Telecentric sub-field deflection with vail

Claim 2

A two stage, vail electron beam projection system including (a) a target, (b) a source of an electron beam and means for projecting said electron beam towards said target with the upper surface thereof defining a target plane, (c) a magnetic projection lens having a principal plane and a back focal plane located between said means for projecting and said target, (d) said means for projecting providing an electron beam directed towards said target, (e) lower stage means for providing deflection of said beam from area to area within a field, (f) upper stage means for providing deflection of said beam within a said area within a said field, said upper stage means being located above said lower stage means, said upper stage means deflecting said beam in a first direction away from the geometrical axis of said system, and then reflecting said beam in a second direction towards said geometrical axis of said system, said lower stage means deflecting said beam in one direction, and then in another, direction substantially normal to said target plane, (g) said beam crossing said back focal plane producing a telecentric condition of said beam in the image plane with said beam substantially normal to said target plane from said principal plane to said target plane, (h) said magnetic projection lens including a magnetic compensation structure positioned within said projection lens, whereby said projection system projects on said target plane from said projection system as deflected by said upper and lower stages, at all times maintaining the telecentric condition at said target plane throughout the entire range of deflection of said beam, assuring minimum errors due to target height variations.

Claim 3

A two stage, electron beam projection system in accordance with claim 1 wherein said magnetic compensation structure is substantially proportional to the first derivative of the axial magnetic projection field, with said axial magnetic projection field providing substantially a zero first derivative of said axial magnetic projection field in the vicinity of said target.

Claim 4

A two stage, electron beam projection system in accordance with claim 1 wherein said magnetic compensation structure includes a magnetic compensation yoke providing a field compensating for the radial component of the magnetic field of said projection lens.

Claim 5

A two stage, electron beam projection system including (a) a source of an electron beam and means for projecting said electron beam towards support means for holding a target with the upper surface thereof defining a target plane, (b) a magnetic projection lens having a principal plane and a back focal plane, (c) a plurality of magnetic beam shifting means for shifting the axis of said beam and the axis of said projection lens in synchronism, (d) lower stage means for providing deflection of said beam within a field, said lower stage means including first and second sets of deflection means, (e) said first set of deflection means deflecting said beam once in a first direction away from the geometrical axis of said system, said second set of deflection means then deflecting said beam back into a path towards the geometrical axis of said system, (f) upper stage means for providing deflection of said beam comprising third and fourth sets of deflection means for providing deflection of said beam to areas within said field, said upper stage means being located above said lower stage deflection means, (g) said third and fourth sets of deflection means being directed in the x and y directions of deflection for deflecting said beam once with said third set of deflection means, said fourth set of deflection means then deflecting said beam back into a path through a rocking point in said back focal plane and normal to said back focal plane of said projection lens, (h) said magnetic projection lens including a magnetic compensation structure positioned within the bore of said projection lens which is substantially proportional to the first derivative of the axial magnetic projection field, with said axial magnetic projection field providing substantially a zero first derivative of the magnetic projection field in the vicinity of said target, whereby said beam crosses said back focal plane of said projection lens producing a telecentric condition in the image plane with said beam substantially normal to said target plane from said principal plane to said target plane, whereby said projection system projects said spot on said target plane from said projection system as deflected by said upper and lower stages, at all times maintaining the telecentric condition at said target plane throughout the entire range of axis movement assuring minimum errors due to target height variations.

