DISCOVERY OF VERY HIGH ENERGY γ-RAY EMISSION FROM THE SNR G54.1+0.3

In recent years, new insights into the most extreme environments in the Galaxy have been obtained through the very high energy (VHE, >100 GeV) gamma-ray band (Aharonian et al. 2005a). The majority of the >50 Galactic TeV sources found thus far are associated with supernova remnants (SNRs) or pulsar wind nebulae (PWNe).³⁰ The detection of these stellar remnants in VHE gamma rays constitutes a probe of non-thermal astrophysical processes. The acceleration of electrons or nuclei, above 1 TeV, in these sources leads to the generation of gamma rays. Relativistic electrons can produce gamma rays by non-thermal bremsstrahlung, and by inverse Compton (IC) scattering on ambient microwave, IR, or optical photons, whereas protons and atomic nuclei can generate gamma rays via the decay of neutral pions produced in hadronic interactions with ambient material. A confirmation of the latter process associated with the gamma rays from SNRs is seen as a probe of nucleonic cosmic-ray production sites in the Galaxy.

The SNR G54.1+0.3 has been predicted to emit gamma rays detectable with the current generation of TeV instruments after the discovery of a rotation-powered pulsar in its center, a source of high energy electrons (e.g., Bednarek & Bartosik 2005). This pulsar, PSR J1930+1852 (P = 136 ms), with a derived spin-down power of  = 1.2 ×10³⁷ erg s⁻¹ and a spin-down age of τ_c ∼ 2900 years (Camilo et al. 2002), is among the youngest and most energetic pulsars known. The PWN powered by this pulsar was first recognized as such from high-resolution radio observations (Reich et al. 1985). The PWN exhibits a filled-center morphology (2' × 15), a flat radio spectrum (α ≈ 0.13) that is fairly constant over the entire source extent, and a high level of polarization (Velusamy & Becker 1988). The discovery of an X-ray jet, consistent with the radio extension, and the measurement of its non-thermal spectrum confirmed the PWN nature of G54.1+0.3 (Lu et al. 2001). More detailed X-ray observations by Lu et al. (2002) resolved the inner structure of the nebula as a central pointlike source with a surrounding ring and bipolar elongations, comparable to the Crab Nebula. The same authors suggested a distance of ∼5 kpc, based on the X-ray absorption. The most recent estimate is 6.2^+1.0_−0.6 kpc, based on an apparent morphological association between the PWN and a nearby molecular CO cloud (Leahy et al. 2008).

Similar to the Crab Nebula, G54.1+0.3 lacks a strong surrounding circumstellar interaction between the SNR forward shock and the progenitor star wind (Chevalier 2005), in which particles could be accelerated and produce an additional non-thermal emission contribution. Recently, Leahy et al. (2008) found a shell of 30' diameter surrounding G54.1+0.3, but the authors concluded that these are unlikely to be associated based on the different measured distances. After that, Koo et al. (2008) identified a partial shell-like infrared structure surrounding much of the X-ray/radio core in G54.1+0.3, which they proposed to be a star-forming region triggered by late-phase winds from the SNR progenitor star. Based on high-resolution IR spectra, however, Tenim et al. (2010) suggested that the shell is composed of freshly formed ejecta dust that appears to be heated by the expanding PWN.

G54.1+0.3 has not been previously detected at γ-ray energies. The source lies 14 from the EGRET source 3EG J1928+1733 (Hartman et al. 1999). This is slightly outside the 99% confidence-level error box. The older (τ_c ∼ 8.2 × 10⁴ years) and less-energetic ( ergs s⁻¹) pulsar PSR J1928+1746 is proposed as a more likely counterpart to the unidentified 3EG source (Cordes et al. 2006). This is strengthened with the much better localization of the gamma-ray source 1FGL J1929.0+1741c, associated with 3EG J1928+1733 in the first Fermi catalog (Abdo et al. 2010). This other pulsar is 12 away from PSR J1930+1852. In the VHE γ-ray domain, the only published observation is an upper limit from the HEGRA collaboration at 20% of the Crab Nebula flux above 600 GeV (Aharonian et al. 2002). In this Letter, we report the discovery by VERITAS of VHE gamma-ray emission from the direction of the very young system G54.1+0.3/PSR J1930+1852. The instrument and observations are described in Section 2, while the analysis performed on these data is detailed in Section 3. Results are presented in Section 4, and interpretation and conclusion in Section 5.

