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Energy calibration of Calorimetric Electron Telescope (CALET) in space

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Abstract

The Calorimetric Electron Telescope (CALET) is a space experiment, currently under development by Japan in collaboration with Italy and the United States. CALET will measure the flux of cosmic ray electrons (including positrons) up to 20 TeV, gamma-rays up to 10 TeV and nuclei from Z = 1 up to 40 up to 1000 TeV during a two-year mission on the International Space Station (ISS), extendable to five years. The unique feature of CALET is its thick, fully active calorimeter that allows measurements well into the TeV energy region with excellent energy resolution ( ), coupled with a fine imaging upper calorimeter to accurately identify the starting point of electromagnetic showers. For continuous high performance of the detector, it is required to calibrate each detector component on orbit. We use the measured response to minimum ionizing particles for the energy calibration, taking data in a dedicated trigger mode and selecting useful events in off-line analysis. In this paper, we present on-orbit and off-line data handling methods for the energy calibration developed through beam tests at CERN-SPS and Monte Carlo simulations.

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... Employing dual shaping amplifiers with two different gains for each APD (PMT) and PD, increases the dynamical range to 10 6 (10 4 ). As a consequence, the TASC can measure the energy of the incident electrons and gamma rays with a resolution < 2% above 100 GeV [11] . Another important role of the TASC is to efficiently identify high-energy electrons among the overwhelming background of cosmic-ray protons. ...
... Their energy spectrum depends on the cutoff rigidity, and hence the geomagnetic latitude. As a result, the position of the MIP peaks will shift by several percent as a function of the geomagnetic latitude [11] . To account for this effect, the incident particle energy distributions are assessed by simulating the energy spectra of incoming primary particles [11] using ATMNC3 [13] , in which AMS-01 proton and helium spectra [14] were used as input, since these data were taken at various geomagnetic latitudes, as well as them being in good agreement with BESS [15] and re- cent experiments. ...
... As a result, the position of the MIP peaks will shift by several percent as a function of the geomagnetic latitude [11] . To account for this effect, the incident particle energy distributions are assessed by simulating the energy spectra of incoming primary particles [11] using ATMNC3 [13] , in which AMS-01 proton and helium spectra [14] were used as input, since these data were taken at various geomagnetic latitudes, as well as them being in good agreement with BESS [15] and re- cent experiments. As well, contamination by interacting particles and/or scattered and stopped particles can cause a systematic shift in the determined position of MIP peaks. ...
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In August 2015, the CALorimetric Electron Telescope (CALET), designed for long exposure observations of high energy cosmic rays, docked with the International Space Station (ISS) and shortly thereafter began to collect data. CALET will measure the cosmic ray electron spectrum over the energy range of 1 GeV to 20 TeV with a very high resolution of 2% above 100 GeV, based on a dedicated instrument incorporating an exceptionally thick 30 radiation-length calorimeter with both total absorption and imaging (TASC and IMC) units. Each TASC readout channel must be carefully calibrated over the extremely wide dynamic range of CALET that spans six orders of magnitude in order to obtain a degree of calibration accuracy matching the resolution of energy measurements. These calibrations consist of calculating the conversion factors between ADC units and energy deposits, ensuring linearity over each gain range, and providing a seamless transition between neighboring gain ranges. This paper describes these calibration methods in detail, along with the resulting data and associated accuracies. The results presented in this paper show that a sufficient accuracy was achieved for the calibrations of each channel in order to obtain a suitable resolution over the entire dynamic range of the electron spectrum measurement.
... The on-orbit commissioning phase was successfully completed in the first days of October 2015. Calibration and test of the instrument took place at the CERN-SPS during five campaigns between 2010 and 2015 with beams of electrons, protons, and relativistic ions [40][41][42]. ...
... A dedicated trigger mode [42,43] allows the selection of penetrating protons and He particles for the individual onorbit calibration of all channels. First, raw data are corrected for gain differences among the channels, light output nonuniformity, and any residual dependence on time and temperature. ...
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The Calorimetric Electron Telescope (CALET), in operation on the International Space Station since 2015, collected a large sample of cosmic-ray iron over a wide energy interval. In this Letter a measurement of the iron spectrum is presented in the range of kinetic energy per nucleon from 10 GeV/n to 2.0 TeV/n allowing the inclusion of iron in the list of elements studied with unprecedented precision by space-borne instruments. The measurement is based on observations carried out from January 2016 to May 2020. The CALET instrument can identify individual nuclear species via a measurement of their electric charge with a dynamic range extending far beyond iron (up to atomic number Z=40). The energy is measured by a homogeneous calorimeter with a total equivalent thickness of 1.2 proton interaction lengths preceded by a thin (3 radiation lengths) imaging section providing tracking and energy sampling. The analysis of the data and the detailed assessment of systematic uncertainties are described and results are compared with the findings of previous experiments. The observed differential spectrum is consistent within the errors with previous experiments. In the region from 50 GeV/n to 2 TeV/n our present data are compatible with a single power law with spectral index −2.60±0.03.
