E. J. Ahn’s research while affiliated with Fermi National Accelerator Laboratory (Fermilab) and other places

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Publications (142)


Figure 1. Schematic view of the internal structure of a SiPM made up of an array of cells, all connected in parallel. Each cell is composed of an APD working in Geiger mode and a quenching resistor (R Q ) in series.
Figure 3. SiPM Calibration Setup. The three stages are distinguished with dotted lines. The output of the fast shaper amplifier ( * ) has a DC offset component.
Figure 4. On the left, the measurement of the rate of the SiPM pulses as a function of the DAC value. DC level corresponds to the fast shaper DC offset component. See subsection 4.1.1 for details on the setup. On the right, the absolute value of the derivative of the rate evidences the distribution of the SPE peaks. The mean value of the SPE peak (D max ) is obtained with a Gaussian fit of the points (red curve).
Figure 5. Equations 4.4 and 4.5 are presented graphically in the plot on the left. The mean SPE peak as a function of the V bias for four different SiPMs is plotted on the right. The mean SPE peak is proportional to
Figure 6. The six stages of the setup needed for the detector calibration. The 4 m plastic scintillation bar has a threaded 5 m wavelength-shifting optical fiber. The difference in length is due to the extra fiber needed to reach the optical connector.

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Muon Counting using Silicon Photomultipliers in the AMIGA detector of the Pierre Auger Observatory
  • Preprint
  • File available

March 2017

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5 Reads

The Pierre Auger Collaboration

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A. Aab

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P. Abreu

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[...]

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F. Zuccarello

AMIGA (Auger Muons and Infill for the Ground Array) is an upgrade of the Pierre Auger Observatory designed to extend its energy range of detection and to directly measure the muon content of the cosmic ray primary particle showers. The array will be formed by an infill of surface water-Cherenkov detectors associated with buried scintillation counters employed for muon counting. Each counter is composed of three scintillation modules, with a 10 m2^2 detection area per module. In this paper, a new generation of detectors, replacing the current multi-pixel photomultiplier tube (PMT) with silicon photo sensors (aka. SiPMs), is proposed. The selection of the new device and its front-end electronics is explained. A method to calibrate the counting system that ensures the performance of the detector is detailed. This method has the advantage of being able to be carried out in a remote place such as the one where the detectors are deployed. High efficiency results, i.e. 98 % efficiency for the highest tested overvoltage, combined with a low probability of accidental counting (\sim2 %), show a promising performance for this new system.

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Muon Counting using Silicon Photomultipliers in the AMIGA detector of the Pierre Auger Observatory

March 2017

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950 Reads

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28 Citations

Journal of Instrumentation

AMIGA (Auger Muons and Infill for the Ground Array) is an upgrade of the Pierre Auger Observatory designed to extend its energy range of detection and to directly measure the muon content of the cosmic ray primary particle showers. The array will be formed by an infill of surface water-Cherenkov detectors associated with buried scintillation counters employed for muon counting. Each counter is composed of three scintillation modules, with a 10 m² detection area per module. In this paper, a new generation of detectors, replacing the current multi-pixel photomultiplier tube (PMT) with silicon photo sensors (aka. SiPMs), is proposed. The selection of the new device and its front-end electronics is explained. A method to calibrate the counting system that ensures the performance of the detector is detailed. This method has the advantage of being able to be carried out in a remote place such as the one where the detectors are deployed. High efficiency results, i.e. 98% efficiency for the highest tested overvoltage, combined with a low probability of accidental counting (~2%), show a promising performance for this new system.


Testing Hadronic Interactions at Ultrahigh Energies with Air Showers Measured by the Pierre Auger Observatory

October 2016

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154 Reads

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235 Citations

Physical Review Letters

Ultrahigh energy cosmic ray air showers probe particle physics at energies beyond the reach of accelerators. Here we introduce a new method to test hadronic interaction models without relying on the absolute energy calibration, and apply it to events with primary energy 6-16 EeV (E_CM = 110-170 TeV), whose longitudinal development and lateral distribution were simultaneously measured by the Pierre Auger Observatory. The average hadronic shower is 1.33 +- 0.16 (1.61 +- 0.21) times larger than predicted using the leading LHC-tuned models EPOS-LHC (QGSJetII-04), with a corresponding excess of muons.


