Blue and green jets in laboratory discharges initiated by runaway electrons |
2819 |
3091 |
291 |
Gas lasers pumped by runaway electrons preionized diffuse discharge |
1224 |
1224 |
4 |
Studying the thermodynamic processes in excilamps by the pressure jump method (review) |
1008 |
1013 |
8 |
Excilamps and their applications |
1719 |
2066 |
370 |
Apokamp discharge as a source of nitrogen oxcides |
792 |
1049 |
284 |
Excitonic states in diamond in the spectra of optical absorption and luminescence |
996 |
1219 |
259 |
Theoretical simulation of the picosecond runaway-electron beam in coaxial diode filled with SF6 at atmospheric pressure |
2659 |
3084 |
467 |
Luminescence of crystals excited by a runaway electron beam and by excilamp radiation with a peak wavelength of 222 nm |
8245 |
8412 |
307 |
Whether and how the vapors of Al, Cu, Fe, and W influence the dynamics of apokamps |
1256 |
1423 |
196 |
NOx formation in apokamp-type atmospheric pressure plasma jets in air initiated by a pulse-repetitive discharge |
2919 |
3087 |
226 |
Luminescence of atoms and ions of metals in a pulse-periodic nanosecond discharge |
1123 |
1332 |
226 |
Characteristics of a pulse-periodic corona discharge in atmospheric air |
2656 |
2920 |
329 |
Formation of nitrogen oxides in an apokamp-type plasma source |
1863 |
1844 |
3 |
Runaway electrons preionized diffuse discharges |
2498 |
2478 |
4 |
Luminescence of Ga2O3 crystals excited with a runaway electron beam |
3431 |
3370 |
3 |
Parameters of REP DDs plasma formed during the pulse and pulse-periodic modes in dense gases |
1219 |
1431 |
219 |
Subnanosecond breakdown in high-pressure gases |
1191 |
1177 |
5 |
Generation of neutrons in a nanosecond low-pressure discharge in deuterium |
2523 |
2756 |
252 |
Optical characteristics of DBD driven cold plasma needle radiation at elevated pressures |
813 |
966 |
164 |
Effect of pulse nanosecond volume discharge in air at atmospheric pressure on electrical properties of MIS structures based on p-HgCdTe grown by molecular beam epitaxy |
7857 |
7823 |
6 |
The relaxation of electrophysical properties HgCdTe epitaxial films affected by plasma of high frequency nanosecond volume discharge in atmospheric-pressure air |
13326 |
13158 |
194 |
Excilamps and their applications |
1239 |
1228 |
7 |
Presowing XeCl excilamp irradiation of crops: field research and prospects |
3242 |
3532 |
367 |
Luminescence of polymethyl methacrylate excited by a runaway electron beam and by a KrCl excilamp |
3866 |
3820 |
4 |
Influence of pulsed nanosecond volume discharge in atmospheric-pressure air on the electrical characteristics of MCT epitaxial films |
2026 |
2306 |
303 |
ICCD-imaging of a plasma glow during the prebreakdown stage of nanosecond discharges at both polarities in nitrogen, air and argon |
2956 |
3160 |
240 |
Laboratory demonstration in the air red and blue mini-jets |
866 |
1045 |
198 |
Spots on electrodes and images of a gap during pulsed discharges in an inhomogeneous electric field at elevated pressures of air, nitrogen and argon |
20070 |
19743 |
6 |
Acoustic Characteristics of a Barrier Discharge XeCl Excilamp |
1208 |
1208 |
6 |
Inverted polarity effect at the subnanosecond high voltage breakdown of air |
1667 |
1668 |
7 |
On the question of the source of the apokamp |
1048 |
1213 |
193 |
Anode and cathode spots in high-voltage nanosecond-pulse discharge initiated by runaway electrons in air |
16019 |
15728 |
9 |
Laser action in run-away electron preionized diffuse discharges |
1417 |
1865 |
462 |
Changes in the electro-physical properties of MCT epitaxial films affected by a plasma volume discharge induced by an avalanche beam in atmospheric-pressure air |
3888 |
4111 |
236 |
Formation of a small 'bead lightning' in a half-microsecond discharge in air |
1189 |
1184 |
4 |
Emission spectra of apokamp-type atmospheric pressure plasma jets in air, argon, and helium |
704 |
813 |
133 |
Influence of nanoparticles and metal vapors on the color of laboratory and atmospheric discharges |