... In order to assess the relatively large uncertainties in the hadronic interactions, a series of beam tests were carried out at CERN-SPS using the CALET beam test model [43][44][45]. Trigger efficiency and energy response derived from MC simulations were tuned using the beam test results obtained in 2012 [43,44,46] with proton beams of 30, 100, and 400 GeV. The correction for the trigger efficiency obtained by the EPICS simulation was determined to be 7.7% for the LE trigger and 11.2% for the HE trigger, irrespective of proton energies. ...
... In order to assess the relatively large uncertainties in the hadronic interactions, a series of beam tests were carried out at CERN-SPS using the CALET beam test model [43][44][45]. Trigger efficiency and energy response derived from MC simulations were tuned using the beam test results obtained in 2012 [43,44,46] with proton beams of 30, 100, and 400 GeV. The correction for the trigger efficiency obtained by the EPICS simulation was determined to be 7.7% for the LE trigger and 11.2% for the HE trigger, irrespective of proton energies. ...
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In this paper, we present the analysis and results of a direct measurement of the cosmic-ray proton spectrum with the CALET instrument onboard the International Space Station, including the detailed assessment of systematic uncertainties. The observation period used in this analysis is from October 13, 2015 to August 31, 2018 (1054 days). We have achieved the very wide energy range necessary to carry out measurements of the spectrum from 50 GeV to 10 TeV covering, for the first time in space, with a single instrument the whole energy interval previously investigated in most cases in separate subranges by magnetic spectrometers (BESS-TeV, PAMELA, and AMS-02) and calorimetric instruments (ATIC, CREAM, and NUCLEON). The observed spectrum is consistent with AMS-02 but extends to nearly an order of magnitude higher energy, showing a very smooth transition of the power-law spectral index from −2.81±0.03 (50–500 GeV) neglecting solar modulation effects (or −2.87±0.06 including solar modulation effects in the lower energy region) to −2.56±0.04 (1–10 TeV), thereby confirming the existence of spectral hardening and providing evidence of a deviation from a single power law by more than 3σ.
... The total thickness of the TASC is about 27 X 0 at normal incidence. In order to identify individual chemical elements in the cosmic-ray flux, a Charge Detector (CHD) is positioned at the top of the CALET instrument to provide a measurement of the electric charge [1,2,3]. Calibration and test of the instrument took place at CERN SPS during five campaigns in 2010, 2011, 2012, 2013 and 2015 with beams of electrons, protons and relativistic ions. ...
... Using the dedicated CHarge Detector (CHD) on top of the instrument, a charge resolution of 0.15 -0.3 charge units has been demonstrated [2,3]. Nevertheless, a redundant measurement of the charge of the incident particle is of great importance. ...
... The calibration of each channel of CHD, IMC and TASC is performed using penetrating protons and He particles, selected in-flight with a dedicated trigger mode (Asaoka et al., 2017;Niita et al., 2015). Raw data are corrected for gain differences among the channels, light output nonuniformity, and any residual dependence on time and temperature. ...
... Detailed Monte Carlo (MC) simulations have been performed, based on the EPICS simulation package [46,47]. In order to assess the relatively large uncertainties in the modeling of hadronic interactions, a series of beam tests were carried out at the CERN-SPS using the CALET beam test model [48][49][50]. Trigger efficiency and energy response derived from MC simulations were tuned using the beam test results obtained in 2015 with ion beams of 13, 19, and 150 GeV=n. For helium nuclei a shower energy correction of 10.4% (8%) at 13ð19Þ GeV=n was applied, while a 3.2% energy independent correction was applied at 150 GeV=n and above. ...
