Alison Mitchell’s research while affiliated with Friedrich-Alexander-University Erlangen-Nürnberg and other places

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Publications (65)


Fig. 8. Neutrino flux prediction for our re-acceleration model, for reference the current generation of neutrino detectors have an optimal sensitivity at 100 TeV of approximately 10 −12 erg cm −2 s −1 (Aartsen et al. 2019).
Fixed parameters set in the simulation with associated values based on previous literature.
Hadronic emission from the environment of the Crab Pulsar Wind Nebula by re-accelerated particles
  • Preprint
  • File available

April 2025

Samuel T. Spencer

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Alison M. W. Mitchell

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Brian Reville

The observation of peta-electronvolt (PeV) γ\gamma-ray photons from the Crab Nebula by LHAASO has revitalised the possibility of a secondary population of hadrons producing the highest energy emission through neutral pion decay. Despite previous studies modelling this population, the origin of such high-energy hadronic particles remains unclear. We consider possible acceleration scenarios for multi PeV particles in the Crab Nebula environment, including one in which high-energy protons produced at the supernova remnant's outer shock diffuse into the pulsar wind nebula. Particles which reach the Crab Pulsar's wind termination shock can be accelerated to the required energies, and subsequently interact with the dense filaments surrounding the nebula. We perform particle transport simulations of this scenario, including the effects of the expansion of the pulsar wind nebula into the surrounding supernova ejecta. We find that this results in PeV photons being produced over the lifetime of the Crab system, without over-estimating the flux at lower energies or exceeding the energy budget of the Crab Pulsar. This results in a reasonable match to the LHAASO data at the highest energies. We also present predictions for the resulting all-flavour neutrino flux, finding it to be approximately an order of magnitude below the sensitivity of current generation instruments.

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Clustering analysis of Fermi-LAT unidentified point sources

April 2025

Giovanni Cozzolongo

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Alison M. W. Mitchell

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Samuel T. Spencer

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[...]

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Tim Unbehaun

The Fermi Large Area Telescope (LAT) has detected thousands of sources since its launch in 2008, with many remaining unidentified. Some of these point sources may arise from source confusion. Specifically, there could be extended sources erroneously described as groups of point sources. Using the DBSCAN clustering algorithm, we analyze unidentified Fermi-LAT sources alongside some classified objects from the 4FGL-DR4 catalog. We identified 44 distinct clusters containing 106 sources, each including at least one unidentified source. Detailed modeling of selected clusters reveals some cases where extended source models are statistically preferred over multiple point sources. The work is motivated by prior observations of extended TeV gamma-ray sources, such as HESS J1813-178, and their GeV counterparts. In the case of HESS J1813-178, two unidentified Fermi-LAT point sources were detected in the region. Subsequent multiwavelength analysis combining TeV and GeV data showed that a single extended source is a better description of the emission in this region than two point-like sources.


Deriving pulsar pair-production multiplicities from pulsar wind nebulae using H.E.S.S. and LHAASO observations

February 2025

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1 Read

Pulsar Wind Nebulae (PWNe) dominate the galactic gamma-ray sky at very high energies, and are major contributors to the leptonic cosmic ray flux. However, whether or not pulsars also accelerate ions to comparable energies is not yet experimentally confirmed. We aim to constrain the birth period and pair-production multiplicity for a set of pulsars. In doing so, we aim to constrain the proportion of ions in the pulsar magnetosphere and hence the proportion of ions that could enter the pulsar wind. We estimate possible ranges of the value of the average pair production multiplicity for a sample of 26 pulsars in the Australia Telescope National Facility (ATNF) catalogue, which have also been observed by the High Energy Stereoscopic System (H.E.S.S.) telescopes. We then derive lower limits for the pulsar birth periods and average pair production multiplicities for a subset of these sources where the extent of the pulsar wind nebula and surrounding supernova shell have been measured in the radio. We also derive curves for the average pair production multiplicities as a function of birth period for sources recently observed by the Large High Altitude Air Shower Observatory (LHAASO). We show that there is a potential for hadrons entering the pulsar wind for most of the H.E.S.S. and LHAASO sources we consider, dependent upon the efficiency of luminosity conversion into particles. We also present estimates of the pulsar birth period for six of these sources, which all fall into the range of \simeq10-50 ms.


