Panoramic SETI Program Update and High-Energy Astrophysics Applications J er ome Mairea Shelley A. Wrightab Jamie Holderc David Andersond Wystan Benbowe

2025-05-06 0 0 9.46MB 9 页 10玖币
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Panoramic SETI: Program Update and High-Energy
Astrophysics Applications
J´erˆome Mairea, Shelley A. Wrighta,b, Jamie Holderc, David Andersond, Wystan Benbowe,
Aaron Browna, Maren Cosensa,b, Gregory Footec, William F. Hanlone, Olivier Hervetf, Paul
Horowitzg, Andrew W. Howardh, Ryan Leed, Wei Liud,i, Rick Raffantij, Nicolas Rault-Wangd,i,
Remington P. S. Stonek, Dan Werthimerd,i, James Wileya,b, and David A. Williamsf
aCenter for Astrophysics & Space Sciences, University of California San Diego, CA, USA
bDepartment of Physics, University of California San Diego, CA, USA
cDepartment of Physics and Astronomy, University of Delaware, DE, USA.
dSpace Sciences Laboratory, University of California Berkeley, CA, USA
eCenter for Astrophysics |Harvard & Smithsonian, Cambridge, MA, USA
fSanta Cruz Institute for Particle Physics and Department of Physics, University of California,
Santa Cruz, CA, USA
gDepartment of Physics, Harvard University, Cambridge, MA, USA
hAstronomy Department, California Institute of Technology, Pasadena, CA, USA
iDepartment of Astronomy, University of California Berkeley, CA, USA
jTechne Instruments, Oakland, CA, USA
kUniversity of California Observatories, Lick Observatory, CA, USA
ABSTRACT
Optical SETI (Search for Extraterrestrial Intelligence) instruments that can explore the very fast time domain,
especially with large sky coverage, offer an opportunity for new discoveries that can complement multimessenger
and time domain astrophysics. The Panoramic SETI experiment (PANOSETI) aims to observe optical transients
with nanosecond to second duration over a wide field-of-view (2,500 sq.deg.) by using two assemblies of tens
of telescopes to reject spurious signals by coincidence detection. Three PANOSETI telescopes, connected to a
White Rabbit timing network used to synchronize clocks at the nanosecond level, have been deployed at Lick
Observatory on two sites separated by a distance of 677 meters to distinguish nearby light sources (such as
Cherenkov light from particle showers in the Earth’s atmosphere) from astrophysical sources at large distances.
In parallel to this deployment, we present results obtained during four nights of simultaneous observations with
the four 12-meter VERITAS gamma-ray telescopes and two PANOSETI telescopes at the Fred Lawrence Whipple
Observatory. We report PANOSETI’s first detection of astrophysical gamma rays, comprising three events with
energies in the range between 15 TeV and 50 TeV. These were emitted by the Crab Nebula, and identified
as gamma rays using joint VERITAS observations.
Keywords: Nanosecond timing, transients, Cherenkov shower, Cosmic Rays, Gamma Rays, SETI
1. INTRODUCTION
Astronomical instruments with precision time resolution can be employed to search for technosignatures by means
of detecting nano- to milli-second light pulses that could be emitted, for instance, for the purpose of interstellar
communications or energy transfer. Numerous programs have been conducted to search for technosignatures
using optical wavelengths17including near-infrared.8With 0.32 sq.deg. of instantaneous field-of-view, the first
optical SETI all-sky surveys9,10 used a transit observing approach to cover the sky in 150 clear nights. To
Further author information: (Send correspondence to J.M.)
J.M.: E-mail: jmaire@ucsd.edu
arXiv:2210.01356v1 [astro-ph.IM] 4 Oct 2022
efficiently and constantly survey the entire sky, however, groups of single-aperture telescopes capable of collecting
light instantaneously from different parts of the sky are still required.
The Panoramic SETI experiment (PANOSETI1114) is an all-sky observatory project aiming to detect tran-
sients that will cover a wide range of timescales in a search for nanosecond to second pulsed light signals across all
optical wavelengths. Each part of the sky is observed simultaneously from two locations for direct detection and
confirmation of transients. Based upon two assemblies of twenty-four 0.46-m Fresnel-lens telescopes equipped
with fast, low-noise silicon photo-multipliers operating in the 0.32–0.85 µm spectral range, the PANOSETI in-
strument can detect flashes of light that could have been sent from kiloparsec distances and beamed toward our
