“…For neutron and gamma-quantum separation Pulse Shape Discrimination was used. More detailed instrument description for the orbital complex and the CORONAS-I satellite is given by Bogomolov et al (1998) and for the MIR station-by Bogomolov et al (2002). As it can be seen from the figure, the spectrum calculated for the SPEKTR module of the MIR orbital station agrees with the spectrum as measured on the orbital complex, whereas the neutron fluxes as reconstructed from the data of the measurements taken on the MIR station are substantially higher.…”
Section: Spectra Of Secondary Neutron Fluxesmentioning
“…For neutron and gamma-quantum separation Pulse Shape Discrimination was used. More detailed instrument description for the orbital complex and the CORONAS-I satellite is given by Bogomolov et al (1998) and for the MIR station-by Bogomolov et al (2002). As it can be seen from the figure, the spectrum calculated for the SPEKTR module of the MIR orbital station agrees with the spectrum as measured on the orbital complex, whereas the neutron fluxes as reconstructed from the data of the measurements taken on the MIR station are substantially higher.…”
Section: Spectra Of Secondary Neutron Fluxesmentioning
“…It can be explained by the energy spectrum of intrinsic background being extremely hard, (see, for ex. [66]) in presentation E J it can even grow with energy. Of course, the intrinsic background depends strongly on the spacecraft mass, which should be as low as possible, but such energy dependence of the intrinsic background intensity is valid for satellites.…”
The non-linear electrodynamics influence of pulsar magnetic field on the electromagnetic pulse polarization is discussed from the point of observation interpretation. The calculations of pulsar magnetic field impact on electromagnetic pulse polarization are made in such a way to make it easier to interpret these effects in space experiments. The law of hard emission pulse propagation in the pulsar magnetic field according to the vacuum nonlinear electrodynamics is obtained. It was shown, that due to the birefringence in the vacuum the front part of any hard emission pulse coming from a pulsar should be linearly polarized and the rest of pulse can have arbitrary polarization. Observational possibilities of vacuum birefringence are discussed. The estimations of detector parameters such as effective area, exposure time and necessity of polarization measurements with high accuracy are given. The combination of large area and extremely long exposure time gives the good opportunity to search the fine polarization effects like vacuum non-linear electrodynamics birefringence.
“…These particles can be recognized on the basis of their pulse shapes. In a number of space-based instruments that detected neutrons by nuclear reactions in CsI (e.g., the SONG [11,13] and NEGA-1 [14]), neutrons were identified using the dependence of the pulse shape in CsI on the average ionization [15]. (The secondary products of neutron interactions have a higher ionization.)…”
Section: Description Of the Instrumentmentioning
confidence: 99%
“…The multichannel analyzers and digital electronic units, all of which were similar to those required for our instrument, had already been employed in space-based equipment [8,10,11,13,14].…”
Section: Electronic Components Of the Detectormentioning
The InterSONG instrument now being developed at the Skobel'tsyn Institute of Nuclear Physics will allow the sensitivity of experiments on solar neutrons to be significantly raised by performing measurements in the immediate neighborhood of the Sun. It is expected that this instrument will be used on the Inter-HELIOS automatic interplanetary station operating at distances of as many as 25 solar radii. The instrument is based on a LiI scintillating crystal enriched with 6 Li, and a boron-containing plastic scintillator that also acts as a fast neutron moderator. The instrument is designed to detect neutrons with energies of 0.1-100 MeV and electromagnetic radiation over the range 0.03-10 MeV.
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