eROSITA X-ray analysis of the PeVatron candidate Westerlund 1

January 2025

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12 Reads

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1 Citation

Astronomy and Astrophysics

Context. It is still unclear which fraction of cosmic rays above an energy of 1 PeV is accelerated by the observed Galactic PeVatron population. These sources of unknown physical origin are detected through their γ -ray emission, which also identifies them as particle accelerators. However, their γ -ray data are typically degenerate between hadronic and leptonic emission scenarios, which hinders their straightforward association with the mainly hadronic cosmic ray population. Aims. In this study, we aimed to distinguish between leptonic and hadronic particle acceleration scenarios for the PeVatron candidate HESS J1646−458, which is associated with the star cluster Westerlund 1 (Wd 1). To this end, we first studied the diffuse X-ray emission from Wd 1 to better understand if its origin is of thermal or nonthermal nature. In addition, we searched for X-ray synchrotron emission from the associated PeVatron candidate HESS J1646−458 to put new constraints on the magnetic field strength and the leptonic particle population of this source. Methods. We used data from the all-sky surveys 1 to 4 of the extended Roentgen Survey with an Imaging Telescope Array ( eROSITA ) on board the Spectrum-Roentgen-Gamma orbital platform to spectrally analyze the diffuse emission from Wd 1 and HESS J1646−458. For Wd 1, we fitted and compared a purely thermal model and a model with a thermal and a nonthermal component. Next, we analyzed the spectra of four annuli around Wd 1 that coincide with HESS J1646−458 to search for synchrotron radiation. Results. We find that eROSITA data cannot distinguish between thermal and nonthermal source scenarios for the diffuse emission from Wd 1 itself. For a thermal source scenario, the observed X-ray flux can be explained in large part by unresolved pre-main sequence stars or by thermalized stellar wind shocks. In the case of the PeVatron candidate HESS J1646−458, we find no evidence of synchrotron emission. We estimated an upper confidence bound of the synchrotron flux up to 40 ′ around Wd 1 of 1.9 ⋅ 10 ⁻³ keV ⁻¹ cm ⁻² s ⁻¹ . We used this result to study the spectral energy distribution of the source. From that, we obtained an upper 1 σ confidence bound on the magnetic field strength of HESS J1646−458 of 7 μG. Conclusions. Our upper bound on the magnetic field strength in HESS J1646−458 is compatible with a previous estimate in the literature for a fully leptonic source scenario. Therefore, a purely leptonic emission scenario is compatible with our results. The same is the case for hadronic and hybrid scenarios, for which even less synchrotron flux is expected compared to the leptonic scenario.


Fig. 6. Histograms of the residua obtained via subtracting background from source spectra in blue with corresponding Gaussian fits in red. Region pairs 1, 2, 3, and 4 correspond to panels a), b), c), and d), respectively. For each region pair, we employed the minimum bin size which resulted in no empty bins
Fig. 7. Upper panels: Spectra of the four source regions 1, 2, 3, and 4 with the corresponding background model fits in panels a), b), c), and d), respectively. The main model components are shown using different colors and line styles: The LHB is red and dashed, the CGM is orange and dashed-dotted, the corona is yellow and solid, the CXB is light blue and dashed, and the GX 340+0 halo components are purple and dotted. Lower panels: Normalized residua of the fits.
Fig. A.1. eROSITA RGB image of the surroundings of Wd 1. Red, green, and blue colors correspond to 0.7 to 1.1 keV, 1.1 to 2.3 keV, and 2.3 to 10 keV, respectively. The image was smoothed using a Gaussian kernel with standard deviation 10 arcsec. The large annulus indicates the background region for the Wd 1 spectral fit, from which the white circle around Wd 1 itself was excluded.
Fig. C.1. Spectral energy distribution fits to HESS J1646−458, assuming E min = 100 MeV (upper panel) and E min = 1 GeV (lower panel). The data is, from left to right: the Planck radio upper limit in red, the eROSITA X-ray upper confidence bound in orange, the Fermi-LAT HE γ-ray upper limit in blue, and the H.E.S.S. VHE γ-ray data from Aharonian et al. (2022) in purple. The solid orange lines are synchrotron radiation and the solid blue lines are IC scattering. The different target photon contributions to the IC scattering are given by the thin black lines: The CMB is solid, diffuse Galactic infrared radiation dashed, diffuse Galactic optical light dashed-dotted, and Wd 1's photon field dotted.
eROSITA X-ray Analysis of the PeVatron Candidate Westerlund 1