FIG. 3. The contributions of different components to the average signal as a function of zenith angle, for stations at 1 km from the shower core, in simulated 10 EeV proton air showers illustrated for QGSJet-II-04.
FIG. 4. Best-fit values of RE and R had for QGSJet-II-04 and EPOS-LHC, for pure proton (solid circle/square) and mixed composition (open circle/square). The ellipses and gray boxes show the 1-σ statistical and systematic uncertainties.
Testing Hadronic Interactions at Ultrahigh Energies with Air Showers Measured by the Pierre Auger Observatory

Ultrahigh energy cosmic ray air showers probe particle physics at energies beyond the reach of accelerators. Here we introduce a new method to test hadronic interaction models without relying on the absolute energy calibration, and apply it to events with primary energy 6-16 EeV (E_CM = 110-170 TeV), whose longitudinal development and lateral distribution were simultaneously measured by the Pierre Auger Observatory. The average hadronic shower is 1.33 +- 0.16 (1.61 +- 0.21) times larger than predicted using the leading LHC-tuned models EPOS-LHC (QGSJetII-04), with a corresponding excess of muons.


Table 1 Observed r G (X * max , S * 38 ) with statistical uncertainty, and simulated r G (X * max , S * 38 ) for various compositions using different interaction models (statistical uncertainties 
Fig. 2. Dependence of the correlation coefficients r G on σ (ln A) for EPOS-LHC (left) and QGSJetII-04 (right). Each simulated point corresponds to a mixture with different fractions of protons, helium, oxygen and iron nuclei, the relative fractions changing in 0.1 steps (4 points for pure compositions are grouped at σ (ln A) = 0). Colors of the points indicate ln A of the corresponding simulated mixture. The shaded area shows the observed value for the data. Vertical dotted lines indicate the range of σ (ln A) in simulations compatible with the observed correlation in the data. the maximum spread of masses 0.5 p-0.5 Fe (σ (ln A) 2) for all three interaction models. For the data, a negative correlation of r G (X * max , S * 38 ) = −0.125 ± 0.024 (stat) is found. For proton simulations correlations are close to zero or positive in all models. Pure compositions of heavier primaries show even more positive correlations (r G ≥ 0.09) than for protons. Hence, observations cannot be reproduced by any pure composition of mass A ≥ 1, irrespective of the interaction model chosen. In the proton dip model, even small admixtures of heavier nuclei, such as a 15-20% helium fraction at the sources, were shown to upset the agreement of the pair-production dip of protons with the observed flux [1,2,26,27]. The values of r G in simulations for a mixture at Earth of 0.8 p-0.2 He are added in Table 1. They are essentially unaltered compared to the pure proton case and equally inconsistent to the observed correlation. 
Evidence for a mixed mass composition at the ‘ankle’ in the cosmic-ray spectrum

September 2016

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199 Reads

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140 Citations

Physics Letters B

We report a first measurement for ultrahigh energy cosmic rays of the correlation between the depth of shower maximum and the signal in the water Cherenkov stations of air-showers registered simultaneously by the fluorescence and the surface detectors of the Pierre Auger Observatory. Such a correlation measurement is a unique feature of a hybrid air-shower observatory with sensitivity to both the electromagnetic and muonic components. It allows an accurate determination of the spread of primary masses in the cosmic-ray flux. Up till now, constraints on the spread of primary masses have been dominated by systematic uncertainties. The present correlation measurement is not affected by systematics in the measurement of the depth of shower maximum or the signal in the water Cherenkov stations. The analysis relies on general characteristics of air showers and is thus robust also with respect to uncertainties in hadronic event generators. The observed correlation in the energy range around the ‘ankle’ at differs significantly from expectations for pure primary cosmic-ray compositions. A light composition made up of proton and helium only is equally inconsistent with observations. The data are explained well by a mixed composition including nuclei with mass . Scenarios such as the proton dip model, with almost pure compositions, are thus disfavored as the sole explanation of the ultrahigh-energy cosmic-ray flux at Earth.


Measurement of the Radiation Energy in the Radio Signal of Extensive Air Showers as a Universal Estimator of Cosmic-Ray Energy

May 2016

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1 Read

We measure the energy emitted by extensive air showers in the form of radio emission in the frequency range from 30 to 80 MHz. Exploiting the accurate energy scale of the Pierre Auger Observatory, we obtain a radiation energy of 15.8 \pm 0.7 (stat) \pm 6.7 (sys) MeV for cosmic rays with an energy of 1 EeV arriving perpendicularly to a geomagnetic field of 0.24 G, scaling quadratically with the cosmic-ray energy. A comparison with predictions from state-of-the-art first-principle calculations shows agreement with our measurement. The radiation energy provides direct access to the calorimetric energy in the electromagnetic cascade of extensive air showers. Comparison with our result thus allows the direct calibration of any cosmic-ray radio detector against the well-established energy scale of the Pierre Auger Observatory.