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We present the results of a direct measurement of the cosmic-ray helium spectrum with the CALET instrument in operation on the International Space Station since 2015. The observation period covered by this analysis spans from October 13, 2015, to April 30, 2022 (2392 days). The very wide dynamic range of CALET allowed for the collection of helium data over a large energy interval, from ∼40 GeV to ∼250 TeV, for the first time with a single instrument in low Earth orbit. The measured spectrum shows evidence of a deviation of the flux from a single power law by more than 8σ with a progressive spectral hardening from a few hundred GeV to a few tens of TeV. This result is consistent with the data reported by space instruments including PAMELA, AMS-02, and DAMPE and balloon instruments including CREAM. At higher energy we report the onset of a softening of the helium spectrum around 30 TeV (total kinetic energy). Though affected by large uncertainties in the highest energy bins, the observation of a flux reduction turns out to be consistent with the most recent results of DAMPE. A double broken power law is found to fit simultaneously both spectral features: the hardening (at lower energy) and the softening (at higher energy). A measurement of the proton to helium flux ratio in the energy range from 60 GeV/n to about 60 TeV/n is also presented, using the CALET proton flux recently updated with higher statistics.
... Many space-borne experiments, such as AMS-02 [1], PAMELA [2], CALET [3], Fermi-LAT [4], measured galactic CR fluxes which are important in understanding their origin and propagation mechanisms. DAMPE is a satellite-based general-purpose high energy particle detector. ...
... Raw data are corrected for nonuniformity in light output, time and temperature dependence, and gain differences among the channels. The latter are individually calibrated on orbit by using penetrating proton and He particles, selected by a dedicated trigger mode [34,35]. After calibrations, each CR particle track is reconstructed and a charge and an energy are assigned for each event. ...
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In this paper, we present the measurement of the energy spectra of carbon and oxygen in cosmic rays based on observations with the Calorimetric Electron Telescope on the International Space Station from October 2015 to October 2019. Analysis, including the detailed assessment of systematic uncertainties, and results are reported. The energy spectra are measured in kinetic energy per nucleon from 10 GeV/n to 2.2 TeV/n with an all-calorimetric instrument with a total thickness corresponding to 1.3 nuclear interaction length. The observed carbon and oxygen fluxes show a spectral index change of ∼0.15 around 200 GeV/n established with a significance >3σ. They have the same energy dependence with a constant C/O flux ratio 0.911±0.006 above 25 GeV/n. The spectral hardening is consistent with that measured by AMS-02, but the absolute normalization of the flux is about 27% lower, though in agreement with observations from previous experiments including the PAMELA spectrometer and the calorimetric balloon-borne experiment CREAM.
... HERE are some space-borne experiments (AMS [1], Fermi-LAT [2], PAMELA [3], CALET [4]) to search for evidence of dark matter by measuring the spectra of photons, electrons and positrons. Exciting results from the successful operation of these experiments have been published [5][6][7][8]. ...
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The DArk Matter Particle Explorer (DAMPE) developed in China was designed to search for evidence of dark matter particles by observing primary cosmic rays and gamma rays in the energy range from 5 GeV to 10 TeV. Since its launch in December 2015, a large quantity of data has been recorded. With the data set acquired during more than a year of operation in space, a precise time-dependent calibration for the energy measured by the BGO ECAL has been developed. In this report, the instrumentation and development of the BGO Electromagnetic Calorimeter (BGO ECAL) are briefly described. The calibration on orbit, including that of the pedestal, attenuation length, minimum ionizing particle peak, and dynode ratio, is discussed, and additional details about the calibration methods and performance in space are presented.
... The reduced accuracy with which the energy deposit can be determined below 10 GeV is due to pedestal noise. As reported in detail in Ref. [4], the requirements for the calibration error of each TASC log can be relaxed by a factor of ∼3 compared to that for the energy resolution, as long as these individual errors of in total ∼6% are randomly distributed. This is due to the fact that, on average, ∼10 TASC logs contribute significantly to an event's energy measurement. ...
... Yosui Akaike event rate. Details are described in the reference [12], so we present here just an outline. ...
... Combining these components as well as the trigger system, data acquisition system and support sensors described in the following sections, the CALET detector features (1) a proton rejection factor of more than 10 5 , (2) a 2% energy resolution above 30 GeV, (3) an angular resolution of 0.1 to 0.5 • , and (4) a large geometrical factor on the order of 0.1 m 2 sr. The basic features of detector performance were investigated using Monte Carlo (MC) simulations [7], and verified by the beam tests at CERN-SPS [8][9][10]. The sufficiently high rejection capability of protons enables the suppression of systematic errors in the electron spectrum due to uncertainties in proton rejection factor calculation due to pos-sible interaction model dependence. ...
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... Detailed calibration achieved a fine energy resolution of 2% or better in the energy region from 20 GeV to 20 TeV (<3% for 10-20 GeV). The validity of our simulation has been checked with beam test data [23][24][25]. Regarding temporal variations occurring during long-term observations, each detector component is calibrated by modeling variations of the minimum ionizing particles (MIP) peak obtained from noninteracting particles (protons or helium) recorded with a dedicated trigger mode. ...
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