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Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA Suzhou, September 24, 2007

Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

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Page 1: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device

Xie, JinLin & LMPD groupCAS KEY LABORATORY OF BASIC PLASMA PHYSICS

UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINASuzhou, September 24, 2007

Page 2: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Outline• Introduction

– What & Why & How– LMPD in USTC

• What we have done by now– Background plasma– Topology of the magnetic field for MR– Diagnostics / Data Acquisition System / …

• Preliminary result• Future plan

Page 3: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Introduction: Linear Magnetized Plasma Device in USTC

DC, RF & Helicon discharge source;

Bmax: 1000GuassTe:1~10evTi:0.03~0.5evDenisty:108~1013cm-3

Experimental chamber

LIFquad-probe

emissive probelangmuir probe

Page 4: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Nagoya antenna

13.56MHz,2KWMatch network

Radius

Plasma source: Helicon discharge

RF Power

Plas

ma

Den

sity

Page 5: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Typical ParametersTypical ParametersLCD

UCLA Pre-update LMPD LMPD

Machine typical Length[cm] 30 10 10

Plasma Denisty[m-3] 1018 1014 ~1016 1014 ~1019

Electron temperature Te[ev] 10 ~4 1~10

Ion temperature Ti[ev] 2 0.03 0.03~0.5

B for Magnetic Reconnection[T]

0.002 0.01 0.01

Ion mass Mi/Mp 40 40 1~40

Ion sound gyro-radius Rci[cm] 60 13 2~18

Ion skin depth [cm] c/wpi 60 4500 7 ~ 14300

Electron skin depth [cm] c/wpe 0.5 17 0.2 ~ 53

Electron free path [cm] 100 ~40 >100 ~ 3

Resistive time [ms] 1.5 0.2 ~ 0.1

Alfven time[us] 25 <1 0.1 ~ 10

Lundquist number ~60 300 10 ~ 1000

Background plasma for MR experiment

Page 6: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

coil Vertical window

Pump

Hor. Window Experimental chamber

Plasma Source

Simulation result via OPERA

Magnetic field for reconnection

7 s 5 s

2500A

time

Curr

ent

Page 7: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Copper plate and Pulse current source

Page 8: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Diagnostics for MR • Characteristic for MR experiment in lab plasma

– High spatial resolution: small size Vs large enough S/N– Wide signal bandwidth: Low freq. ~ MHz or microwave High Spatio-temporal resolution

• What we have now:– 3D B dot probe B0 , B1 Current sheet, E…– Retarding grid energy analyzer EVDF & IVDF & flux– Electrostatic probes: Langmuir probe, emissive probe, Mach

probe… Ne, Te, Vf, Vp, Iion, Ie, Ion flux… – Laser induced fluorescence(LIF) IVDF & ion flux – Microwave antenna and related instrument EM radiation

– DAQ system: 12 channels x 5M; 128 x 2M; 2 x 60M

Page 9: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Vacuum chamber

precision platform for 2D scanning probe

Page 10: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Ion Saturation Current Electron Temperature

1 2 3 4 5 6 7 8 91

2

3

4

5

6

7

8

9

10

11

1.4

1.6

1.8

2

2.2

2.4

2.6

2.8

3

Page 11: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Reconstruction of the magnetic field linein order to verify MR process

x

Page 12: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Vacuum evolution

Page 13: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Research plan

• Verification of MR process in LMPD

• Heating and acceleration of electron & ion

• Electrostatic & electromagnetic turbulence

• ……….

Page 14: Progress of Magnetic Reconnection experiment in Linear Magnetized Plasma Device Xie, JinLin & LMPD group CAS KEY LABORATORY OF BASIC PLASMA PHYSICS UNIVERSITY

Thank you!