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A cusp field or and end block can greatly increase the density

A cusp field or and end block can greatly increase the density. G. Chevalier and F.F. Chen , Experimental modeling of inductive discharges , J. Vac. Sci. Technol. A 11 , 1165 ( 1993 ). Radial mode structure is m = +1, even when antenna is made to excite m = –1.

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A cusp field or and end block can greatly increase the density

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  1. A cusp field or and end block can greatly increase the density G. Chevalier and F.F. Chen, Experimental modeling of inductive discharges, J. Vac. Sci. Technol. A11, 1165 (1993)

  2. Radial mode structure is m = +1,even when antenna is made to excite m = –1 M. Light and F.F. Chen, Helicon Wave Excitation with Helical Antennas, Phys. Plasmas2, 1084 (1995) RH antenna LH antenna

  3. Axial beating of radial modes M. Light, I.D. Sudit, F.F. Chen, and D. Arnush, Axial Propagation of Helicon Waves, Phys. Plasmas2, 4094 (1995)

  4. Density is peaked 50 cm downstream,due to pressure balance I.D. Sudit and F.F. Chen, Discharge equilibrium of a helicon plasma, Plasma Sources Sci. Technol.5, 43 (1996)

  5. F.F. Chen, I.D. Sudit, and M. Light, Downstream physics of the helicon discharge, Plasma Sources Sci. Technol.5, 173 (1996) Helical antennas are directional;Nagoya IIIs are not Beating length and KTe decayagree with theory

  6. Rotating the field with a bifilar antenna is betterthan spatial rotation with helical antennas D.G. Miljak and F.F. Chen, Helicon wave excitation with rotating antenna fields, Plasma Sources Sci. Technol.7, 61 (1998)

  7. Injecting from both ends does not increase thedensity because of neutral depletion D.G. Miljak and F.F. Chen, Density limit in helicon discharges, Plasma Sources Sci. Technol.7, 537 (1998)

  8. Half wavelength helical antennas are betterthan full wavelength antennas L. Porte, S.M. Yun, F.F. Chen, and D. Arnush, Superiority of half-wavelength helicon antennas,LTP-110 (Oct. 2001)

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