January 2025

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5 Reads

It is unclear which fraction of cosmic rays above an energy of 1 PeV is accelerated by the observed Galactic PeVatron population. These sources' gamma-ray data is typically degenerate between hadronic and leptonic emission scenarios, which hinders their straightforward association with the cosmic ray population. Here, we aimed to distinguish between leptonic and hadronic particle acceleration scenarios for the PeVatron candidate HESS J1646-458, associated with the star cluster Westerlund 1 (Wd 1). We first studied the diffuse X-ray emission from Wd 1 to better understand if its origin is of thermal or nonthermal nature. In addition, we searched for X-ray synchrotron emission from the associated PeVatron candidate HESS J1646-458 to put new constraints on the magnetic field strength and the leptonic particle population of this source. We used data from eROSITA on board the SRG orbital platform to spectrally analyze the diffuse emission from Wd 1 and HESS J1646-458. For Wd 1, we compared a purely thermal model and a model with a thermal and a nonthermal component. Next, we analyzed the spectra of four annuli around Wd 1 which coincide with HESS J1646-458 to search for synchrotron radiation. We find that eROSITA data cannot distinguish between thermal and nonthermal source scenarios for the diffuse emission from Wd 1 itself. In the case of HESS J1646-458, we find no evidence of synchrotron emission. We estimated an upper confidence bound of the synchrotron flux up to 40' around Wd 1 of 1.9e-3 keV-1 cm-2 s-1, which we used to study the spectral energy distribution of the source. From this, we obtained an upper 1 sigma bound on the magnetic field strength of HESS J1646-458 of 7 uG. This is compatible with a previous estimate in the literature for a fully leptonic source scenario. A purely leptonic emission scenario, a hadronic, and a hybrid one are compatible with our results.


Simultaneous two-colour intensity interferometry with H.E.S.S

November 2024

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7 Reads

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2 Citations

Monthly Notices of the Royal Astronomical Society

In recent years, intensity interferometry has been successfully applied to the Imaging Atmospheric Cherenkov Telescopes H.E.S.S. , MAGIC, and VERITAS. All three telescope systems have proven the feasibility and capability of this method. After our first campaign in 2022, when two of the H.E.S.S. telescopes in Namibia were equipped with our external setup and the angular diameter of two stars was measured, our setup was upgraded for a second campaign in 2023, where the goal is to perform simultaneous two colour measurements. The second campaign not only involves a third equipped telescope, but also each mechanical setup now includes two interference filters at two different wavelengths (375 nm and 470 nm) with a broader bandwidth of 10 nm. This enables having simultaneous two-colour measurements, which yields information about the star’s physical size at different wavelengths. This is the first time that simultaneous dual-waveband intensity interferometry measurements are performed. The angular diameter results of the 4 stars, Mimosa (β Cru), Eta Centauri (η Cen), Nunki (σ Sgr) and Dschubba (δ Sco), are reported, where the effects of limb darkening are also taken into account.


Figure 3. Schematic of the intensity interferometer including optics and data transfer. Each telescope has an identical setup. The blue bandpass filter for the transmitted light has a wavelength of 470 nm and the purple one for the reflected beam a wavelength of 375 nm. Both have a bandwidth of 10 nm. The main difference to the optics of the 2022 campaign is the order of lenses and filters. For the single colour measurements in 2022 the order was lens-filterlens-beamsplitter-detectors. For the two waveband measurements in 2023 the order was lens-beamsplitter-filters-lens-detectors.
List of the measurement segments and segment times in minutes for each star.
Zero baseline amplitudes computed by the UD fit model in fs for each filter colour and their weighted average.
Stellar targets and their characteristic parameters. Spectral types and B magnitudes are taken from SIMBAD. The reference angular diameters are recovered from NSII (Hanbury Brown 1974), where the stars were measured at a wavelength of 443 nm, and from Underhill et al. (1979a). í µí±‡ eff is the effective temperature of the star and log(g) is the surface gravity. These are parameters needed to derive the LD coefficient í µí±¢ í µí¼† . í µí±Ž values are from Cohen et al. (2008), í µí± values are from Arcos et al. (2018a), í µí± values are from Underhill et al. (1979b), í µí±‘ values are from Arcos et al. (2018b).
Table of observed stars and their measured angular diameters listed with their uncertainties for the UD and LD model and for 470 nm and 375 nm.
Simultaneous Two Colour Intensity Interferometry with H.E.S.S

