1 (NLS1) galaxies host low-power blazartype jets aligned with our line of sight (Berton et al. 2018). The broadband spectral energy distributions (SED) of blazars show a typical double-peaked structure. The low-energy peak is produced by synchrotron emission from the relativistic electrons in the jet. The emission processes giving rise to the highenergy emission peak are somewhat less clear. The simplest models invoke inverse Compton (IC) emission from the same electrons producing the low-energy synchrotron emission (the so called leptonic emission models), while more advanced models involve relativistic protons as well (lepto-hadronic emission models, see, for example, Böttcher et al. 2013). Abdo et al. (2010a) introduced an alternative classification scheme for blazars based on the peak frequency of the synchrotron component ν (HSP). FSRQs and blazar-like NLS1s are typically LSP, while the peak synchrotron frequency in BL Lacs can range across the three classes (Abdo et al. 2010a). While this is true when considering archival multi-wavelength data, some sources have shown extreme changes in their broadband spectral properties during flaring states. This implies that their place in classification schemes such as the ones mentioned above should be considered as time-dependent. Exemplary cases of time-dependent blazar classification are PKS 2155−304 (Foschini et al. 2008), PKS 1510−089 (D'Ammando et al. 2011), PMN J2345−1555 (Ghisellini et al. 2013), 4C +49.22 (Cutini et al. 2014) and PKS 1441+25 (Ahnen et al. 2015).
PKS 0346−27 (also known as BZQ J0348−2749, Massaro et al. 2009), with coordinates RA = 57.1589354 • and Dec = −27.8204344 • (J2000, Beasley et al. 2002) is a blazar source located at a redshift z = 0.991 (White et al. 1988). It was first identified as a radio source in the Parkes catalog (Bolton et al. 1964); additionally, White et al. (1988) classified it as a quasar based on its optical spectrum. It was later revealed as an X-ray source by ROSAT (Voges et al. 1999, and references therein). In the γ-ray band, it was not detected by the Energetic Gamma Ray Experiment Telescope (EGRET, Thompson et al. 1993), but it was detected by Fermi-LAT and included in the Fermi-LAT First Source Catalog (1FGL, Abdo et al. 2010b). In the latest catalog, the Fermi-LAT Fourth Source Catalog (4FGL, The Fermi-LAT Collaboration 2019) it is associated with the γ-ray source 4FGL J0348.5−2749. No elevated state of γ-ray activity from this source has been reported and studied in detail so far.
A near infrared (NIR) flare from PKS 0346−27 was first reported based on data taken on 2017 Nov. 14 (MJD 58071, Carrasco et al. 2017). A few months later, strong γ-ray flaring activity was reported on 2018 Feb. 02 (MJD 58151) based on Fermi-LAT data (Angioni 2018). The source was found in an elevated state, reaching a daily γ-ray (>100 MeV) flux more than 100 times larger than the average flux reported in the 3FGL, and a significantly harder spectrum with respect to the one reported in the 3FGL. This prompted multi-wavelength follow-up observations which revealed enhanced activity in the optical-NIR (Nesci 2018a;Vallely et al. 2018), ultraviolet (UV) and X-ray (Nesci 2018b). The high-energy flare continued over the following months, showing a second, brighter peak on 2018 May 13 (MJD 58251, Ciprini 2018), with a daily flux ∼150 times the 3FGL catalog level.
In this paper, we characterize the flaring activity of PKS 0346−27, probing the temporal and spectral behavior in γ-rays. We investigate the changes in the broadband SED using quasi-simultaneous, multi-wavelength and archival data, and comparing the observations to theoretical models. In Sect. 2 we describe the data acquisition and analysis in the different bands. In Sect. 3 we discuss the variability observed with each instrument, with a focus on the object's γ-ray properties. In Sect. 4 we qualitatively describe the time-resolved quasi-simultaneous SEDs of PKS 0346−27, and in Sect. 5 we discuss a theoretical modeling of the SEDs. Throughout the paper we assume a cosmology with H 0 = 73 km s −1 Mpc −1 , Ω m = 0.27, Ω Λ = 0.73 (Komatsu et al. 2011).