Measurement of the Radiation Energy in the Radio Signal of Extensive Air Showers as a Universal Estimator of Cosmic-Ray Energy

May 2016

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431 Reads

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179 Citations

Physical Review Letters

We measure the energy emitted by extensive air showers in the form of radio emission in the frequency range from 30 to 80 MHz. Exploiting the accurate energy scale of the Pierre Auger Observatory, we obtain a radiation energy of 15.8 \pm 0.7 (stat) \pm 6.7 (sys) MeV for cosmic rays with an energy of 1 EeV arriving perpendicularly to a geomagnetic field of 0.24 G, scaling quadratically with the cosmic-ray energy. A comparison with predictions from state-of-the-art first-principle calculations shows agreement with our measurement. The radiation energy provides direct access to the calorimetric energy in the electromagnetic cascade of extensive air showers. Comparison with our result thus allows the direct calibration of any cosmic-ray radio detector against the well-established energy scale of the Pierre Auger Observatory.


Prototype muon detectors for the AMIGA component of the Pierre Auger Observatory

May 2016

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11 Reads

Auger Muons and Infill for the Ground Array) is an upgrade of the Pierre Auger Observatory to extend its range of detection and to directly measure the muon content of the particle showers. It consists of an infill of surface water-Cherenkov detectors accompanied by buried scintillator detectors used for muon counting. The main objectives of the AMIGA engineering array, referred to as the Unitary Cell, are to identify and resolve all engineering issues as well as to understand the muon-number counting uncertainties related to the design of the detector. The mechanical design, fabrication and deployment processes of the muon counters of the Unitary Cell are described in this document. These muon counters modules comprise sealed PVC casings containing plastic scintillation bars, wavelength-shifter optical fibers, 64 pixel photomultiplier tubes, and acquisition electronics. The modules are buried approximately 2.25 m below ground level in order to minimize contamination from electromagnetic shower particles. The mechanical setup, which allows access to the electronics for maintenance, is also described in addition to tests of the modules' response and integrity. The completed Unitary Cell has measured a number of air showers of which a first analysis of a sample event is included here.


Prototype muon detectors for the AMIGA component of the Pierre Auger Observatory

May 2016

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42 Reads

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49 Citations

Journal of Instrumentation

AMIGA (Auger Muons and Infill for the Ground Array) is an upgrade of the Pierre Auger Observatory to extend its range of detection and to directly measure the muon content of the particle showers. It consists of an infill of surface water-Cherenkov detectors accompanied by buried scintillator detectors used for muon counting. The main objectives of the AMIGA engineering array, referred to as the Unitary Cell, are to identify and resolve all engineering issues as well as to understand the muon-number counting uncertainties related to the design of the detector. The mechanical design, fabrication and deployment processes of the muon counters of the Unitary Cell are described in this document. These muon counters modules comprise sealed PVC casings containing plastic scintillation bars, wavelength-shifter optical fibers, 64 pixel photomultiplier tubes, and acquisition electronics. The modules are buried approximately 2.25 m below ground level in order to minimize contamination from electromagnetic shower particles. The mechanical setup, which allows access to the electronics for maintenance, is also described in addition to tests of the modules' response and integrity. The completed Unitary Cell has measured a number of air showers of which a first analysis of a sample event is included here.


The Pierre Auger Observatory Upgrade - Preliminary Design Report

April 2016

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1,704 Reads

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83 Citations

The Pierre Auger Observatory has begun a major Upgrade of its already impressive capabilities, with an emphasis on improved mass composition determination using the surface detectors of the Observatory. Known as AugerPrime, the upgrade will include new 4 m2^2 plastic scintillator detectors on top of all 1660 water-Cherenkov detectors, updated and more flexible surface detector electronics, a large array of buried muon detectors, and an extended duty cycle for operations of the fluorescence detectors. This Preliminary Design Report was produced by the Collaboration in April 2015 as an internal document and information for funding agencies. It outlines the scientific and technical case for AugerPrime. We now release it to the public via the arXiv server. We invite you to review the large number of fundamental results already achieved by the Observatory and our plans for the future.


Citations (88)


... ANDESPix is a digital silicon photomultiplier (SiPM) [1] Application Specific Integrated Circuit (ASIC) which has been specifically designed to detect the photons produced by scintillation and wavelength-shifting (WLS) fibers commonly used in muon detectors [2]. The future ANDES Laboratory [3] will host the next generation of muon detectors that, in turn, will take advantage of the new ASIC. ...

Reference:

ANDESPix: A Digital SiPM for Muon Detectors
Muon Counting using Silicon Photomultipliers in the AMIGA detector of the Pierre Auger Observatory

Journal of Instrumentation

... Inconsistencies in the mass-interpretations of the size of the muon signal from underground detectors [4] and from inclined showers [5] with respect to X max have been observed, being at a level of < 3σ , see Fig. 1. These inconsistencies have been measured at various energies and zenith angles, and also in surface-detector signals at lower zenith angles where the total signal is induced by a combination of muonic and electromagnetic particles [6]. Given the X max expectations, the size of the muon component predicted by the models of hadronic interactions needs to be increased by around 30-60%. ...