direction. For instance, a pulse of light emitted by a laser delivering 20 ns shaped pulses of megajoule energies
and collimated with a 10-m telescope located at 1 kpc away from us would be orders of magnitude brighter than
the entire broadband visible stellar background from our perspective.4
The small aperture, wide field-of-view, and low cost of the PANOSETI telescopes also make them potentially
well-suited for gamma-ray astronomy at the highest energies. When a high-energy gamma-ray photon or cosmic-
ray particle enters the Earth’s atmosphere, it initiates a particle cascade which can be detected via the pulse of
blue Cherenkov radiation it emits. Ground-based gamma-ray telescopes exploit this effect, using large aperture
(>10 m) mirrors and fast photo-detector cameras to record Cherenkov images of the showers. Subsequent
analysis of these images allows determination of the nature of the primary (photon or particle), its arrival
direction and its energy. The energy range covered by this technique is typically from around 100 GeV to tens
of TeV, reaching 100 TeV only for the brightest sources. Hundreds of astrophysical gamma-ray sources, both
Galactic and extragalactic, have been identified using this technique. At higher energies, direct detection of the
shower particles is used; recent results from the LHAASO collaboration have revealed the existence of gamma-ray
emitters extending up to PeV energies.15 The main benefit of this particle detection approach is that it provides
the large effective area (>1 km2) which is required to measure the extremely low flux of gamma rays at the
highest energy. Cherenkov telescopes can operate in the same energy range, but are typically non-imaging, to
reduce unit cost (e.g., TAIGA-HiScore16). The unit cost of PANOSETI telescopes is approximately two orders
of magnitude less than a large aperture imaging Cherenkov telescope, such as those that make up the VERITAS
array. A large array of low-cost PANOSETI telescopes, each equipped with a 1,000 pixel camera, would permit
applying the benefits of the imaging technique (excellent angular resolution, energy resolution and background
discrimination) to the PeV regime.
We describe in Sect.2the recent deployment of a third PANOSETI telescope at Lick Observatory providing
a baseline separation of 677-m. We report in Sect.3results obtained from joint PANOSETI and VERITAS
observations at the Whipple Observatory in November 2021.
2. PANOSETI: PROGRAM UPDATE
The PANOSETI experiment aims to observe 2,350 square degrees instantaneously by making use of multiple
large field-of-view telescopes. PANOSETI is currently in its final design phase, and at final production two
dedicated observatories will house 24 telescopes per site. Each part of the sky is observed simultaneously from
two locations for direct detection and confirmation of optical transients.
Each telescope is equipped with a 0.46-m f/1.32 Fresnel-lens which focuses the light onto a 32x32-pixel photon-
counting detector subdivided into 16 adjacent 8x8-pixel Multi-Pixel Photon Counter (Hamamatsu S13361-
3050AE-08) detector arrays operating in the 0.32 - 0.85 µm spectral range. These silicon photomultipliers (SiPMs)
are comprised of Geiger-mode-operated avalanche photodiodes highly linear in pulse intensity, with a high in-
ternal gain to enable single-photon detection while featuring low dark count (<1 Mcps per SiPM), high photon
detection efficiency in the visible (45%), and nanosecond timing resolution. Each PANOSETI detector contains
four custom readout boards that make use of a 64-bit Application-Specific Integrated Circuit (ASIC) capable of
pulse shaping and trigger detection of individual pulses. Each detector board reads four 8x8 pixel SiPM arrays
that feed four ASICs, amplifying the signal and delivering a per-pixel trigger signal to a Field Programmable Gate
Array (FPGA). A 1 Gb per second fiber connection provides data communications to a central multi-telescope
10 Gb network switch connected to a central computer.
http://tevcat.uchicago.edu/
摘要:

PanoramicSETI:ProgramUpdateandHigh-EnergyAstrophysicsApplicationsJer^omeMairea,ShelleyA.Wrighta,b,JamieHolderc,DavidAndersond,WystanBenbowe,AaronBrowna,MarenCosensa,b,GregoryFootec,WilliamF.Hanlone,OlivierHervetf,PaulHorowitzg,AndrewW.Howardh,RyanLeed,WeiLiud,i,RickRa antij,NicolasRault-Wangd,i,Rem...

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