Data set and analysis
In this section we present the data set and describe the data reduction process in the γ-ray band (Sect. 2.1), optical-UV and X-rays (Sect. 2.2), near infrared (Sect. 2.3) and radio-mm (Sect. 2.4).

Fermi-LAT
The Large Area Telescope (LAT) is a pair-conversion telescope, launched on 2008 June 11 as one of the two scientific instruments on board the Fermi Gamma-ray Space Telescope (Atwood et al. 2009). Its main energy range is 0.1−100 GeV, but its sensitivity extends down to 20 MeV and up to >1 TeV (Ajello et al. 2017). In the third LAT point source catalog, the 3FGL (Acero et al. 2015), PKS 0346−27 is associated to the γ-ray source 3FGL J0348.6−2748, with a 0.1−300 GeV flux of (9 ± 2) × 10 −9 photons cm −2 s −1 and a power-law spectrum with index 2.4 ± 0.1.
We have used the Python package Fermipy (Wood et al. 2017) to analyze the Fermi-LAT data. We used Pass8 event data (Atwood et al. 2013) and select photons of the SOURCE class, in a region of interest (ROI) of 10 • × 10 • square, centered at the position of the target source. We included in the ROI model all point sources listed in the 3FGL and located within 15 • from the ROI center, along with the Galactic (Acero et al. 2016) and isotropic diffuse emission (gll_iem_v06.fits and iso_P8R2_SOURCE_V6_v06.txt, respectively). We performed a binned analysis with 10 bins per decade in energy and 0.1 • binning in space, in the energy range 0.1−300 GeV, adopting the instrument response functions P8R2_SOURCE_V6. A correction for energy dispersion was included for all sources in the model except for the Galactic and isotropic diffuse components.
We first performed a maximum likelihood analysis over the full time range considered here, that is 2008 Aug. 04 15:43:36.000 UTC to 2018 Sep 01 00:00:00.000 UTC (MET 1 239557417 to 557452805). In the initial fit, we modeled the ROI sources adopting the spectral shapes and parameters reported in the 3FGL catalog. We fit as free parameters the normalization and spectral index of the target source, and the normalization of all sources within 5 • of the ROI center, in addition to the isotropic diffuse and Galactic components. Since our data set more than doubles the integration time with respect to the 3FGL catalog, we looked for potentially new sources, present in the ROI, with an iterative procedure. We produced a Test Statistic (TS) map. The TS is defined as 2 log(L/L 0 ) where L is the likelihood of the model with a point source at a given position, and L 0 is the likelihood without the source. A value of TS = 25 corresponds to a significance of 4.2σ, when accounting for two degrees of freedom (Mattox et al. 1996). A TS map was produced by including a test source at each map pixel and evaluating its significance over the current model. We looked for significant (TS > 25) peaks in the TS map, with a minimum separation of 0.3 • , and added a new point source to the model at the position of the most significant peak found, assuming a powerlaw spectrum. We then fit again the ROI, and produced a new TS map. This process was iterated until no more significant excesses were found 2 . We also performed a best-fit position localization for the target source and all new sources with TS > 25 found in the ROI.
In order to investigate the temporal variability of PKS 0346−27, we computed several light curves with different time binning (see Sect. 3.1). In each light curve, we performed a full likelihood fit in each time bin. The number of free parameters in the fit depends on the statistics in each bin. We first attempted a fit leaving the normalisation and index of 1 Mission Elapsed Time, that is seconds since 2001.0 UTC. 2 The source finding process resulted in the addition of four point sources to the 3FGL starting model. None of these are close or bright enough to the ROI center to significantly affect the results on the target source.
A140, page 2 of 11 the target source and the normalization of all sources in the inner 3 • of the ROI free to vary. If the fit did not converge or resulted in a non-detection (TS < 25), we progressively restricted the number of free parameters in the fit in an iterative fashion. First we reduced the radius including sources with free normalization to 1 • , then we left only the spectrum of the target source free to vary, and finally we fixed all parameters to their average values except for the target source's normalization. We consider the target source to be detected if TS > 9 in the corresponding bin, and the signal-to-noise ratio (that is, flux over its error, or F/∆F) in that bin is larger than two. If this is not the case, we reported a 95% confidence upper limit.