751 |
803 |
59 |
E-beam generation in discharges initiated by voltage pulses with a rise time of 200 ns at an air pressure of 12.5–100 kPa |
3707 |
3673 |
4 |
Cooling techniques for excilamps driven by dielectric barrier discharge |
315 |
355 |
51 |
Mechanism of additional self-focusing of an electron beam generated during a high-voltage nanosecond discharge in a gas-filled diode |
381 |
453 |
84 |
Narrow band UV lamp based on iodine vapor |
186 |
267 |
89 |
Runaway electrons at the formation of a positive ionization wave in nitrogen and air |
330 |
328 |
1 |
Plasma spectroscopy of runaway electron preionized diffuse discharges |
917 |
1129 |
218 |
Dynamics of ionization processes in high-pressure nitrogen, air, and SF6 during a subnanosecond breakdown initiated by runaway electrons |
982 |
1200 |
229 |
The relaxation of electrophysical properties of MCT epitaxial films after influence of a high frequency nanosecond volume discharge in atmospheric pressure air |
4408 |
4546 |
223 |
Bending of a Paths of a Cathode Streamer and Spark Leader in Runaway Electron Preionized Diffuse Discharges |
6529 |
6732 |
301 |
Modification of electrophysical parameters of HgCdTe epitaxial heterostructures under the action of a pulsed nanosecond discharge in gas environment at atmospheric-pressure |
3026 |
3240 |
260 |
Production of nitrogen oxides in air pulse-periodic discharge with apokamp |
1392 |
1371 |
4 |
Recombination radiation in synthetic and natural diamonds exposed to pulsed UV laser radiation |
1032 |
1027 |
4 |
Role of streamers in the formation of a corona discharge in a highly nonuniform electric field |
2526 |
2502 |
4 |
Spark discharge formation in an inhomogeneous electric field under conditions of runaway electron generation |
7631 |
7492 |
9 |
Influence of plasma volume discharge in atmospheric-pressure air on the admittance of MIS structures based on MBE p-HgCdTe |
3205 |
3368 |
217 |
Temporal and spatial structure of a runaway electron beam in air at atmospheric pressure |
1652 |
1639 |
6 |
Features of recording the time profile of single picosecond pulses in the real-time mode |
1178 |
1400 |
227 |
Formation of a negative streamer in nitrogen and air in a non-uniform electric field at submicrosecond front of voltage pulse |
1133 |
1431 |
323 |
Electro-physical characteristics of a HgCdTe epitaxial films upon exposure by a volume discharge in air at atmospheric pressure |
2266 |
2461 |
221 |
Apokamps produced by repetitive discharges in air |
4333 |
4601 |
339 |
Influence of complex impact of the picosecond electron beam and volume discharge in atmospheric-pressure air on the electronic properties of MCT epitaxial films surface |
1520 |
1671 |
227 |
The effect of convection rate on energy characteristics of Xe2 excilamp |
574 |
706 |
142 |
A planar source of atmospheric-pressure plasma jet |
2813 |
3004 |
253 |
Influence of pulsed nanosecond volume discharge in atmospheric-pressure air on the electrical characteristics of MCT epitaxial films |
24241 |
24138 |
309 |
Influence of frequency and voltage to apokamp discharge dynamics at moderate pressures |
1443 |
1617 |
218 |
Review of supershort avalanche electron beam during nanosecond-pulse discharges in some gases |
13211 |
13396 |
389 |
The features of breakdown of high-voltage nanosecond discharge initiated with runaway electrons in a nonuniform electric field |
1338 |
1533 |
213 |
X-ray radiation and runaway electron beams generated during discharges in atmospheric-pressure air at rise times of voltage pulse of 500 and 50 ns |
11176 |
11237 |
280 |
The impact of the plasma volume discharge in the atmospheric-pressure air on the distribution of the surface potential in a V-defect region of epitaxial HgCdTe films |
4559 |
4732 |
236 |
Efficient gas lasers pumped by double-discharge circuits with semiconductor opening switch |
990 |
993 |
8 |
Gas lasers pumped by diffuse discharge formed by run-away electrons |
920 |
1114 |
209 |
Diffuse discharge produced by repetitive nanosecond pulses in open air, nitrogen, and helium |