Claim 6

A two stage, electron beam projection system including (a) a source of an electron beam and means for projecting said electron beam towards support means for holding a target with the upper surface thereof defining a target plane, (b) a magnetic projection lens having a principal plane and a back focal plane, (c) a plurality of magnetic beam shifting means for shifting the axis of said beam and the axis of said projection lens in synchronism, (d) lower stage means for providing deflection of said beam within a field, said lower stage means including first and second sets of deflection means, (e) said first set of deflection means deflecting said beam once in a first direction away from the geometrical axis of said system, said second set of deflection means then deflecting said beam back into a path towards the geometrical axis of said system, (f) upper stage means for providing deflection of said beam comprising third and fourth sets of deflection means for providing deflection of said beam to areas within said field, said upper stage means being located above said lower stage deflection means, (g) said third and fourth sets of deflection means being directed in the x and y directions of deflection for deflecting said beam once with said third set of deflection means, said fourth set of deflection means then deflecting said beam back into a path through a rocking point in said back focal plane and normal to said back focal plane of said projection lens, (h) said magnetic projection lens including a magnetic compensation structure positioned within the bore of said projection lens which is substantially proportional to the first derivative of the axial magnetic projection field, with said axial magnetic projection field providing substantially a zero first derivative of the magnetic projection field in the vicinity of said target, whereby said beam crosses said back focal plane of said projection lens producing a telecentric condition in the image plane with said beam substantially normal to said target plane from said principal plane to said target plane, whereby said projection system projects said spot on said target plane from said projection system as deflected by said upper and lower stages, at all times maintaining the telecentric condition at said target plane throughout the entire range of axis movement assuring minimum errors due to target height variations.

Claim 7

A two stage, electron beam projection system including (a) a source of an electron beam and means for projecting said electron beam, (b) a magnetic projection lens having a principal plane and a back focal plane, (c) a plurality of magnetic beam shifting means for shifting the axis of said beam and the axis of said projection lens in synchronism, (c) a collimating lens, (d) a target plane, (e) said electron beam being providing a spot directed at said target plane, (f) said projection system including means for scanning a field to be exposed by said beam, (g) lower stage means for providing deflection of said beam over a field in a discontinuous row-by-row scan of said field, (h) upper stage means for providing deflection of said beam comprising first and second sets of electrostatic deflection plates for providing vector deflection of said beam to a series of particular loci upon a target, said upper stage means being located above said lower stage deflection means, (i) said first and second sets of plates being directed in the x and y directions of deflection for deflecting said beam once with said first set of plates and said second set of plates then deflecting said beam back into a path intersecting the geometrical axis of said beam at a rocking point in said back focal plane of said final projection lens in the absence of a deflection by said lower stage means, at the back focal plane of said final projection lens producing a telecentric condition in the image plane with said beam substantially normal to said target plane, whereby said projection system projects said spot on said target plane from said projection system as deflected by said upper and lower stages, at all times maintaining the telecentric condition at said target plane throughout the entire range of axis movement assuring minimum errors due to target height variations.

Claim 8

A two stage, electron beam projection system including (a) a source of an electron beam and means for projecting said electron beam, (b) a magnetic projection lens having a principal plane and a back focal plane, (c) a plurality of magnetic beam shifting means for shifting the axis of said beam and the axis of said projection lens in synchronism, (c) a collimating lens, (d) a target plane, (e) said electron beam being providing a spot directed at said target plane, (f) said projection system including means for scanning a field to be exposed by said beam, (g) lower stage means for providing deflection of said beam over a field in a discontinuous row-by-row scan of said field, (h) upper stage means for providing deflection of said beam comprising first and second sets of electrostatic deflection plates for providing vector deflection of said beam to a series of particular loci upon a target, said upper stage means being located above said lower stage deflection means, (i) said first and second sets of plates being directed in the x and y directions of deflection for deflecting said beam once with said first set of plates and said second set of plates then deflecting said beam back into a path intersecting the geometrical axis of said beam at a rocking point in said back focal plane of said final projection lens in the absence of a deflection by said lower stage means, at the back focal plane of said final projection lens producing a telecentric condition in the image plane with said beam substantially normal to said target plane, whereby said projection system projects said spot on said target plane from said projection system as deflected by said upper and lower stages, at all times maintaining the telecentric condition at said target plane throughout the entire range of axis movement assuring minimum errors due to target height variations.

Claim 9

A system in accordance with claim 5 wherein said lower stage deflection system comprises a magnetic deflection system for scanning said beam in a modified raster scan extending over a field on said target plane, with said modified raster scan proceeding from the center of one sub-field position to the next sub-field position, one-by-one, with said beam temporarily arresting its scan as it reaches the center of each current sub-field it reaches in said field to permit completion of operations of said electrostatic deflection system.

Claim 10

A system in accordance with claim 5 wherein said upper stage deflection system is proximate to said collimating lens.