Swift-XRT/UVOT
PKS 0346−27 was observed with the Neil Gehrels Swift Observatory (Gehrels et al. 2004) as a Target of Opportunity (ToO), following the detection of the first γ-ray flare (Angioni 2018). The Swift data were analyzed using the tools available at the ASI Space Science Data Center (SSDC). The source has no nearby potential contaminants either in X-rays nor in optical, so it was possible to use the standard aperture photometry technique to evaluate the source parameters. Archival Swift-XRT observations of this source are available on 2009 Mar. 29 and 2009 May 18. Unfortunately, for both dates the exposure times were too low to perform a meaningful X-ray spectral fit. Spectral fits were possible during the high state in 2018, modeling the source emission with a single power law, the N H absorption frozen to the Galactic value (9.1 × 10 19 cm −2 , Kalberla et al. 2005), and a number of energy bins ranging between 4 and 12.
Swift-UVOT images in six bands were obtained for most of the pointings. Aperture photometry for all bands was obtained using the on-line tool available at the ASI SSDC, which provides magnitudes in the Vega system and fluxes in mJy. No reddening corrections were applied, which are on the order of a few hundredth magnitudes at most, and therefore comparable to the photometric errors. Given the source redshift (z = 0.991), the interstellar UV absorption band of the host galaxy at 2200 Å, if present, falls outside the UVOT range, and therefore does not affect these observations.

REM
The Rapid Eye Mount (REM) telescope is a 60 cm robotic instrument located at La Silla Observatory in Chile, and operated by the Istituto Nazionale di Astrofisica (INAF) 3 . Followup observations of PKS 0346−27 with REM started a few days after the first reported γ-ray flare in February 2018, using the ROSS2 camera for the r and i bands, and REMIR for the J and H bands. Time sampling was initially daily, then reduced to two days and weekly. Aperture photometry with IRAF (using apphot) was performed using nine nearby comparison stars from the 2MASS catalog with AAA quality flag, and twelve stars from the Fourth US Naval Observatory CCD Astrograph Catalog (UCAC4, Zacharias et al. 2013). The aperture diameter was set at twice the FWHM of the images, which was not the same in different nights. This is not critical because no nearby sources were present in any filter at our sensitivity level. Conversion from magnitudes to mJy for all REM bands was computed using the on-line tool from the Louisiana State University 4 . No Galactic reddening corrections were applied.

ALMA
PKS 0346−27 has been observed in the mm-band as a calibrator for the Atacama Large Millimeter Array (ALMA) since 2012. The flux density measurements in Bands 3 (84-116 GHz), 6 (211-275 GHz) and 7 (275-373 GHz) are publicly available as part of the ALMA calibrator catalog 5 .

Fermi-LAT
We show a weekly binned γ-ray light curve of PKS 0346−27 in Fig. 1. A pronounced peak is seen already in December 2017, lasting only one week. A more extended flaring period is seen between April and June 2018, with a peak 0.1−300 GeV flux of (1.28 ± 0.06) × 10 −6 photons cm −2 s −1 in the week centered on 2018 May 13. With a photon index of 1.88 ± 0.04, this translates to a luminosity of (9.6 ± 0.5) × 10 48 erg s −1 . Finally, a period of renewed activity is observed again in October 2018, but not at the same magnitude as the events in May 2018.
