KINETIC CORRELATION IN NON-EQUILIBRIUM FERMION–BOSON GAS

2013 ◽  
Vol 12 (04) ◽  
pp. 1350023 ◽  
Author(s):  
M. RAMONAS ◽  
R. KATILIUS ◽  
A. MATULIONIS ◽  
S. V. GANTSEVICH
Keyword(s):  
Electric Field ◽  
Strong Electric Field ◽  
Kinetic Equations ◽  
Hot Electrons ◽  
Classical Approach ◽  
Mathematical Apparatus ◽  
Quantitative Investigation ◽  
Particle Correlation ◽  
Hot Phonons ◽  
Non Equilibrium

We present a theoretic treatment of particle–particle correlation in a non-equilibrium fermion–boson gas subjected to strong electric field. The detailed description is based on an example of hot electrons and hot phonons in a solid under quasi-classical approach in terms of Boltzmann-like kinetic equations. We develop the mathematical apparatus, based on diagrammatic approach, for quantitative investigation of the flows of correlated particles. Non-trivial terms are resolved, and the correlations crucial for electric fluctuations are discussed.

Stimulated and spontaneous far infra-red emission from uniaxially strained gapless Hg1−xCdxTe

2010 ◽  
Vol 18 (3) ◽  
Author(s):  
S.G. Gasan-Zade ◽  
M.V. Strikha ◽  
G.A. Shepelskii
Keyword(s):  
Electric Field ◽  
Impact Ionization ◽  
Strong Electric Field ◽  
Radiative Transition ◽  
Hot Electrons ◽  
Acceptor Level ◽  
Threshold Values ◽  
Red Emission ◽  
V Band ◽  
Infra Red

AbstractThe intensive far infra-red irradiation in the range of 80–100 μm was observed in uniaxially strained gapless p-Hg1−xCdxTe (MCT) with x = 0.14 in the strong electric field. The inverse occupation in strained MCT is created because the hot electrons distribution occurs in the c-band under impact ionization, while the holes are localized near the v-band top. The probability of band-to-band radiative transition increases dramatically when the acceptor level becomes resonance in the v-band. At threshold values of strain and electric field (P = 2.5–2.7 kbar, E = 50–55 V/cm), increase in irradiation (by 3 orders of magnitude) and increase in current (by 4–6 times) occur.

Ozone Gas Generator Using Uniaxially Polarized LiTaO3 Single Crystal

2007 ◽  
Vol 1034 ◽  
Author(s):  
Nakanishi Yoshikazu ◽  
Junko Ide ◽  
Jun Kondo ◽  
Shinji Fukao ◽  
Katsumi Handa ◽  
...  
Keyword(s):  
Electric Field ◽  
Single Crystal ◽  
Temperature Change ◽  
Atmospheric Pressure ◽  
Gas Flow ◽  
Strong Electric Field ◽  
Ozone Production ◽  
Maximum Temperature ◽  
Gas Generator ◽  
Non Equilibrium

AbstractThe phenomenon that a ferroelectrics crystal carries out intrinsic polarization by the temperature change generally is known. The Ozone gas generation was investigated due to a strong electric field of this crystal under atmospheric pressure . When we added a rapid temperature change to the crystal, the charge non–equilibrium occurs around the crystal. Oxygen is influenced due to the non-equilibrium in charge and ozone is considered to be generated. Therefore, we used the high electric field induced due to the polarization of a ferroelectrics crystal in order to produce the ozone under atmospheric pressure.As a result, we were able to produce ozone of the density of 400ppb in a oxygen gas flow of 1.5 liters per minute using this simple system: The crystals (Yamaju Co. Ltd. and Sumitomo metal mining Co. Ltd.) are used in thickness of 3, 5, 7, 10, 20, and 30 mm with a diameter of 4 inches, respectively. They are poled crystals.Experiments on the maximum temperature (300 degree), the temperature gradient (100 degree/10 minite), and substrate materials(Cu and Al), the thickness of the crystal, and z face etc. were carried out during the temperature of LiTaO3 single crystal from 20C to about 300C. It is found that the amount of the ozone production increases rapidly, when the maximum temperature of LiTaO3 single crystal is raised and have a relation with the thickness of the crystal. However, the amount of the ozone production doesn't closely related with the X-ray generation that we use the crystal for.In the present study, when the thickness of the crystal became large, polarization voltage became high, but generated efficiency of ozone was not necessarily proportional to thickness.

