# US 2014/0151571 A1 · Charged particle beam lens and exposure apparatus using the same > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 2014/0151571 A1 - Document ID: US20140151571A1 - Status: Published application - Kind: A1 - Application number: 14/005,175 - Filed: 2012-03-14 - Published: 2014-06-05 - Earliest claimed: 2011-03-15 - Assignees: Canon Kabushiki Kaisha - Inventors: Takahisa Kato; Yutaka Setomoto - Web page: https://patentgrep.com/patent/US20140151571A1 ## CPC - H01J 37/12: electrostatic - H01J 2237/04924: electrostatic - H01J 2237/1205: Microlenses - H01J 2237/1207: Einzel lenses - H01J 2237/31774: Multi-beam - H01J: ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS (spark-gaps H01T; electric arc lamps H05B31/00; particle accelerators H05H) ## Abstract In a charged particle beam lens according to the present invention, the orientations of through-holes formed in electrodes and precision of forming the through-holes are determined in accordance with the degree of influences of the surfaces of the electrodes on the aberration of the lens. ## Claims ### Claim 1 An electrostatic charged particle beam lens comprising: a first flat plate including a first surface having a normal line extending in a direction of an optical axis and a second surface opposite to the first surface; a second flat plate including a third surface facing the second surface and a fourth surface opposite to the third surface; and a third flat plate including a fifth surface facing the fourth surface and a sixth surface opposite to the third surface, wherein the first flat plate has a first through-hole extending therethrough from the first surface to the second surface, wherein the second flat plate has a second through-hole extending therethrough from the third surface to the fourth surface, wherein the third flat plate has a third through-hole extending therethrough from the fifth surface to the sixth surface, wherein the first through-hole, the second through-hole, and the third through-hole are arranged so that a charged particle beam is allowed to successively pass therethrough, and wherein, when an opening cross section is defined as a cross section of one of the through-holes taken along a plane perpendicular to the optical axis and an incircle and a circumcircle are respectively defined as two concentric circles having a smaller radius and a larger radius between which the opening cross section is disposed and having the smallest difference in the radii, a difference in the radii of the incircle and the circumcircle of the opening cross section at each of the first surface and the sixth surface is larger than a difference in the radii of the incircle and the circumcircle of the opening cross section at each of the second surface, the third surface, the fourth surface, and the fifth surface. ### Claim 2 (depends on 1) The charged particle beam lens according to claim 1, wherein, when the first surface and the second surface have a first potential, the third surface and the fourth surface have a second potential, the fifth surface and the sixth surface have a third potential, and the charged particle beam has a negative charge, the difference in the radii of the incircle and the circumcircle of the opening cross section of one of the second surface and the third surface having a lower potential is smaller than the difference in the radii of the incircle and the circumcircle of the opening cross section of one of the second surface and the third surface having a higher potential. ### Claim 3 (depends on 1) The charged particle beam lens according to claim 1, wherein, when the first surface and the second surface have a first potential, the third surface and the fourth surface have a second potential, the fifth surface and the sixth surface have a third potential, and the charged particle beam has a negative charge, the difference in the radii of the incircle and the circumcircle of the opening cross section of one of the fourth surface and the fifth surface having a lower potential is smaller than the difference in the radii of the incircle and the circumcircle of the opening cross section of one of the fourth surface and the fifth surface having a higher potential. ### Claim 4 (depends on 2) The charged particle beam lens according to claim 2, wherein the first potential and the third potential are a ground potential, the second potential is a negative potential, and the difference in the radii of the incircle and the circumcircle of the opening cross section of the third surface is smaller than the difference in the radii of the incircle and the circumcircle of the opening cross section of the fourth surface. ### Claim 5 (depends on 1) The charged particle beam lens according to claim 1, wherein, when the first surface and the second surface have a first potential, the third surface and the fourth surface have a second potential, the fifth surface and the sixth surface have a third potential, and the charged particle beam has a positive charge, the difference in the radii of the incircle and the circumcircle of the opening cross section of one of the second surface and the third surface having a higher potential is smaller than the difference in the radii of the incircle and the circumcircle of the opening cross section of one of the second surface and the third surface having a lower potential. ### Claim 6 (depends on 1) The charged particle beam lens according to claim 1, wherein when the first surface and the second surface have a first potential, the third surface and the fourth surface have a second potential, the fifth surface and the sixth surface have a third potential, and the charged particle beam has a positive charge, the difference in the radii of the incircle and the circumcircle of the opening cross section of one of the fourth surface and the fifth surface having a higher potential is smaller than the difference in the radii of the incircle and the circumcircle of the opening cross section of one of the fourth surface and the fifth surface having a lower potential. ### Claim 7 (depends on 5) The charged particle beam lens according to claim 5, wherein the first potential and the third potential are a ground potential, the second potential is a positive potential, and the difference in the radii of the incircle and the circumcircle of the opening cross section of the third surface is smaller than the difference in the radii of the incircle and the circumcircle of the opening cross section of the fourth surface. ### Claim 8 (depends on 1) The charged particle beam lens according to claim 1, wherein at least one of the first flat plate, the second flat plate, and the third flat plate has a stacked or bonded structure. ### Claim 9 (depends on 1) The charged particle beam lens according to claim 1, wherein each of the first flat plate, the second flat plate, and the third flat plate is an array having a plurality of through-holes. ### Claim 10 (depends on 1) An exposure apparatus comprising the charged particle beam lens according to claim 1 and using a charged particle beam. ### Claim 11 (depends on 10) The exposure apparatus according to claim 10 using a plurality of charged particle beams. ### Claim 12 An electrostatic charged particle beam lens comprising: a first flat plate including a first surface having a normal line extending in a direction of an optical axis and a second surface opposite to the first surface; a second flat plate including a third surface facing the second surface and a fourth surface opposite to the third surface; and a third flat plate including a fifth surface facing the fourth surface and a sixth surface opposite to the third surface, wherein the first flat plate has a first through-hole extending therethrough from the first surface to the second surface, wherein the second flat plate has a second through-hole extending therethrough from the third surface to the fourth surface, wherein the third flat plate has a third through-hole extending therethrough from the fifth surface to the sixth surface, wherein the first through-hole, the second through-hole, and the third through-hole are arranged so that a charged particle beam is allowed to successively pass therethrough, and wherein, when an opening cross section is defined as a cross section of one of the through-holes taken along a plane perpendicular to the optical axis, a value of circularity of the opening cross section at each of the first surface and the sixth surface is larger than a value of circularity of the opening cross section at each of the second surface, the third surface, the fourth surface, and the fifth surface.