We investigated the presence of significant short-time scale variability in PKS 0346−27 during the brightest flaring period in May 2018. The 6 h, 3 h and orbit-binned light curves are shown in Fig. 2. The γ-ray flux of the source in this time period is high enough to yield significant detections in most bins, even on such short time scales. Fast variability appears evident at a visual inspection. To quantify its significance, we computed the so-called variability index (see Abdo et al. 2010b). The variability index is defined as where F wt is the weighted average and w i is the weight, which is computed as for bins with a significant detection and for bins where an upper limit is placed (F UL is the 95% confidence flux upper limit). The variability index follows a χ 2 distribution with N bin − 1 degrees of freedom. The results of the test are listed in Table 1. The variability appears to be the most significant (>10σ) on six hours and three hours time scales, but is still strongly significant on orbital scales. In order to provide a more quantitative estimate of the shortest significant variability time scale, we have computed the doubling or halving time using two-point flux changes, following Eq. (1) from Foschini et al. (2011). In this procedure, we only consider bins with significant detections where the flux difference between consecutive bins (with no upper limit in between) is larger than two times their 1σ uncertainty (that is, their error bar). In all three light curves, we find a shortest doubling or halving time scale consistent with the bin size. . The latter is only plotted for bins where it was possible to fit it as a free parameter (see Sect. 2.1). Filled blue points represent significant detections, downward grey arrows represent 95% confidence level upper limits. The detection threshold is set at TS > 9 and F/∆F > 2. For ease of representation, the length of the arrows has been set as equal to the average error for significantly detected bins. The dashed line in the bottom plot indicates the average photon index during the quiescent state (see Table 3). A zoom-in of this light curve to the period after 2017.5 (MJD 57936.5) is shown in Fig. 4.   separation in the distribution of photon index from this time period compared to the rest of the light curve. This is best visualized with the histogram in Fig. 3, showing the distribution of photon index. With respect to the average photon index excluding flaring periods (that is, "quiescent period" in Sect. 4), Γ index avg = 2.43 ± 0.07, we can see that most of the points with Γ index < Γ index avg are found during the hard state, while during the rest of the time the source spanned a much wider range of photon index, dominating the steeper end of the distribution. A two-sample Kolmogorov-Smirnov test yields a statistic of 0.38 and a p-value of 0.02. Therefore the hypothesis that the distributions of photon index in the two time intervals are drawn from the same parent distribution can be rejected at >95% confidence level.
Finally, given the hard spectrum observed during the flare, we investigated the production of high-energy photons with E > 10 GeV. Using the gtsrcprob tool, we calculated the probability of each photon of being associated to PKS 0346−27. In the third panel of Fig. 4, we show the arrival time and energy of the highest energy photons with probability higher than 80% of having been emitted by the target source. Interestingly, while most of the high-energy photons are clustered around the peak of activity in May 2018 (see Sect. 4), the highest energy photon, with E ∼ 100 GeV, was observed on 2018 Jan 20.

Swift-XRT/UVOT
The number of available Swift observations is not sufficient for a detailed characterization of variability and higher-level processing such as cross-correlation analysis with the γ-ray data. The optical-UV and X-ray data all show enhanced emission with respect to the quiescent values. The XRT and UVOT light curves are shown in Fig. 4. The resulting X-ray spectral parameters are listed in Table 2. It is interesting to note that during the peak of the γ-ray activity in May 2018, PKS 0346−27 was significantly more active in optical-UV than in X-rays. This reflects the shift in the position of the low-energy SED peak to higher frequencies in this period (see Sects. 4 and 5).

REM
The source flux varied coherently in the four bands (r, i, J, H), showing significant variability also on a daily scale. These variations are fairly well correlated with the γ-ray ones. A mild correlation (r = 0.67) between the (r-H) color index and the optical-NIR flux is present, hinting at a redder when fainter behavior, albeit with a large scatter. The average spectral slope in the range r-H covered by REM is −0.33 in the plane log(ν)-log(νFν).

ALMA
The γ-ray flaring activity in PKS 0346−27 was accompanied by an enhanced state in the radio band as well, as revealed by the mm-band data from ALMA, shown in Fig. 4. The flux density increased by a factor of three, rising from ∼0.5 Jy at the onset of activity up to ∼1.5 Jy at its peak. In this case as well, the sampling is not dense enough to perform a detailed analysis of correlated variability with other bands.

Time-resolved SEDs
We have constructed time-resolved SEDs of PKS 0346−27, by using contemporaneous data taken during the high-energy flaring state and archival data from different ground and space-based observatories. The time interval for each SED were chosen in order to probe different phases of activity, as traced by the γ-ray light curve. The multi-wavelength data for each time-resolved SED were selected based on the integration time used to produce the corresponding LAT spectrum. For example, if the LAT data for one SED were integrated over three months, all multiwavelength data taken during this time interval are considered to be contemporaneous and are used to build the time-resolved SED. The SEDs are shown individually in Fig. 5, and the γ-ray properties in each of the states are summarized in Table 3.
