Patent Number: 
Section: claims

1. A method of accelerating an ion beam having an initial energy to a final higher energy and final direction while substantially eliminating contaminant ions and neutral atoms having energies other than the final energy, the method comprising:generating a beam of ions at an initial energy, guiding the ion beam along an ion beam path;controlling and adjusting the electrostatic potential and electric fields along the beam path so as to cause the ion beam to follow a generally s-shaped path while being accelerated, so that the ions in the ion beam are accelerated to the final energy and a centroid of the beam after acceleration travels generally in the final direction; andintercepting undeflected neutral atoms or molecules and/or charged fragmented molecular ions so as to remove them from the ion beam. 2. The method of claim 1 wherein the beam is deflected by a set of electrodes that provide two opposed successive sideways components on an accelerator field to provide the generally s-shaped path. 3. The method of claim 2 wherein the deflections each amount to an angle of at least 10 degrees. 4. The method of claim 1 wherein beam stops are utilized to intercept the undeflected ions. 5. The method of claim 1 wherein the energy of the beam is raised beyond the desired final energy, then retarded to the final energy in a short, approximately straight, final decelerating gap. 6. A method of decelerating an ion beam having an initial energy to a final higher energy and final direction while substantially eliminating contaminant ions and neutral atoms having energies other than the final energy, the method comprising:generating a beam of ions at an initial energy, guiding the ion beam along an ion beam path;controlling and adjusting the electrostatic potential and electric fields along the beam path so as to cause the ion beam to follow a generally s-shaped path while being decelerated, so that the ions in the ion beam are decelerated to the final energy and a centroid of the beam after acceleration travels generally in the final direction; andintercepting undeflected neutral atoms or molecules and/or charged fragmented molecular ions so as to remove them from the ion beam. 7. The method of claim 6 wherein the beam is deflected by a set of electrodes that provide two opposed successive sideways components on an accelerator field to provide the generally s-shaped path. 8. The method of claim 7 wherein the deflections each amount to an angle of at least 10 degrees. 9. The method of claim 6 wherein beam stops are utilized to intercept the undeflected ions. 10. The method of decelerating an ion beam wherein the energy of the beam is slightly increased prior to deceleration according to the method of claim 6, thereby preventing the acceleration of unwanted particles of opposite charge to the desired ions. 11. A system of accelerating an ion beam having an initial energy to a final higher energy and final direction while substantially eliminating contaminant ions and neutral atoms having energies other than the final energy, the system comprising:means for generating a beam of ions at an initial energy, guiding the ion beam along an ion beam path;means for controlling and adjusting the electrostatic potential and electric fields along the beam path so as to cause the ion beam to follow a generally s-shaped path while being accelerated, so that the ions in the ion beam are accelerated to the final energy and a centroid of the beam after acceleration travels generally in the final direction; andmeans for intercepting undeflected neutral atoms or molecules and/or charged fragmented molecular ions so as to remove them from the ion beam. 12. The system of claim 11 wherein the beam is deflected by a set of electrodes that provide two opposed successive sideways components on an accelerator field to provide the generally s-shaped path. 13. The system of claim 12 wherein the deflections each amount to an angle of at least 10 degrees. 14. The system of claim 11 wherein beam stops are utilized to intercept the undeflected ions. 15. The system of claim 11 wherein the energy of the beam is raised beyond the desired final energy, then retarded to the final energy in a short, approximately straight, final decelerating gap. 16. A system of decelerating an ion beam having an initial energy to a final higher energy and final direction while substantially eliminating contaminant ions and neutral atoms having energies other than the final energy, the system comprising:means for generating a beam of ions at an initial energy, guiding the ion beam along an ion beam path;means for controlling and adjusting the electrostatic potential and electric fields along the beam path so as to cause the ion beam to follow a generally s-shaped path while being decelerated, so that the ions in the ion beam are decelerated to the final energy and a centroid of the beam after acceleration travels generally in the final direction; andmeans for intercepting undeflected neutral atoms or molecules and/or charged fragmented molecular ions so as to remove them from the ion beam. 17. The system of claim 16 wherein the beam is deflected by a set of electrodes that provide two opposed successive sideways components on an accelerator field to provide the generally s-shaped path. 18. The system of claim 17 wherein the deflections each amount to an angle of at least 10 degrees. 