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Home Image Analysis Bean-scanning-and-method-of-use-for-ion-implantation

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Details
Inventors: Turner, Norman L.;
Assignee: Varian Associates, Inc. (Palo Alto, CA)
Primary Examiner: Dixon; Harold A.
Assistant Examiner:
Attorney, Agent or Firm: Cole; Stanley Z., Berkowitz; Edward H.

In an ion implantation system, departure from uniform ion dosage of a planar workpiece is first compensated by modulating the scan rate of at least one coordinate of scan deflection in accordance with a non-linear waveform. The non-linear waveform is digitally synthesized from a plurality of contiguous linear segments, such segments having equal projection on the time axis. The pattern of two-dimensional scanning is then configured to correspond to an astable Lissajous figure. When the trace of such Lissajous figure returns to the initial origin of the pattern, the origin is then displaced by a fraction 1/n of the interval between parallel traces of the basic Lissajous pattern and the displaced Lissajous pattern is executed and again displaced n times until the interval has been traversed. The number n is chosen with reference to scan amplitude and the lateral extension of the beam at the workpiece; a sufficient noise component is tolerated in the deflection system to dither the beam about the average scan trace in order to remove small pattern in homogeneities.

DETAILED DESCRIPTION OF THE INVENTION The present invention in the functional context of an ion implantation system may be seen in FIG.
1.
A high voltage terminal 2 is held at high potential relative to ground by high voltage power supply 4.
Terminal 2 houses the apparatus required to form a beam of ions of desired species.
In common practice a gaseous feedstock of the desired species is employed.
To this end, a source gas produced from gas handling system 6 is directed to ion source 8.
A typical ion source will require a power supply 10 to sustain an ionizing discharge, power supply 12 to impose an axial magnetic field across the discharge region, and extraction supply 14 and vernier 14' cooperating with extraction electrode 16 to shape the electric field at the aperture of the source for effective removal of a well defined high current ion beam.
A more detailed description of ion source techniques is outside the scope of this work.
See for example L.
Valyi, "Atom and Ion Sources, Wiley-Interscience, 1978.
" The beam 18 diverging from the ion source 8 is momentum analyzed in analyzer magnet 20, the latter energized from analyzer power supply 22.
Analyzed beam passes through analyzer exit slit 24 and then to accelerator tube 26 where it encounters a carefully designed field gradient from the high voltage terminal 2 to ground potential.
Optical elements, such as a quadrupole triplet 28, 30, 32, and associated control system 34, operate to produce a spatial-energy focus at a desired image plane.
Two sets of electrostatic deflection plates, 40 and 42, arbitrarily labeled y and x respectively serve to direct the beam over the desired area of the image plane.
The waveform applied to the respective deflection plates and their synchronization to form the appropriate scanning program is accomplished by scanning system 43.
The quiescent beam is deflected sufficiently to completely separate neutral beam 44 (arising from charge-exchange collisions with residual gases) from the charged beam.
Target chamber 46 contains beam defining apertures, beam monitoring and integrating apparatus and equipment for introducing the wafer substrate in the vacuum system and aligning same with respect to the target plane



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