The different activity states are defined as follows. For the quiescent state, we consider data until 2016 Jan 01, as this is the date after which the source started to be significantly detected on weekly time scales (see top panel of Fig. 1). Since this was the first flaring episode observed in PKS 0346−27, the quiescent Fermi-LAT spectrum has been produced integrating from the mission start until 2016 Jan. 01 (MJD 54682.66 to 57388). Together with the archival multi-wavelength data from the ASI SSDC, this provides a well-sampled SED for the quiescent state of PKS 0346−27, which is shown in the upper left panel of Fig. 5. The data show a well-defined synchrotron peak at a frequency of ∼10 12 Hz. A thermal emission component is clearly visible, peaking in the optical-UV region, which corresponds to the so called Big Blue Bump. The γ-ray spectrum is relatively steep, and combined with the X-ray data it constrains the highenergy SED peak to ∼MeV energies.   (9) 15.85 ± 0.01 * We compare this quiescent-state SED with several others constructed using multi-wavelength data taken after the start of the flaring activity in PKS 0346−27. First, we defined a period of intermediate γ-ray activity between 2018 Jan. 01 and 2018 Apr. 01, which we indicate as "flare A" (MJD 58119 to 58209). During this time interval, the LAT spectrum is complemented by ALMA data in the mm-band and REM data in the NIR (see Fig. 4). The corresponding SED is shown in the upper-right panel of Fig. 5. Given the large scatter in the REM data due to variability, we have averaged the data and taken its standard deviation as error, in order to be consistent with the averaged γ-ray spectrum. A shift in the SED peak positions is already evident in this intermediate state: the synchrotron peak lies now in the region ∼10 13 −10 14 Hz. The combination of the peak shift and the change in normalization implies that the thermal component is now swamped by the non-thermal jet emission. The LAT spectrum is virtually flat, indicating a highenergy peak at GeV energies.
It is possible to construct an SED with data from the same day on 2018 Apr 20 (MJD 58228), probing a further higher activity period for PKS 0346−27, intermediate between the longterm flaring and the flare peak, occurring in May. The daily SED is shown in the center-left panel of Fig. 5. The synchrotron peak is constrained by the REM and UVOT data, while the XRT and Fermi-LAT data probe the high-energy peak. The synchrotron peak position is shifted further up to ∼10 14 Hz, and the simultaneous spectrum from NIR to UV is featureless, confirming that this region of the SED is completely dominated by nonthermal jet emission in this state. The most prominent change is the strong hardening of the γ-ray spectrum, suggesting a peak at ∼10 GeV.
Swift data allowed us to build an SED probing the week of highest flaring activity, on 2018 May 16 (MJD 58254), at a time when it was not possible to observe PKS 0346−27 with ground-based facilities. The resulting daily SED is shown in the center-right panel of Fig. 5. The highest normalization of the high-energy peak is not accompanied by the hardest spectrum (see Table 3), with a peak energy on the order of tens of GeV.
Interestingly, another daily SED taken on the following week, on 2018 May 20, (MJD 58258, see lower-left panel of Fig. 5), shows a synchrotron peak position which appears to have shifted further right, to ∼10 14.5 Hz. Because of this, the X-ray data shows a clear synchrotron contribution at low energies, which causes a break in the spectrum. To better quantify the significance of this spectral feature, we have fit the XRT spectrum from 2018 May 20 with a power-law (PL) and a broken power-law (BPL), using a simple χ 2 regression. We defined the functions following their definition in XSPEC (Arnaud 1996), that is: for the PL and BPL models, respectively, where K is the normalization at 1 keV, Γ indicates the power-law photon index and E b is the break energy. For the PL fit, we find K = (6.3 ± 0.5) × 10 −4 photons keV −1 cm −2 s −1 and Γ = 2.3 ± 0.2, with a reduced chi-squaredχ 2 = 1.687 and five degrees of freedom. For the BPL fit, we find K = (5.1 ± 0.7) × 10 −4 photons keV −1 cm −2 s −1 , Γ 1 = 3.2 ± 0.4, Γ 2 = 1.9 ± 0.3, E b = (1.1 ± 0.2) keV, with a reduced chi-squaredχ 2 = 0.126 and three degrees of freedom 6 . The XRT spectrum and the two models are shown in Fig. 6. An F-test to assess the significance of the BPL model with respect to the PL one yields F = 31.98 and a p-value p = 0.0306. The break is therefore significant at the 95% confidence level. Finally, we constructed a daily SED probing the period of renewed γ-ray activity in September-October 2018, namely on 2018 Oct. 18 (MJD 58409, see lower-right panel of Fig. 5). While the normalization of the high-energy peak is comparable to the levels observed in May 2018, the spectrum is significantly softer (see Table 3). Together with the hard X-ray spectrum, this indicates a peak in the ∼100 MeV range.