19. The system of claim 16 wherein beam stops are utilized to intercept the undeflected ions. 20. The system of decelerating an ion beam wherein the energy of the beam is initially raised beyond the desired final energy, then retarded to the final energy gy using the system of claim 16. 21. An ion implantation apparatus comprising:an ion source, an extraction assembly for extracting an ion beam;a magnetic analyzer for separating unwanted ion species from a traveling ribbon ion beam; anda target chamber in which is mounted a target for implantation, Illustratively, the target is a semiconductor wafer or flat panel display, which is moved through the beam (optionally back and forth) along a single path; wherein the beam is ribbon shaped, with one dimension many times greater than the other, and the longer dimension is aligned with the non-dispersive plane of the magnetic analyzer. 22. The on implantation apparatus of claim 21 wherein the magnetic analyzer comprises:central axis and intended arc pathway for a ribbon ion beam as it travels, said central axis having a curvilinear shape;an arcuate yoke construct encompassing said predetermined curvilinear shaped central axis and surrounding said intended arc pathway for the continuous ribbon ion beam as it travels, said arcuate yoke construct being formed at least in part of a ferromagnetic material and comprising an arcuate wall structure having fixed dimensions and a substantially rectangular cross-section, two discrete open ends which serve as an entrance and exit for the traveling beam, and an internal spatial region of determinable volume which serves as a spatial passageway for the traveling beam; anda mirror symmetrical pair of discrete loop-shaped coils utilized as an aligned array. 23. The on implantation apparatus of claim 22 wherein each discrete coil of the pair in the aligned array (i) is an elongated complete loop comprised at least in part of electrically conductive material, (ii) is an elongated complete loop having two rounded and inclined discrete loop ends, each of which is bent in the same direction, and (iii) is an elongated complete loop formed as a set of multiple conductive segments placed in sequential series wherein each segment lies at a pre-chosen sequence position and individual angle orientation with respect to the central axis and intended arc pathway for the ribbon ion beam as it travels within said internal spatial region of said arcuate yoke construct. 24. The ion implantation apparatus of claim 23 wherein the aligned array of two looped-shaped coils set in mirror symmetry (iv) presents a bend direction for the two rounded inclined ends of one looped-shaped coil which is opposite to the bend direction for the two rounded inclined ends of the other looped-shaped coil in the pair, (v) provides a central open spatial channel via the cavity volume of the closed loop in each of the two coils, said central open spatial channel extending from each pair of inclined rounded loop ends to the other over the linear dimensional distance of the array, (vi) is positioned within said internal spatial region along the interior surfaces of two opposing walls of said arcuate yoke construct such that one pair of oppositely bent inclined loop ends extends from and lies adjacent to each of the two open ends of said arcuate yoke construct, (vii) serves as limiting boundaries for said curvilinear central axis and intended arc pathway for the continuous ribbon ion beam as it travels in the gap space between said two loop-shaped coils after being positioned within said internal spatial region of said arcuate yoke construct. 25. The ion implantation apparatus of claim 22 wherein in order to create a magnetic field with good uniformity, without excessive stray field, the field is generated by at least two coils or symmetric sets of coils, which are of saddle shape, one above and one below the beam, wherein the region of uniform field is bounded by the coil windings. 26. The ion implantation apparatus of claim 22 in which the arc pathway includes, an arc with a radius ranging between about 0.25 and 2 meters, and an angle of curvature ranging from not less than about 45 degrees to not more than about 110 degrees of curvature.