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1.
Summary EAS-TOP is a detector of the extensive air showers that very high-energy cosmic rays ( E
0≥10 14eV) produce in the atmosphere. The array is located on top of the underground Gran Sasso Laboratory in central Italy; a subarray
(11 modules of the e.m. detector) has been operating since the end of 1987. From such data the stability of the detector,
and the accuracies in the determination of the arrival directions and in the reconstruction of the electron lateral distribution
and of the shower size are derived. The results obtained on VHE-UHE γ-ray sources in the first months of operation are presented.
To speed up publication, the proofs were not sent to the authors and were supervised by the Scientific Committee. 相似文献
2.
Gamma ray bursts (GRBs) have been proposed as one possible class of sources of the ultrahigh energy cosmic ray (UHECR) events
observed up to energies ≳ 10 20 eV. The synchrotron radiation of the highest energy protons accelerated within the GRB source should produce gamma rays up
to TeV energies. Here we briefly discuss the implications on the energetics of the GRB from the point of view of the detectability
of the prompt TeV γ-rays of proton-synchrotron origin in GRBs in the up-coming ICECUBE muon detector in the south pole. 相似文献
3.
Possible extragalactic sources of cosmic rays with energies above 4 × 10 19 eV detected at the Yakutsk EAS array are sought. The correlation of the shower arrival directions with objects from Véron’s catalog that are located closer than 100 Mpc from the Earth confirms the observations at the Pierre Auger Observatory, as well as the Greisen-Zatsepin-Kuzmin effect on the spectrum of cosmic rays. The detailed analysis of the data reveals the classes of objects belonging to the active galactic nuclei that are the most probable sources of ultrahigh-energy cosmic rays. 相似文献
4.
The Large High Altitude Air Shower Observatory(LHAASO) is a composite cosmic ray observatory consisting of three detector arrays: kilometer square array(KM2 A), which includes the electromagnetic detector array and muon detector array, water Cherenkov detector array(WCDA) and wide field-of-view Cherenkov telescope array(WFCTA). One of the main scientific objectives of LHAASO is to precisely measure the cosmic rays energy spectrum of individual components from 10~(14) eV to 10~(18) eV. The hybrid observation will be employed by the LHAASO experiment, in which the lateral and longitudinal distributions of extensive air shower can be observed simultaneously. Thus, many kinds of parameters can be used for primary nuclei identification. In this paper, high purity cosmic ray simulation samples of the light nuclei component are obtained using multi-variable analysis. The apertures of 1/4 LHAASO array for pure proton and mixed proton and helium(HHe) samples are 900 m~2 Sr and1800 m~2 Sr, respectively. Prospect of obtaining proton and HHe spectra from 100 TeV to 4 PeV is discussed. 相似文献
5.
A method is proposed for measuring extragalactic magnetic fields in observations of TeV γ rays from distant sources. Multi-TeV
γ rays from these sources interact with the infrared photon background producing secondary electrons and positrons, which
can be just slightly deflected by extragalactic magnetic fields before they emit secondary γ rays via inverse Compton scattering
of cosmic microwave background photons. Secondary γ rays emitted toward an observer on the Earth can be detected as an extended
emission around an initially point source. The energy dependent angular profile of the extended emission is related to the
strength of the extragalactic magnetic field along the line of sight. Small magnetic fields B ≤ 10 −12 G in the voids of the large scale structure can be measured in this way.
The text was submitted by the authors in English 相似文献
6.
We present a method for determining the energy of the primary particle that generates an extensive air shower (EAS) of comic rays based on measuring the total flux of Cherenkov light from the shower. Applying this method to Cherenkov light measurements at the Yakutsk EAS array has allowed us to construct the cosmic ray energy spectrum in the range 10 15 ? 3 × 10 19 eV. 相似文献
7.
