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S. Shibata ?? ??? Yamagata Univ. ???? Department of Phys ????

S. Shibata ?? ??? Yamagata Univ. ???? Department of Phys ????

? FAN3 22 June 2012. The Structure of the Pulsar Magnetosphere via Particle Simulation. S. Shibata ?? ??? Yamagata Univ. ???? Department of Phys ????. Aim of our numerical study. via particle simulation, the main problems to be challenged are.

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642 views • 50 slides
Production of Ultra Slow Antiproton Beam and A Cusp Trap for ` H Synthesis

Production of Ultra Slow Antiproton Beam and A Cusp Trap for ` H Synthesis

Sept.25-26, Villars Meeting. Production of Ultra Slow Antiproton Beam and A Cusp Trap for ` H Synthesis. Y.Yamazaki On behalf of MUSASHI Group, ASACUSA Collaboration. Why intense ultra-slow/trapped ` ps?. 1 ? Atomic physics of "Heavy Electron" Ionization by ` p vs p

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573 views • 40 slides
PLASMA

PLASMA

PLASMA. SHERIN WAEL D.ISAM AL-ASHQER. What is plasma?. what is plasma?

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588 views • 24 slides
Electron Acceleration and Propagation and the Thermal Response in Solar Flares

Electron Acceleration and Propagation and the Thermal Response in Solar Flares

Electron Acceleration and Propagation and the Thermal Response in Solar Flares. Gordon D. Holman NASA/Goddard Space Flight Center. Chapter 3. The Collisional Thick-Target Model.

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289 views • 17 slides
The Self-Modulation I nstability

The Self-Modulation I nstability

Affects long drive beams. Long beam enters plasma. Free e- pulled towards proton beam. E- overshoot the proton beam. Ion region left behind head of proton beam. E- pulled back on axis by ions Impinge on proton beam. The Self-Modulation I nstability. +. +. -. -.

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188 views • 1 slides

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