4915 |
4813 |
2 |
Influence of complex impact of the picosecond electron beam and volume discharge in atmospheric-pressure air on the electronic properties of MCT epitaxial films surface |
11567 |
11615 |
257 |
Parameters of runaway electron beam generated during excitation by nanosecond voltage pulses in short gaps filled with nitrogen |
1242 |
1512 |
279 |
Apokamp - a new source of ionisation waves in potential pulse-periodic discharge |
990 |
1150 |
185 |
Subnanosecond breakdown of a point-to-plane gap at negative and positive polarities |
864 |
1020 |
182 |
On the mechanism of the generation of runaway electrons after a breakdown of a gap |
298 |
296 |
2 |
Dynamics of apokamp-type atmospheric pressure plasma jets |
2124 |
2105 |
5 |
Ministarters and mini blue jets in air and nitrogen at a pulse-periodic discharge in a laboratory experiment |
1975 |
1943 |
4 |
Influence of a high-frequency pulsed nanosecond diffusion discharge in the nitrogen atmosphere on the electrical characteristics of a CdHgTe epitaxial films |
15602 |
15649 |
349 |
Excitonic absorption and emission in diamond near the edge of fundamental absorption |
3128 |
3448 |
361 |
Influence of electrode spacing and gas pressure on parameters of a runaway electron beam generating during the nanosecond breakdown in SF6 and nitrogen |
36435 |
35714 |
4 |
Duration of the runaway electron beam at a subnanosecond leading edge of the voltage pulse |
263 |
264 |
2 |
Theoretical and experimental study of the acoustic spectrum of a DBD-driven planar KrCl excilamp |
1195 |
1194 |
12 |
Self focusing mechanisms of an electron beam formed in a high voltage nanosecond low pressure discharge |
186 |
337 |
165 |
Diffuse discharge in SF6 and its mixtures with H2, D2 and C2H6 formed by nanosecond voltage pulses in non-uniform electric field |
1692 |
1908 |
263 |
Note: Measurement of extreme-short current pulse duration of runaway electron beam in atmospheric pressure air |
1632 |
1621 |
9 |
Applications of excilamps in microbiological and medical investigations |
1550 |
1860 |
325 |
Breakdown features of a high-voltage nanosecond discharge initiated with runaway electrons at subnanosecond voltage pulse rise time |
2022 |
2495 |
509 |
Titanium alloy surface modification by excimer laser irradiation |
1614 |
1609 |
2 |
Blue and Green Jets in Laboratory Discharges Initiated by Runaway Electrons |
1771 |
1984 |
238 |
Streamers at the subnanosecond breakdown of argon and nitrogen in nonuniform electric field at both polarities |
2463 |
2634 |
208 |
Efficient gas lasers pumped by run-away electron preionized diffuse discharge |
2002 |
2469 |
487 |
Displacement current during the formation of positive streamers in atmospheric pressure air with a highly inhomogeneous electric field |
2435 |
2807 |
420 |
Bent paths of a positive streamer and a cathode-directed spark leader in diffuse discharges preionized by runaway electrons |
15927 |
16102 |
390 |
Laser system: powerful XeCl* laser-dye laser for ecological monitoring of the atmosphere |
5595 |
5883 |
380 |
Influence of plasma volume discharge in atmospheric-pressure air on the admittance of MIS structures based on MBE p-HgCdTe |
3136 |
3349 |
225 |
Presowing irradiation of agricultural crops XeCl-excilamp: fieldwork and perspectives |
2610 |
2829 |
244 |
Dynamics of a positive streamer in atmospheric pressure air in a sharply inhomogeneous field under threshold conditions for breakdown of a gap |
849 |
1051 |
233 |
The laser-induced electron-hole liquid in the diamond: critical lattice temperature and non-equilibrium carrier density |
1462 |
1842 |
404 |
Features of streamer formation in a sharply non-uniform electric field |
2360 |
2617 |
299 |
High Energy Electrons Behind the Plane-Grid Cathode at Subnanosecond Discharge in Atmospheric Pressure Air |
842 |
1035 |
214 |
The laser-induced electron-hole liquid in the diamonds: critical lattice temperature and non-equilibrium carrier density |
764 |
940 |
204 |