VERITAS is an array of four imaging atmospheric Cherenkov telescopes located at the Fred Lawrence Whipple Observatory in southern Arizona, USA (Holder et al. 2006, 2008). Each telescope has a mirror area of 110 m² and is equipped with a 499 pixel camera of 35 diameter field of view. The system, completed in the fall of 2007, is run in a coincident mode requiring at least two of the four telescopes to trigger in each event. This design allows for the observations of astrophysical objects in the energy range from 100 GeV to above 30 TeV. VERITAS has an angular resolution (68% containment) of 01 diameter per event and a 5σ point-source sensitivity of 1% of the steady Crab Nebula flux above 300 GeV in less than 50 hr of observation at a 20° zenith angle.

The first pointed observations of the G54.1+0.3/PSR J1930+1852 system with VERITAS took place during a survey of northern hemisphere Galactic pulsars between 2007 September and 2008 October. The live time of this first data set, after data-quality selection based on weather and hardware status, amounts to 14.5 hr (some of which was taken in partial moonlight). Analysis of these data revealed evidence of a VHE γ-ray signal at the position of PSR J1930+1852 at the 4σ level after accounting for all analysis trials. This evidence triggered further observations between 2009 April and 2009 June, resulting in 22.2 additional hours after quality selection. Of these, the most recent 15.2 hr of data were taken using only three telescopes, as telescope T1 was in the process of being relocated to optimize the instrument sensitivity (Perkins et al. 2010). The zenith angle range of observation of the combined data sets is 13°–35°, and the total live time is 36.6 hr.

After calibration, the standard VERITAS event reconstruction scheme is applied to the data: tail-cuts image-cleaning, second-moment parameterization of these images (Hillas 1985), and stereoscopic direction determination based on the intersection of image axes (see, e.g., Krawczynski et al. 2006 for details). An initial selection of the events is performed to reject those in which the primary parameters, energy and direction, cannot be well-reconstructed. The events surviving this quality selection are those for which at least two telescope images have more than 4 pixels included in the image with a total integrated charge in each image of more than 80 photoelectrons, and with less than 20% of the total charge in the outermost ring of camera pixels. This selection removes images with insufficient Cherenkov light for accurate parameterization, or which are truncated by the camera boundary. In addition, events for which only the telescopes T1 and T4 have surviving images are excluded, as their separation of only 35 m introduces an irreducible high background rate, due to local muons, degrading the instrument sensitivity (Maier & Knapp 2007).

A further selection of events is performed to suppress the otherwise overwhelming hadronic cosmic-ray background. This is achieved by comparing the shapes of the event images in each telescope with the expected shapes of simulated gamma-ray showers. These mean-reduced-scaled width (MRSW) and mean-reduced-scaled length (MRSL) cuts (see definition in Krawczynski et al. 2006), as well as an additional cut on the arrival direction of the incoming gamma ray with respect to the source position (θ²), reject more than 99.9% of the hadronic cosmic-ray background while keeping 45% of the gamma rays. Different sets of these cuts, optimized for different source properties, are applied to the G54.1+0.3 data. Two a priori test positions are defined as the locations of the high spin-down power pulsars: J1930+1852 (19^h30^m3013, + 18°52'141) and J1928+1746 (19^h28^m4248, + 17°46'27''). In the search for a VHE γ-ray signal from a point source with a Crab-like spectrum, the following cuts were employed: −1.2 < MSCW/L < 0.5 and θ² < 0.015 deg², resulting in an analysis threshold of 250 GeV. Since the emission region may be extended, as is the case of most of the galactic PWN detected at VHE γ-rays (Aharonian et al. 2005a), a larger cut in the arrival direction θ² < 0.055 deg² is also considered. In addition, a rather tight cut on the integrated charge of ∼225 photoelectrons is applied, to maximize the signal-to-noise ratio for a weak source with a hard spectrum. The latter cut results in an analysis threshold of 500 GeV and in superior angular resolution. For the spectral analysis, this cut is 80 photoelectrons providing maximal coverage in energy.

For the background estimation, we employ two different methods, as described in Berge et al. (2007). The background estimate for each position in the two-dimensional sky map is taken from a ring of mean radius 05 and an area six times that of the on-source region. For the spectral analysis, the background is taken from seven positions in the field of view with the same offset from the pointing direction as the source regions. This eliminates the need for corrections concerning the radial dependence of the background acceptance. The on-source and background region counts, together with a normalization factor for the different acceptance of these regions, are used to derive the statistical significance of any excess following the likelihood method of Li & Ma (1983).

