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Q - (e-ch .) Brutal force Sophisticated appr. 10 11 10 KW

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Q - (e-ch .) Brutal force Sophisticated appr. 10 11 10 KW

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  1. Electron String Phenomenon:Physics and ApplicationsbyE. D. Donets, S. V. Gudkov, D. E. Donets, E. E. Donets, A. D. Kovalenko, S. V. Salnikov, V. B. Shutov, E. M. Syresin, Yu. A. Tumanova and V. P. VadeevThe work was supported in part by the International Association (Grants: INTAS-96-0255, INTAS-01-2354), the Civilian Research and Development Foundation (Grants: RP1-2110, RP1-2417-DU-02), the Royal Swedish Academy of Science and by the Government of Japan in frame of the “Centers of Excellence” program.

  2. 1. Electron string is the first discovered high temperature stationary state of one component electron plasma, which is confined by strong solenoid magnetic and weak constant electric fields. 2. Electron string is formed in nonlinear process via strong instability of trapped electrons and exists as a dynamic equilibrium of injecting and loosing electrons. 3. Electron string state is quasi stable and quiet in a broad region of condition parameters, so that it can be used for ion trapping in its space charge and for production of highly charged ionsby string electron impact. 4. Electron string ion source was developed and applied on the Nuclotron facility for production of relativistic beams of Ar16+ and Fe24+ . 200  A and 150  A pulse ion currents correspondingly were produced for injection into the LINAC.

  3. 5. The tubular version of the electron string state is a goal of researches now. Factor 100-1000 in increase of ionization efficiency and of ion output is expected for a tubular apparatus. 6. Electron string phenomenon can be used for the proof of the p-p chain in the standard model of Sun energy generation to bring the new information on neutrino production in the chain. 7. Similar to electron string the positron one can exist.

  4. Q-(e-ch.) Brutal force Sophisticated appr. 1011 10 KW 1012 200 KW 1013 5000 KW

  5. Experimental conditions:Bmax = 3.5 T; Vacuum P < 10-12 torr Drift tube temperature 4.2 K Total length of the drift tube structure 1.2 m 0.2 mm 1 mm 3 mm

  6. DRIFT TUBE -Q -Q -Q R -Q t -Q IMAGE CURRENT VIA THE RESISTOR

  7. 5 A electron current injected Electron current accumulated Injection electron current:5 A

  8. 50 Aelectron current injected Electron current accumulated Electron current ejected Injection electron current:50 A

  9. 500 Aelectron current injected Electron current accumulated Injection electron current:500 A

  10. measured with the method of controlled decay of electron string

  11. The method of radiative electron capture Kinetic electron energy distribution in the string with the feeding electron energy equal to 5.4 KeV

  12. Transition to the electron string state, detected by means of observation of the change in the pulse ion current produced. (1996)

  13. Charge state distribution of Ar ions after 500 ms confinement in an electron string space. IAr16+ = 200 A in 8 s

  14. Charge state distribution of Fe ions after 1100 ms confinement in space of an electron string. IFe24+ = 150 A in 8 s

  15. Tubular electron string (painting)

  16. Off-axis ion extraction from tubular electron string (painting)

  17. 3D-simulation of the off-axis ion extraction from a tubular string

  18. Q-(e-ch.) Brutal force. ESIS/TESIS 1011 10 KW 50 W 1012 200 KW 200 W 1013 5000 KW 2 KW 1014 20 KW 1015 200 KW

  19. S-f MeVb 14 13 12 11 10 9 8 7 6 5 4 3 2 1 0 LUNA data OCEANdata Extrapolation 16 18 20 22 24 26 28 30 32 34 KeV Ecm

  20. 1. Electron string is the first discovered high temperature stationary state of one component electron plasma, which is confined by strong solenoid magnetic and weak constant electric fields. 2. Electron string is formed in nonlinear process via strong instability of trapped electrons and exists as a dynamic equilibrium of injecting and loosing electrons. 3. Electron string state is quasi stable and quiet in a broad region of condition parameters, so that it can be used for ion trapping in its space charge and for production of highly charged ions by the string electron impact. 4. Electron string ion source was developed and applied on the Nuclotron facility for production of relativistic beams of Ar16+ and Fe24+ . 200 A and 150  A pulse ion currents correspondingly were produced for injection into the LINAC. 5. The tubular version of the electron string state is a goal of researches now. Factor 100-1000 in increase of ionization efficiency and of ion output is expected for a tubular apparatus. 6. Electron string phenomenon can be used for the proof of the p-p chain in the standard model of Sun energy generation to bring the new information on neutrino production in the chain. 7. Similar to electron string the positron one can exist.

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