Abstract:For the first time the emission of neutron bursts in the process of high-voltage discharge in air was observed. Experiments were carried out at an average electric field strength of ∼1 MV·m(-1) and discharge current of ∼10 kA. Two independent methods (CR-39 track detectors and plastic scintillation detectors) registered neutrons within the range from thermal energies up to energies above 10 MeV and with an average flux density of ≳10(6) cm(-2) per shot inside the discharge zone. Neutron generation occurs at… Show more
“…Some impressive hints on neutron production in high-voltage atmospheric discharges are reported in a recent paper [1]. From the theoretical point of view, there is an open debate on whether inverse-β nuclear transmutations could justify such observations [2][3][4][5][6][7].…”
Section: Introductionmentioning
confidence: 99%
“…[1] in plasma discharges of an electrolytic cell that are claimed in the experiment [8] and in patents [9] to produce neutrons. With respect to the existing claims, we perform here a rigorous scrutiny of the detectors and the possible backgrounds to the measurement using a similar experimental setup.…”
Following some recent unexpected hints of neutron production in high-voltage atmospheric discharges, we present a measurement of the neutron flux in plasma discharges in electrolytic cells. We use two different types of neutron detectors, polyallyl diglycol carbonate (PADC, aka CR-39) tracers and indium disks. At 95 % C.L. we provide an upper limit of 1.5 neutrons cm −2 s −1 for the thermal neutron flux at ≈5 cm from the center of the cell. Allowing for a higher energy neutron component, the largest allowed flux is 64 neutrons cm −2 s −1 . This upper limit is two orders of magnitude smaller than the signal previously claimed in an electrolytic cell plasma discharge experiment. Furthermore the behavior of the CR-39 is discussed to point out possible sources of spurious signals.
“…Some impressive hints on neutron production in high-voltage atmospheric discharges are reported in a recent paper [1]. From the theoretical point of view, there is an open debate on whether inverse-β nuclear transmutations could justify such observations [2][3][4][5][6][7].…”
Section: Introductionmentioning
confidence: 99%
“…[1] in plasma discharges of an electrolytic cell that are claimed in the experiment [8] and in patents [9] to produce neutrons. With respect to the existing claims, we perform here a rigorous scrutiny of the detectors and the possible backgrounds to the measurement using a similar experimental setup.…”
Following some recent unexpected hints of neutron production in high-voltage atmospheric discharges, we present a measurement of the neutron flux in plasma discharges in electrolytic cells. We use two different types of neutron detectors, polyallyl diglycol carbonate (PADC, aka CR-39) tracers and indium disks. At 95 % C.L. we provide an upper limit of 1.5 neutrons cm −2 s −1 for the thermal neutron flux at ≈5 cm from the center of the cell. Allowing for a higher energy neutron component, the largest allowed flux is 64 neutrons cm −2 s −1 . This upper limit is two orders of magnitude smaller than the signal previously claimed in an electrolytic cell plasma discharge experiment. Furthermore the behavior of the CR-39 is discussed to point out possible sources of spurious signals.
“…The main characteristics of generated discharge and procedure of electrophysical diagnostics were the same as in the measurements described in [10]. High voltage pulses with a ∼1 MV amplitude were applied to a discharge air gap of the 450-750 mm width (the latter was changed in various runs).…”
Section: Experimental Setup Detector Calibration and The Time Smentioning
confidence: 99%
“…In a previous paper [10] we noted that the momentum of the neutron radiation, the detected scintillation detector placed behind a lead shield, is correlated with the occurrence of x-ray pulse and is located within it. That is, the neutron pulse was observed in the initial "dark" phase of the discharge until closure of cathode and anode streamers.…”
Section: The Real-time Neutron and X-ray Measurementsmentioning
confidence: 99%
“…Recently we reported our first measurements of neutron emission originated by atmospheric lightning like discharge in a laboratory installation [10]. Experiments were carried out inside an electric field with the average strength of the order of ∼1 MV·m −1 and with neutron detectors of two independent kinds: the CR-39 type tracers and the plastic scintillators.…”
The new results concerning neutron emission detection from a laboratory high-voltage discharge in the air are presented. Data were obtained with a combination of plastic scintillation detectors and 3 He filled counters of thermal neutrons. Strong dependence of the hard x-ray and neutron radiation appearance on the field strength near electrodes, which is determined by their form, was found. We have revealed a more sophisticated temporal structure of the neutron bursts observed during of electric discharge. This may indicate different mechanisms for generating penetrating radiation at the time formation and development of the atmospheric discharge.
Positron beams have been observed by the Fermi satellite to be correlated with lightning leaders, and neutron emissions have been attributed to lightning and to laboratory sparks as well. Here we discuss the cross sections to be used for modeling these emissions, and we calculate the emissions of positrons, neutrons, and also protons from lightning leaders. Neutrons were first erroneously attributed to fusion reactions, but the photonuclear reaction responsible for neutrons should create protons as well. We predict them here; they have not been observed yet. In the paper, we first revisit the model for stepped lightning leaders of Xu, Celestin, and Pasko with updated cross sections, we analyze the spatial and energetic structure of the electron beam, and we calculate the spectrum of the generated gamma ray beam at 16 km altitude. Then we review the scattering processes of photons with emphasis on the processes above 5 MeV, in particular the photon energy losses in Compton scattering events and the generation of leptons and hadrons. We provide simple approximations for photon energy loss and lepton and hadron production for any photon with energy above 5 MeV passing through an arbitrary air layer. Finally, we launch a gamma ray beam with the earlier calculated spectrum of the negative stepped lightning leader from 16 km upward and calculate the production and energy of positrons, neutrons, and protons as well as the propagation of positrons.
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