SED modeling
The quiescent and flaring states defined in Sect. 4 were modeled with the one-zone leptonic model described by Finke et al. (2008) and Dermer et al. (2009). A brief description is given here. The model assumes emission from an isotropic and homogeneous single spherical emitting region ("blob") moving at speed βc at small angle to the line of sight θ giving it a bulk Lorentz factor Γ = (1 − β 2 ) −1/2 and Doppler factor δ D = [Γ(1 − β cos θ)] −1 . We assume Γ = δ D . The blob has radius R b in the frame comoving with the blob and is filled with a tangled magnetic field of strength B. The model includes emission components from synchrotron, synchrotron self-Compton (SSC), and external Compton (EC) scattering of some external radiation field. The external radiation field is assumed to be monochromatic, isotropic and homogeneous in the stationary frame, which is a reasonable approximation for scattering of a broad line region or dust torus (see for instance, Dermer et al. 2009;Finke 2016). We chose the external radiation field parameters to be similar to what one would expect for a dust torus.
Based on the dust model of Nenkova et al. (2008), this implies the external radiation field has an energy density u dust = 2.4 × 10 −5 ξ dust 0.1 T dust 10 3 K 5.2 erg cm −3 .
Most blazars do not show significant signs of absorption in their γ-ray spectra from BLR photons (see for example, Costamante et al. 2018;Meyer et al. 2019). PKS 0346−27 does not show emission above 10 GeV, and thus it is not clear if these absorption features are present in its spectra. Nevertheless, we A140, page 8 of 11 do not think models involving scattering of BLR photons are well-motivated any longer unless the SED of a blazar cannot be explained by other models. Emission components from a Shakura-Sunyaev accretion disk (Shakura & Sunyaev 1973) and a blackbody dust torus were also included. The electron distribution in the emitting region was assumed to be a broken power-law where γ is the electron Lorentz factor in the comoving frame. The short-time scale light curves (Fig. 2), show significant variability down to t v ≈ 6 h (see Table 1). This constrains the size of the emitting region R b t v δ D c/(1 + z). All our size scales in the modeling are consistent with this.
Our modeling results can be seen in Fig. 5 and the model parameters can be found in Table 4. Based on the Mg II line measured from the optical spectrum of Baker et al. (1999) and the virial relations from Shen et al. (2011), we estimate the black hole mass of PKS 0346−27 to be M BH ∼ 2 × 10 8 M .
The small implied size scale R b indicates that significant synchrotron self-absorption occurs at radio frequencies, so that the radio emission must be from a larger portion of the jet (see for instance, Blandford & Königl 1979;Finke 2019). The absorption of γ-rays by the extragalactic background light was included based on the model of Finke et al. (2010).
For the low state SED, we used a black hole mass consistent with the optical spectrum of Baker et al. (1999). The disk (modeled as a Shakura-Sunyaev disk, Shakura & Sunyaev 1973) and synchrotron emission were modeled so that their combined emission is in between the Baker et al. (1999) spectrum and the UVOT data, while reproducing the WISE data. We note that Baker et al. (1999) estimate a 20−50% error on their spectrophotometric calibration. The UVOT data were likely taken when the source was in a higher state. The WISE and LAT quiescent state spectra give similar spectral indices, indicating that they are generated from the same electron population. The disk parameters are not well-constrained by the SED, but we use an inner disk radius of 6R g , which may not be consistent with a black hole with high spin.
