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Charge Exchange Cross Sections for Electron Loss from B+, P+, and N+ on N2
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1971
Year
EngineeringNuclear PhysicsDouble Electron LossIon Beam InstrumentationElectron LossCharge TransportIon ProcessElectron PhysicHeavy Ion PhysicCross SectionsElectron SpectroscopyIon BeamIon EmissionCharge Carrier TransportElectrical EngineeringPhysicsAtomic PhysicsQuantum ChemistryNatural SciencesCondensed Matter PhysicsApplied Physics
The cross sections for electron loss from singly ionized B, N, and P ions at 100 keV, 200 keV, and 300 keV in collisions with N2 have been measured. The cross sections for a singly ionized projectile to become doubly ionized, σ12, are (10−16 cm2 per molecule): σ12 (B, 100 keV) = 2.0, σ12 (B, 200 keV) = 3.4, σ12 (B, 300 keV) = 4.4, σ12 (N, 100 keV) = 2.2, σ12 (N, 200 keV) = 3.4, σ12 (N, 300 keV) = 4.6, σ12 (P, 100 keV) = 4.3, σ12 (P, 200 keV) = 6.6, and σ12 (P, 300 keV) = 8.7. The cross sections for double electron loss were also measured. The observed cross section for P+→P2+ indicates that for a 1% contamination of a 300-keV P+ ion beam with P2+, the pressure times path length of the beam is 3.5×10−6 Torr m.