November 2024

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16 Reads

In recent years, intensity interferometry has been successfully applied to the Imaging Atmospheric Cherenkov Telescopes H.E.S.S. , MAGIC, and VERITAS. All three telescope systems have proven the feasibility and capability of this method. After our first campaign in 2022, when two of the H.E.S.S. telescopes in Namibia were equipped with our external setup and the angular diameter of two stars was measured, our setup was upgraded for a second campaign in 2023, where the goal is to perform simultaneous two colour measurements. The second campaign not only involves a third equipped telescope, but also each mechanical setup now includes two interference filters at two different wavelengths (375 nm and 470 nm) with a broader bandwidth of 10 nm. This enables having simultaneous two colour measurements, which yields information about the star's physical size at different wavelengths. This is the first time that simultaneous dual-waveband intensity interferometry measurements are performed. The angular diameter results of the 4 stars, Mimosa (beta Cru), Eta Centauri (eta Cen), Nunki (sigma Sgr) and Dschubba (delta Sco), are reported, where the effects of limb darkening are also taken into account.


Detectability of Supernova Remnants with the Southern Wide-field Gamma-ray Observatory

October 2024

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3 Reads

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1 Citation

Supernova remnants (SNRs) remain prime candidates for hadronic particle acceleration within our galaxy, accounting for much of the Cosmic Ray flux. Next-generation instruments such as the Southern Wide-field Gamma-ray Observatory (SWGO) will be of crucial importance in identifying new candidate SNRs. SWGO will observe two-thirds of the gamma-ray sky, covering the energy range between a few hundreds GeV and a PeV. In this work, we apply a model of SNR evolution to predict their gamma-ray spectra. Furthermore, we use our model in combination with the target SWGO sensitivity range to explore the SNR emission phase space and quantify detection prospects for SWGO. Finally, we validate our model for sources observed with current-generation instruments, fitting it using a Monte-Carlo Markov Chain technique to the observed gamma-ray emission from four SNRs. We anticipate that at least 8 SNRs will be detected by SWGO within 1 year.



A background-estimation technique for the detection of extended gamma-ray structures with IACTs

September 2024

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19 Reads

Estimation of the amount of cosmic-ray induced background events is a challenging task for Imaging Atmospheric Cherenkov Telescopes (IACTs). Most approaches rely on a model of the background signal derived from archival observations, which is then normalised to the region of interest (ROI) and respective observation conditions using emission-free regions in the observation.This is, however, disadvantageous for the analysis of large, extended γ\gamma-ray structures, where no sufficient source free region can be found. We aim to address this issue by estimating the normalisation of a 3-dimensional background model template from separate, matched observations of emission-free sky regions. As a result, the need for a emission-free region in the field of view of the observation becomes unnecessary. For this purpose, we implement an algorithm to identify observation pairs with as close as possible observation conditions. The open-source analysis package Gammapy is utilized for estimating the background rate, facilitating seamless adaptation of the framework to many γ\gamma-ray detection facilities. Public data from the High Energy Stereoscopic System (H.E.S.S.) is employed to validate this methodology. The analysis demonstrates that employing a background rate estimated through this run-matching approach yields results consistent with those obtained using the standard application of the background model template. Furthermore, the compatibility of the source parameters obtained through this approach with previous publications and an analysis employing the background model template approach is confirmed, along with an estimation of the statistical and systematic uncertainties introduced by this method.


Citations (31)


... If the emission is caused by jets, it may indicate areas of higher energy if the jets are oriented within the galaxy plane and thus pushing through denser material. It also suggests that the emission may instead be similar to a superbubble (e.g., Ando et al. 2023), or massive star clusters (e.g., Westerlund 1; K. Haubner et al. 2025). All of these are areas of potential particle acceleration and CR or neutrino origin. ...

Reference:

ASKAP and VLASS Search for a Radio-continuum Counterpart of Ultra-high-energy Neutrino Event KM3–230213A
eROSITA X-ray analysis of the PeVatron candidate Westerlund 1

Astronomy and Astrophysics

... To quantify the number of SNRs detectable to SWGO, the previous analysis from Scharrer et al. (2024) was repeated using the same simplistic model, but with updated sensitivity curves used throughout this work. The results of this are shown in Figure 17. ...

