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Electron interactions with CO 2 Bob Merlino Department of Physics and Astronomy The University of Iowa Iowa City, IA U. S. Department of Energy National.

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Presentation on theme: "Electron interactions with CO 2 Bob Merlino Department of Physics and Astronomy The University of Iowa Iowa City, IA U. S. Department of Energy National."— Presentation transcript:

1 Electron interactions with CO 2 Bob Merlino Department of Physics and Astronomy The University of Iowa Iowa City, IA U. S. Department of Energy National Energy Technology Laboratory May 30, 2008

2 Electron impact ionization

3 Electron attachment to CO 2 Y. Itikawa, J. Phys. Chem. Ref. Data, 31,749, 2002 CO 2 cannot permanently bind an electron, so that is metastable, with lifetimes in the microsec to millisec range, decaying back to CO 2 by auto- detachment: the electron attachment probability is enhanced if CO 2 is in an excited vibrational state electron energy (eV) attach. cross section (10 -18 cm 2 )

4 Devices at the University of Iowa Plasma Laboratory 2 Q machines with magnetic fields up to 0.5 T – 6 cm diam. by 2 m length, variable B profile – 6 cm diam. by 1 m length, which can also operate in the presence of micron sized dust particles A glow discharge, dusty plasma / multidipole device, 60 cm diam. x 90 cm length A multidipole/inductively coupled plasma device, 84 cm diam. x 130 cm length (The UI physics dept. has agreed to provide this device.)

5 Q machine / Discharge plasma This device can be operated either with a thermal, surface ionization plasma source (QM) which produces either as K or Cs plasma, or as a discharge device using He, Ar, Ne, Xe, N 2, by removing the hot plate and biasing the filament negatively. In the Q mode the electrons are relatively cold with Te ~ 0.2 eV In the discharge mode there are thermal electrons with Te ~ 2 – 5 eV and with a population of energetic electrons with Ee ~ 30 –100 V. B Hot Plate Langmuir Probe Hvac Pump Plasma hot filament K oven Cold Plate Solenoid coils Gas inlet

6 IOWA Q-3IOWA Q-2

7 Hot filament multidipole plasma source GAS TURBOMOLECULAR PUMP FILAMENT MAGNETS LANGMUIR PROBE T e  2 – 5 eV 84 cm 130 cm

8 Inductively coupled plasma source TURBOMOLECULAR PUMP GAS LANGMUIR PROBE T e  2 – 5 eV 84 cm 130 cm

9 Formation of The presence of is confirmed by observing the spectrum of ion cyclotron waves in the plasma is a metastable negative ion B = 0.3 T P(CO 2 ) = 6  10 – 5 Torr V probe = 15 V 10 dB K+K+ 0 100 200 300 400 500 Frequency (kHz)

10 Mass spectrometer measurements -160 -120 -80 -40 0 40 80 120 160 K + Cs + SF - 6 VOLTS 2 ion plasma K + / Cs + K + / SF 6 – plasma


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