This paper analyses the possibility of separating distinct groups of nuclei of primary cosmic rays with energies of 10 15–10 16 eV from the data on the spatial-angular distribution of Cherenkov light in extensive air showers. The paper shows that using
an array of a few (3–4) telescopes with a moderately sized angular cell ∼0.5° placed at a distance ∼100 m from one another,
one can achieve almost complete separation of the showers initiated by these nuclei (the Bayesian classification error is
a few percentage points for the case of separating primary protons and nitrogen nuclei). The authors propose new parameters
of the angular Cherenkov image that can greatly enhance the separability of the shower classes as compared to the approach
based on the traditional parameters. 相似文献
8.
The complicated shape of the cosmic ray spectrum recorded by giant arrays in the energy range 10 17–10 20 eV is analyzed. It is shown that in the energy region ∼10 18–10 19 eV the spectrum probably coincides with the injection spectrum whose exponent is equal approximately to 3.2–3.3. The flatter
component in the energy region (3.2–5.0)×10 19 eV is due to braking of extragalactic protons on primordial photons (the cosmic background radiation). At energies exceeding
3.2×10 19 eV the spectrum does not have a blackbody cutoff. The possibility of determining the distances at which cosmic rays originate
and investigating the evolution of their sources on the basis of ultrahigh-energy cosmic ray data is discussed.
Zh. éksp. Teor. Fiz. 113, 12–20 (January 1998) 相似文献
9.
The extensive air shower (EAS) muon number spectrum is obtained with increased statistics using the central muon detector
of the EAS MSU array, which records muons with energies above 10 GeV. The dependence of the mass composition of primary cosmic
rays on the energy is considered. The conclusion is confirmed that for energies from 3 × 10 15 eV (the primary energy spectrum knee) up to 10 17 eV a change in the composition associated with an increase in the proportion of heavy nuclei occurs; however, after the energy
of 10 17 eV, the proportion of heavy nuclei begins to decrease and the composition becomes lighter. A comparison with similar data
from other experiments is conducted. The existence of an additional component of cosmic rays is confirmed; earlier an indication
of its presence was derived from data on the EAS electron number spectrum. 相似文献
11.
Data on muon and electron components of extensive air showers (EAS) (obtained with the EAS MSU array) were used to derive
the primary cosmic ray (PCR) mass composition. It is shown that for energies beyond the knee at energy 3 × 10 15 eV the abundance of heavy nuclei increases with energy. But at energies above 10 17 eV the abundance of light nuclei starts to grow. The primary cosmic ray spectrum in the range 10 15–10 18 eV is analyzed. It is shown that at energies above 10 17 eV the additional component appears and it differs from the bulk of Galactic cosmic rays generated by shocks in SN remnants. 相似文献
12.
Summary The EAS-TOP Extensive Air Shower array, on top of the under-ground Gran Sasso Laboratory, is fully operating as a γ-ray astronomy
observatory since the beginning of 1989. After showing the measured angular resolution of the detector, we present the results
obtained from the analysis of 280 days of measurements in 1989–1990, with the purpose of investigating possible emission (d.c.
and sporadic) from the candidate sources in the Northern hemisphere at an energy, >200 TeV.
Paper presented at the V Cosmic Physics National Conference, S. Miniato, November 27–30, 1990. 相似文献
13.
A hybrid method for detecting cosmic rays and neutrino cascades using the radio method and the conventional method for detecting cascade particles was proposed. Cascades produced in the lunar soil near the surface by ultrahigh-energy cosmic rays and neutrinos in the energy range of 1 GeV–100 TeV, coming from above at different angles, were calculated. The calculated energy and angular distributions were extrapolated to the energy region of 10 20 eV. Using these results, the detection threshold was estimated as 10 20 eV which is approximately identical to the threshold for the radio detector previously considered by the authors. 相似文献
14.
The state of the art and the project of modernization of the extensive-air-shower array Carpet-2 of the Baksan Neutrino Observatory of the Institute for Nuclear Research, Russian Academy of Sciences are described. The modernized array will allow the performance of detailed study of variations in the cosmic ray intensity, the energy spectra and composition of primary cosmic rays in the energy range 10 13–10 16 eV, and the anisotropy of primary cosmic rays with energies above 10 13 eV. 相似文献
15.