Detectability of Supernova Remnants with the Southern Wide-field Gamma-ray Observatory
  • Citing Preprint
  • October 2024

... The presence of dense gas targets, such as interstellar clouds nearby the accelerators, might provide evidence for the escaping flux of particles through the production of gamma rays and neutrinos at hadronic collisions. In this respect, recent wide field-of-view survey instruments have revealed an unexpectedly large population of Galactic gamma ray sources at UHE (larger than 100 TeV) with no counterpart and the scenario of molecular clouds illuminated by nearby SNRs appears to be a viable explanation [12]. Finally, SNe can source not only neutrinos but also Gravitational Waves (GW). ...

Exploring the supernova remnant contribution to the first LHAASO source catalog via passively illuminated interstellar clouds
  • Citing Article
  • October 2024

Journal of High Energy Astrophysics

... Intriguingly, it has recently been reported that the activity of the galaxy SDSS J1430+2303, at a distance of 378 Mpc from Earth hints at a possible SMBH merger within three years [63,64]. The system is currently being monitored by HESS [65], while a gravitational wave signal will be in the observation window of PTAs. ...

Monitoring the first candidate host for the merger of a Supermassive Black Hole Binary with H.E.S.S.

... These challenges can only be addressed with further multiwavelength follow-up investigations of flaring blazars in temporal and spatial coincidence with astrophysical neutrino alerts, both single high energy neutrino events and those within the framework of the GFU program. Furthermore, as seen in Schüssler et al. (2023), such studies are even more effective when we combine observations from multiple IACTs in order to provide a more complete coverage of the entire sky. This also helps to account for cases where the visibility of a source from a single observatory site is adversely affected due to factors such as bad weather, the presence of the Sun or Moon, or technical problems. ...

Joint searches by FACT, H.E.S.S., MAGIC and VERITAS for VHE gamma-ray emission associated with neutrinos detected by IceCube
  • Citing Conference Paper
  • July 2023

... Radio galaxy PKS 0625-35.-Reference [92] reported the association of three IceCube neutrinos with energies between 63 and 302 TeV with a flare of the radio galaxy PKS 0625-35. The pre-trial significance of this apparent association was 3.6σ. ...

H.E.S.S. realtime follow-ups of IceCube high-energy neutrino alerts

... Given the more accurate likelihood description achieved with the FreePACT method, this parameter should become an even more powerful discriminant. These parameters can also be of further use elsewhere, for example for the generation of classes of events with different reconstruction quality as foreseen for CTA [38]. Finally, all of the results presented in this work are derived from simulations of air showers and telescopes. ...

Performance update of an event-type based analysis for the Cherenkov Telescope Array
  • Citing Conference Paper
  • July 2023

... Observations and MC simulations were then consistently processed with the official software cta-lstchain [6]. Developing pybkgmodel, a suite of tools for residual background modeling [8], we evaluated the background with the exclusion-map method [9]. On modeling signals, using standard tools included in gammapy [10,11], we performed a spatially resolved spectral fit of predefined models to the data. ...

Pybkgmodel - a background modelling toolbox for the CTA

... Further updates of the algorithm that are being considered include the implementation of increased flexibility of exposure times for individual pointings, possibly computed based on the assumption of the energy spectrum and lightcurve of the transient phenomena to be observed. tilepy is customized to tackle this case, to study the optimal exposure to detect the source in GW follow-ups by the next generation IACT, the Cherenkov Telescope Array Observatory (Green et al. 2023). A generalization of this custom method to generic spectrum, lightcurve, and instrument response function, to obtain the exposure per pointing required for the source detection, is planned for the near future. ...

Chasing Gravitational Waves with the Chereknov Telescope Array

... The assessment of the sensitivity of the planned GPS to a DM sub-halo signal presented in this paper is a proof of principle, aimed to show that the GPS is complementary to previously suggested strategies for sub-halo detection. In case of no DM sub-halo detection, the sensitivity of the GPS to constrain the DM annihilation cross section is comparable to that of other targets, for example, dSphs [90,91]. Yet, DM sub-halos are less promising targets than the signal from DM annihilation in the GC (see Sec. VI). ...

Dark matter searches in dwarf spheroidal galaxies with the Cherenkov Telescope Array
  • Citing Conference Paper
  • July 2023