For the Apr. 20, May 16, and May 20 flares, the X-ray spectra cannot connect smoothly with the LAT γ-ray spectra. This indicates that the X-rays are likely produced by SSC, and the soft excess in the May 20 X-ray spectrum indicates a contribution from the tail of the synchrotron component. The hard X-ray spectrum in the Oct. 18 flare indicates it is produced by the EC mechanism. The lack of X-ray data during the flare A period implies that R b and other parameters are not well-constrained for this time period. The constraints (EC from a dust torus, compact emitting region, X-rays dominated by SSC during some flares) indicate that a large Γ is required to describe the SED, that is Γ = 60. Such a large value is consistent with the apparent speed of jet components seen with radio Very Long Baseline Interferometry (VLBI), which can be as high as β app = 78 (Jorstad et al. 2017). In previous modeling efforts, it was found that varying only the electron distribution was necessary to reproduce several states from FSRQs (see for example, D'Ammando et al. 2013;Ackermann et al. 2014;Buson et al. 2014) although this is not always the case (see for instance, Dutka et al. 2013Dutka et al. , 2017. For the SEDs of PKS 0346−27, we attempted to model all states varying only the electron distribution. These efforts failed. We then varied the size of the emitting region and the magnetic field to model the states. Therefore, based on the classification of Dutka et al. (2013Dutka et al. ( , 2017, all of the modeled flares from PKS 0346−27 are type 2 flares 7 . The highest jet power is reached on 2018 May 16 and 2018 Oct. 18, with P j,tot = P j,e + P j,B = 5.0 × 10 45 erg s −1 . The accretion power is P acc = L disk /η = 1.3 × 10 47 erg s −1 and the ratio P j,tot /P acc = 0.04. The quiescent state and all flares except the flare A state have the jet power dominated by electrons; however, as mentioned earlier, the model for the latter state is poorly constrained due to the lack of X-ray observations at this time. The general relativistic magnetohydrodynamic simulations by Tchekhovskoy et al. (2011) indicate that the ratio P j,tot /P acc can be as large as 1.4 if the jet is extracting power from the spin of the black hole. The values of the total jet power calculated here can be considered lower limits, since we do not include the uncertain power carried by protons in the jet.
We computed the radiative cooling time scale in the observer frame at 1 GeV from the model parameters (Finke 2016), and we list the results in Table 4. The cooling time scale should be less than the variability time scale, which is indeed the case. R in 6.0 6.0 6.0 6.0 6.0 6.0 Seed photon source energy density [erg cm −3 ] u seed 3.7 × 10 −4 3.7 × 10 −4 3.7 × 10 −4 3.7 × 10 −4 3.7 × 10 −4 3.7 × 10 −4 Dust Torus luminosity [erg s −1 ] L dust 7.0 × 10 43 7.0 × 10 43 7.0 × 10 43 7.0 × 10 43 7.0 × 10 43 7.0 × 10 43 Dust Torus radius [cm] R dust 6.9 × 10 17 6.9 × 10 17 6.9 × 10 17 6.9 × 10 17 6.9 × 10 17 6.9 × 10 17 Dust temperature [K] T t cool 8.0 × 10 2 8.6 × 10 2 5.0 × 10 2 1.0 × 10 3 9.6 × 10 2 1.0 × 10 2 During all the flaring states, the peaks of both the synchrotron and Compton components of the SED shift to higher frequencies. This is similar to the flares detected by the FSRQ PKS 1441+25 (Abeysekara et al. 2015;Ahnen et al. 2015), although in that case the shift was even more extreme. For PKS 1441+25 the synchrotron peak was as high as ≈10 15 Hz, while for the flares from PKS 0346−27 reported here the peak reaches a frequency of 10 14.5 Hz. The source PKS 1441+25 was detected by MAGIC and VERITAS. This fact, together with the hard LAT spectra from PKS 0346−27 during the Apr. 20, May 16, and May 20 flares suggests that it might have been detectable by current imaging atmospheric Cherenkov telescopes such as H.E.S.S. (the only one able to access the relevant declination range). However, our modeling shows that the steeply falling high-energy peak would make a TeV detection challenging. To test whether PKS 0346−27 would be a good target for the upcoming CTA (The Cherenkov Telescope Array Consortium 2017), we plot the latest CTA sensitivity curves for CTA south 8 in Fig. 5. It can be seen that a detection might be possible for states such as 2018 May 16 and 2018 May 20 in the low-energy tail of the CTA energy range, that is few tens of GeV.