scholarly journals Closed system of equations for description of the e+e– γ plasma generated from vacuum by strong electric field

2019 ◽  
Vol 204 ◽  
pp. 06010
Author(s):  
S.A. Smolyansky ◽  
A.M. Fedotov ◽  
A.D. Panferov ◽  
S.O. Pirogov
Keyword(s):  
Electric Field ◽  
Laser Field ◽  
Strong Electric Field ◽  
Kinetic Equations ◽  
Laser Pulses ◽  
Field Approximation ◽  
Constant Field ◽  
Internal Electric Field ◽  
Kinetic Description ◽  
Quantum Radiation

We develop a self-consistent kinetic description of a e+e– γ plasma, generated from vacuum in a focal spot of counterpropagating laser pulses. Our model assumes purely time-dependent external (laser) field, but properly takes into account the semiclassical internal (plasma) field, as well as quantum radiation. While nonperturbative kinetic description of e+e–-pair production from vacuum and the simplest variant of backreaction problem have been previously addressed, quantum radiation is included in such a model for the first time. To achieve this goal we derived coupled kinetic equations for the electron, positron, and photon plasma species and the Maxwell equation for the internal electric field. Photon subsystem is included systematically using the BBGKY chain, which we truncate at the second order of perturbation theory by taking into account the annihilation and radiation channels. An important application of our results would be consideration of laser field depletion due to cascade production beyond the locally constant field approximation.

scholarly journals Axion assisted Schwinger effect

2021 ◽  
Vol 2021 (5) ◽  
Author(s):  
Valerie Domcke ◽  
Yohei Ema ◽  
Kyohei Mukaida
Keyword(s):  
Electric Field ◽  
Production Rate ◽  
Strong Electric Field ◽  
Background Field ◽  
Chiral Anomaly ◽  
Fermion Mass ◽  
Anomaly Equation ◽  
Electric And Magnetic Fields ◽  
Schwinger Effect ◽  
Momentum Transverse

Abstract We point out an enhancement of the pair production rate of charged fermions in a strong electric field in the presence of time dependent classical axion-like background field, which we call axion assisted Schwinger effect. While the standard Schwinger production rate is proportional to $$ \exp \left(-\pi \left({m}^2+{p}_T^2\right)/E\right) $$ exp − π m 2 + p T 2 / E , with m and pT denoting the fermion mass and its momentum transverse to the electric field E, the axion assisted Schwinger effect can be enhanced at large momenta to exp(−πm2/E). The origin of this enhancement is a coupling between the fermion spin and its momentum, induced by the axion velocity. As a non-trivial validation of our result, we show its invariance under field redefinitions associated with a chiral rotation and successfully reproduce the chiral anomaly equation in the presence of helical electric and magnetic fields. We comment on implications of this result for axion cosmology, focussing on axion inflation and axion dark matter detection.

Observation of the Avalanche of Runaway Electrons in Air in a Strong Electric Field

2012 ◽  
Vol 109 (8) ◽  
Author(s):  
A. V. Gurevich ◽  
G. A. Mesyats ◽  
K. P. Zybin ◽  
M. I. Yalandin ◽  
A. G. Reutova ◽  
...  
Keyword(s):  
Electric Field ◽  
Strong Electric Field ◽  
Runaway Electrons

Electric-Field Induced Formation of Superconducting Granular Balls

2002 ◽  
Vol 16 (17n18) ◽  
pp. 2529-2535
Author(s):  
R. Tao ◽  
X. Xu ◽  
Y. C. Lan
Keyword(s):  
Surface Energy ◽  
Electric Field ◽  
Liquid Nitrogen ◽  
Applied Electric Field ◽  
Strong Electric Field ◽  
Particle Surface ◽  
Cooper Pairs ◽  
Surface Charges

When a strong electric field is applied to a suspension of micron-sized high T c superconducting particles in liquid nitrogen, the particles quickly aggregate together to form millimeter-size balls. The balls are sturdy, surviving constant heavy collisions with the electrodes, while they hold over 106 particles each. The phenomenon is a result of interaction between Cooper pairs and the strong electric field. The strong electric field induces surface charges on the particle surface. When the applied electric field is strong enough, Cooper pairs near the surface are depleted, leading to a positive surface energy. The minimization of this surface energy leads to the aggregation of particles to form balls.

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