Figure 1 shows a sky map of the excess counts for the entire data set in the region around G54.1+0.3/PSR J1930+1852 system, derived using the point-source analysis described above. A source of VHE gamma rays is clearly visible and is coincident with the position of the X-ray and radio PWN. An excess of 101 events is observed, corresponding to a pre-trials statistical significance of 7.0σ at the location of PSR J1930+1852, as shown in Table 1. This significance is the highest obtained at the pulsar position for the four different search criteria attempted, and this is taken into account in assessing the true chance probability of the observed signal of 6.8σ. As discussed above, the earlier data set showed evidence for a VHE γ-ray signal at 4.3σ. This evidence is confirmed by the presence of a 5.5σ detection at the same position in 2009 data set alone. This increase is as expected for a steady source with increased exposure time and a slightly reduced sensitivity of the array with only three telescopes.

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The unsmoothed map of excess events, binned in 005 × 005, is fit by a two-dimensional Gaussian in order to study the morphology of the observed emission. The gamma-ray excess is well fit by the point-spread function of the instrument at the corresponding analysis threshold of 500 GeV (∼011), which results in a detection compatible with a pointlike source for VERITAS. The best fit of the Gaussian centroid is 19^h30^m32^s ± 25^s, + 18°52'12'' ± 20'' (J2000) and hence we assign the name VER J1930+188. Given the systematic uncertainty of 002 in this measurement, the centroid is consistent with the pulsar position (at a distance of 0007) and the 003 extent of the PWN G54.1+0.3 around the pulsar.

The total γ-ray excess above 250 GeV, i.e., that within a circle of 015 around the pulsar position, is 214 ± 43 events. Figure 2 shows the reconstructed gamma-ray spectrum from these events. The data are consistent with a power law in energy that extends from 250 GeV up to 4 TeV with a photon index of Γ = 2.39 ± 0.23_stat ± 0.30_sys and a differential flux at 1 TeV of (7.5 ± 1.2_stat ± 1.5_sys) × 10⁻¹³ TeV⁻¹ cm⁻² s⁻¹. The corresponding flux above 1 TeV is 2.5% of the Crab Nebula flux.

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No other significant TeV source is found in the maps, including at the second a priori test position, the location of PSR J1928+1746, for any of the searches performed. The significance at this pulsar position is 1.2σ and the flux upper limit above 1 TeV at the 99% confidence level (Feldman & Cousins 1998), assuming a power-law source spectrum with Γ = 2.5, is F < 2.6 × 10⁻¹³ cm⁻² s⁻¹ (about 1.4% of the flux of the Crab Nebula; see Table 1). We have used the point-source analysis for these calculations, as there is no known X-ray or radio PWN or SNR counterpart associated with this pulsar which can be used to constrain the size of the TeV emission.

VERITAS has detected VHE gamma-ray emission from the direction of the SNR G54.1+0.3, providing a new input to study the non-thermal particle population in this object. This new TeV source, VER J1930+188, appears pointlike within the instrument resolution and does not show a notable offset from the pulsar PSR J1930+1852, placing it among the more compact TeV sources found to be associated with an SNR. The emission is co-located with the X-ray and radio PWN in the SNR G54.1+0.3, and also with a molecular CO cloud in apparent morphological association with the PWN and a partial shell of IR ejecta around the PWN.

Assuming the gamma-ray production in VER J1930+188 is related to the pulsar, the compactness of the TeV source and lack of significant offset between the pulsar and its X-ray PWN and the TeV source can be attributed to its relative youth. The spin-down age of PSR J1930+1852 is 2900 years, which places it as the latest addition to an emergent class of TeV sources associated with very young pulsars: PSR B0531+21/Crab Nebula (Weekes et al. 1989), PSR J1747−2809/HESS J1747−281 in G0.9+0.1 (Camilo et al. 2009; Aharonian et al. 2005b), PSR J1845−0258/HESS J1845−029 in SNR Kes 75, PSR J1833−1036/HESS J1833−105 in G21.5−0.9 (Djannati-Atai et al. 2008), and PSR J1813−1749/HESS J1813−178 in G12.82−0.02 (Gotthelf & Halpern 2009). Those PWNe are good candidates for being in the early stage of evolution, where the wind nebula is interacting with the freely expanding supernova ejecta. This population stands in contrast to an apparently more common variety of energetic-pulsar-associated TeV sources, a group which contains, as notable examples, PSR B1823−1313/HESS J1825−137 (Aharonian et al. 2006a), PSR B0833−45/Vela X (Aharonian et al. 2006b), and PSR J2229+6114/VER J2227+608 (Acciari et al. 2009). These objects show extended TeV emission which is both larger than the X-ray PWN and offset from the pulsar location (see, e.g., de Jager & Djannati-Atai 2009). A common element in this class is older, middle-aged pulsars, with ages >10⁴ yr. Here, the PWN may be displaced in some direction, possibly by an asymmetric SNR reverse shock generated from an explosion into an inhomogeneous medium (Blondin et al. 2001).