Summary and conclusions
In this paper we reported on the γ-ray flaring activity from the FSRQ PKS 0346−27, and the associated multi-wavelength follow-up observations. The available data set, including mmband radio, NIR, optical, UV, X-ray and γ-ray data, allowed us to investigate variations in the broadband SED of the source, and to probe its physical jet parameters through theoretical modeling of the SED in different activity states.
PKS 0346−27 entered an elevated activity state between the end of 2017 and the beginning of 2018, with the flaring activity continuing over the whole year. We investigated the presence of fast variability during the brightest phase of flaring activity, 8 From https://www.cta-observatory.org/ and found significant variability down to time scales of hours, constraining the emission region to be very compact. Throughout 2018, the source showed a consistently harder spectrum with respect to the quiescent state, suggesting a drastic change in its broadband spectral properties.
We investigated this by modeling the SED of the source in its quiescent state and comparing it to the one observed during several different stages of activity. The resulting time-resolved SEDs confirm that the multi-wavelength flare coincided with strong broadband spectral variability, with the two SED peaks shifting up by ∼2 orders of magnitude in energy during the peak of activity. While a clear thermal signature from the accretion disk is visible in the low-energy peak of the quiescent SED, during the flare this component is completely washed out by the non-thermal jet emission. According to our one-zone leptonic modeling, the high-state SEDs require a lower magnetic field, larger emission region size, and higher electron Lorentz factors.
The time-resolved SEDs of PKS 0346−27 show another example of a blazar with variable spectral classification. According to Abdo et al. (2010c), PKS 0346−27 in its quiescent state would be classified as Low-Synchrotron-Peaked (LSP) blazar, as its low-energy SED peak is located at ν syn peak < 10 14 Hz. However, the shift in the synchrotron peak position during the flaring state puts it in the range of Intermediate-Synchrotron-Peaked (ISP) objects. Such a behavior has been observed before in the case of the LSP blazar PKS 1441+25, which showed an HSP-like SED during the elevated state which led to its TeV detection (Ahnen et al. 2015). Another example of a similar time-dependent SED classification is the FSRQ 4C +49.22 (Cutini et al. 2014). Similarly to what we observe for PKS 0346−27, 4C +49.22 showed a two orders of magnitude shift in its synchrotron peak position during a multi-wavelength flaring episode in 2011, transitioning from LSP to ISP. Moreover, the fact that the non-thermal emission is dominant in the optical band during the flare suggests that PKS 0346−27 could possibly appear as a "masquerading BL Lac" in its high state, that is, a blazar with intrinsically strong broad optical lines which are diluted by the non-thermal continuum, to an A140, page 10 of 11 extent that would lead to its classification as a BL Lac based on its optical spectrum (Giommi et al. 2012(Giommi et al. , 2013. The hard γ-ray spectrum suggests that PKS 0346−27 could have been observed by Cherenkov telescopes in the TeV regime; however, the SED modeling shows a steep cutoff in the highenergy peak after ∼10 GeV. By comparing the model with current sensitivity curves from the upcoming CTA, we conclude that such a flare from PKS 0346−27 might have been visible in the low-energy tail of the CTA energy range. Incidentally, if PKS 0346−27 was detected in the TeV range, it would be the highest redshift VHE source (z = 0.991), surpassing the gravitationally lensed blazar S3 0218+35 (z = 0.944, Ahnen et al. 2016) as well as PKS 1441+25 (z = 0.940, Ahnen et al. 2015). Because of this, detecting PKS 0346−27 at VHE would also be relevant for EBL studies.
Continued monitoring of the GeV sky by the Fermi-LAT is crucial in order to observe more flaring events from high-redshift (z 1) blazars and establish the duty cycles of γ-ray activity in relativistic jets. Moreover, the Fermi-LAT is an invaluable tool in order to trigger pointed observations by ground-based γ-ray observatories such as Cherenkov telescopes, including the upcoming CTA. Therefore, continued operations of the Fermi-LAT into the CTA era would be instrumental in order to gain insight into the physics of blazar jets, both in the local universe and at cosmological distances.