Testing Hadronic Interactions at Ultrahigh Energies with Air Showers Measured by the Pierre Auger Observatory
  • Citing Article
  • October 2016

Physical Review Letters

... The correlation of the ground signal and X max is a quasi-model-independent estimator of how the primary beam is mixed. It was shown in Ref. [10] that the QGSJet II-04 model provides too light mix of primary species (protons and helium nuclei only) when the fractions of primary species are fitted to the measured X max distributions in the energy range 10 18.5 − 10 19.0 eV. The measured correlation factor between the ground signal and X max is incompatible with such a mix of light primary particles. ...

Evidence for a mixed mass composition at the ‘ankle’ in the cosmic-ray spectrum

Physics Letters B

... It is important to point out that this uncertainty is independent of the cosmic-ray particle type. The fact that E em is reconstructed from radio data with no significant dependence on the incoming cosmic ray particle type makes it a very suitable energy estimator for use in the discrimination of air showers induced by different primary particles [16][17][18]. The longitudinal development of air showers can be observed directly using fluorescence telescopes. ...

Measurement of the Radiation Energy in the Radio Signal of Extensive Air Showers as a Universal Estimator of Cosmic-Ray Energy

Physical Review Letters

... Plastic scintillator (PS) detectors, invented in the early 1950s 1 , are widely used in the detection of elementary particles in high-energy physics 2-6 , nuclear physics 7 , astroparticle physics 8,9 , as well as in many applications like muon tomography 10 , proton computed tomography for hadron therapy 11 , fast-neutron detection 12,13 and non-destructive imaging 14 . By measuring the energy loss of a particle and tracking its path in the detector, it is possible to identify the type of interacting particle, reconstruct its momentum based on range, measure its original energy using calorimetry, and determine its electric charge if the setup is immersed in a magnetic field. ...

The Pierre Auger Observatory Upgrade - Preliminary Design Report

... Fig. 16 shows two such examples, the measurements of the atmospheric depth ( max ) at which the production of muons reaches its maximum [172] and muon density [174]/muon number [43] at ground (Auger UMD and SD (inclined events)) (see Section 3 for more detailed discussion of the 'Muon Puzzle'). For Auger SD [173,193,207] and TA SD measurements [204] where a comparison of the EM and muon signals is used, the observed discrepancy with the FD data is smaller. ...

Azimuthal asymmetry in the risetime of the surface detector signals of the Pierre Auger Observatory
  • Citing Article
  • April 2016

Physical Review D

... In the configuration used in this work, eleven stations of the SD-433 array are co-located with stations of the Underground Muon Detector (UMD), as illustrated in figure 1, left. Each UMD station consists of three modules, each containing 64 plastic scintillator bars measuring 400 cm in length, 4 cm in width and 1 cm in thickness providing a sensitive area of ∼10 m 2 [42,43]. The central station on the array's western edge contains six modules, providing a sensitive area of ∼50 m 2 , compared to the standard 30 m 2 area in all other stations. ...

Prototype muon detectors for the AMIGA component of the Pierre Auger Observatory
  • Citing Article
  • May 2016

Journal of Instrumentation

... The potentially interesting result with astrophysical neutrino candidates first reported in Refs. [217,218], was not confirmed with more statistics [219][220][221]. ...

Search for correlations between the arrival directions of IceCube neutrino events and ultrahigh-energy cosmic rays detected by the Pierre Auger Observatory and the Telescope Array
  • Citing Article
  • January 2016

... LOPES also pioneered many methods regarding the radio technique which have been used by other experiments, such as LOFAR, AERA, and Tunka-Rex. Examples are the continuous monitoring of the atmospheric electric field and the calibration methods used by LOPES, in particular the monitoring of the relative timing with 20 a beacon [69,70] and the end-to-end amplitude calibration using an absolutely calibrated external reference source [71,72,73]. The latter also enabled the comparison of the absolute energy scales of different air-shower arrays using radio measurements [74]. ...

Nanosecond-level time synchronization of autonomous radio detector stations for extensive air showers

... The detector is capped by a surface detector, aimed at cosmic ray physics, called IceTop. along their journey from source to detection (e.g., Aartsen et al., 2015). Thus their arrival directions at Earth cannot be easily traced to their origins, making the identification of the sources of high-energy cosmic rays one of the biggest challenges in astroparticle physics. ...

Search for correlations between the arrival directions of IceCube neutrino events and ultrahigh-energy cosmic rays detected by the Pierre Auger Observatory and the Telescope Array