Table 2 lists the pulsar properties (spin-down power, age, and distance) and the nebular energetics in several compact PWNe detected in TeV. The total power, L_g, radiated by G54.1+0.3 in the energy band 0.2–10 TeV is 2.1 × 10³⁴ erg s⁻¹ compared to 8.6  ×  10³⁴ erg s⁻¹ for the Crab Nebula. This value of the gamma-ray luminosity of G54.1+0.3 is the same order of magnitude what has been found for the other PWNe in the table. A more relevant quantity to compare is the efficiency of TeV luminosity production compared to the pulsar power which is η_γ∼ 0.17% for G54.1+0.3. This is similar to that of G0.9+0.1 (≈0.1%) and 10 times larger than other young systems like the Crab Nebula (≈0.02%) and HESS G21.5−0.9 (≈0.02%). However, all these PWNe have significantly lower levels (ranging from 0.1% to 2.9%) of X-ray luminosity production efficiency than the Crab Nebula (≈4%). Despite being worst synchrotron emitters than the Crab Nebula, G54.1+0.3, together with the other recent compact TeV PWNe, are similar and even better TeV emitters than the Crab Nebula.

Table 2. Pulsar and Nebular Properties of Compact PWN Detected at TeV

Name		τc	Distance	Lγa	LXb	ηγc	ηXd	LX/Lγ
	(1036 erg s−1)	(kyr)	(kpc)	(1034 erg s−1)	(1034 erg s−1)	(%)	(%)
Crab Nebula	460	1.2	2	8.6	1900	0.02	4	220
G0.9+0.1	43	5.3	8.5	4.4	36	0.1	0.8	8
G21.5−0.9	33	4.85	4.7	0.72	22	0.02	0.7	30
G54.1+0.3	12	2.9	6.2	2.1	2.9	0.17	0.2	1.4
Kes75	8.1	0.7	7.5	2.5	24	0.3	2.9	10

Notes. ^aLuminosity in the 0.2–10 TeV band. ^bLuminosity of the PWN in the 0.5–8 keV band, taken from Kargalstev & Pavlov (2008). ^cEfficiency to convert the spin-down energy to VHE gamma-ray emission: η_γ ≡ L_γ/. ^dEfficiency to convert the spin-down energy to X-ray synchrotron: η_X ≡ L_X/.

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Another diagnostic is the strength of the synchrotron emission relative to the gamma-ray emission, L_X/L_γ. The Crab Nebula has the largest ratio among all young systems by far with L_X/L_γ of 220. That of G54.1+0.3 is the lowest among the others that range between 1.4 and 30. These numbers are consistent with Mattana et al. (2009) who finds L_γ > L_X after 5 kyr from pulsar birth, including a different list of objects and spanning over a larger range of τ_c. The scattering of this ratio in two orders of magnitude, may be attributed to the unique environments in each of these objects, such as the local ambient photon fields or the interactions with the surrounding mediums resulting in an increase of the nebular magnetic field. As suggested by Chevalier (2004) and Djannati-Atai et al. (2008), these PWNe may not be in energy equipartition between particles and magnetic fields, as is the case for the Crab Nebula. Instead, these may be particle-dominated objects. However, proper modeling of each of these PWNe and its surroundings is needed to constrain the nebular magnetic fields.

Given the association by Leahy et al. (2008) of the PWN with a molecular CO cloud, an alternative interpretation of the TeV emission from G54.1+0.3 would be radiation from the decay of neutral pions produced in the hadronic interactions produced between the dense target and the SNR. To establish if this is a compatible scenario, deeper observations of this source would be needed to constrain the size and location of the accelerated particles in the TeV range. A detection by the Fermi Large Area Telescope would add data to the spectral energy distribution of the system, giving an idea of the possible role played by protons by showing (or not) the typical bump in the spectrum expected from neutral pions (e.g., Aharonian et al. 1994). However, based on the association with a high spin-down pulsar, a comparable size of the X-ray and radio PWNe given the instrument resolutions and comparison with similar detected objects, the PWN scenario best explains the data. Under the assumption that the gamma-ray production in VER J1930+188 is IC emission, the recently discovered IR shell of ejecta is an additional source of seed photons from the local dust up-scattered into the TeV energies and contributing in the observed emission.

This research is supported by grants from the U.S. Department of Energy, the U.S. National Science Foundation, and the Smithsonian Institution, by NSERC in Canada, by Science Foundation Ireland, and by STFC in the UK.

Facility: VERITAS - Very Energetic Radiation Imaging Telescope Array System