Using data from inclined events ( 60 degrees 相似文献
16.
We calculate the flux of “GZK photons,” namely, the flux of ultra-high-energy cosmic rays (UHECRs) consisting of photons produced
by extragalactic nucleons through the resonant photoproduction of pions, the so-called GZK effect. We show that for primary
nucleons, the GZK-photon fraction of the total UHECR flux is between 10 −4 and 10 –2 above 10 19 eV and up to the order of 0.1 above 10 20 eV. The GZK-photon flux depends on the assumed UHECR spectrum, the slope of the nucleon flux at the source, and the distribution
of sources and intervening backgrounds. Detection of this photon flux would open the way for UHECR gamma-ray astronomy. Detection
of a larger photon flux would imply the emission of photons at the source or new physics. We compare the photon fractions
expected for GZK photons and the minimal fractions predicted by top-down models. We find that the photon fraction above 10 19 eV is a crucial test for top-down models.
The text was submitted by the authors in English. 相似文献
17.
An experiment for measuring the flux of cosmic diffuse gamma rays with energies above 100 TeV (the Carpet-3 air shower array) is now being prepared at the Baksan Neutrino Observatory, Institute for Nuclear Research, Russian Academy of Sciences. The preparations entail a substantial increase of the areas of both the muon detector and the surface air shower array. The experiment’s sensitivity to showers generated by primary gamma rays is estimated for different configurations of the array. In addition, preliminary estimates of the upper limit on the flux of diffuse gamma rays with energies higher than 1.3 PeV, derived using experimental data from the old Carpet-2 array, are presented for a net exposure time of 9.2 years. 相似文献
18.
The lateral distribution of muons in extensive air showers with energies above 1017 eV detected by underground scintillation detectors with a threshold of 1.0 GeV at the Yakutsk array in 1986–2016 has been analyzed. The experimental data on the muon flux density at a distance of 300 m from the shower axis have been compared to the calculations within various models of hadron interactions at ultrahigh energies. The experimental data are in the best agreement with the QGSJet01 and QGSJet II-04 models. The mass composition of cosmic rays in the energy range of (1–30) × 1017 eV changes from middle nuclei to a purely proton composition. 相似文献
19.
The probability of high-energy γ-ray emission accompanying the spontaneous fission of 252Cf nuclei in the energy range of 5–60 MeV was measured experimentally. The γ rays were detected by a BGO detector with a size
of ∅7.6 × 7.6 cm in coincidence with neutrons detected by an organic polystyrene-based scintillator with a size of ∅6.0 ×
2.0 cm. To reject events associated with the cosmic background, we propose an original method that combines rapid digitizing
of the pulse shape and the time-of-flight method. 相似文献
20.
The space-based GAMMA-400 gamma-ray telescope will measure the fluxes of gamma rays in the energy range from ∼20 MeV to several TeV and cosmic-ray electrons and positrons in the energy range from several GeV to several TeV to investigate the origin of gamma-ray sources, sources and propagation of the Galactic cosmic rays and signatures of dark matter. The instrument consists of an anticoincidence system, a converter-tracker (thickness one radiation length, 1 X0), a time-of-flight system, an imaging calorimeter (2 X0) with tracker, a top shower scintillator detector, an electromagnetic calorimeter from CsI(Tl) crystals (16 X0) with four lateral scintillation detectors and a bottom shower scintillator detector. In this paper, the capability of the GAMMA-400 gamma-ray telescope for electron and positron measurements is analyzed. The bulk of cosmic rays are protons, whereas the contribution of the leptonic component to the total flux is ∼10−3 at high energy. The special methods for Monte Carlo simulations are proposed to distinguish electrons and positrons from proton background in the GAMMA-400 gamma-ray telescope. The contribution to the proton rejection from each detector system of the instrument is studied separately. The use of the combined information from all detectors allows us to reach a proton rejection of up to ∼1 × 104. 相似文献
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