# US 8,569,694 B2 · Aberration-correcting dark-field electron microscopy > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 8,569,694 B2 - Document ID: US8569694B2 - Status: Granted - Kind: B2 - Application number: 13/657,843 - Filed: 2012-10-22 - Published: 2013-02-21 - Granted: 2013-10-29 - Earliest claimed: 2010-02-10 - Assignees: Mochii, Inc. - Applicants: Mochii, Inc. - Inventors: Christopher Su-Yan Own; Andrew Bleloch; Paul John Dabrowski - Web page: https://patentgrep.com/patent/US8569694B2 ## CPC - H01J 37/153: Electron-optical or ion-optical arrangements for the correction of image defects, e.g. stigmators - H01J 37/26: Electron or ion microscopes; Electron or ion diffraction tubes - H01J 2237/2614: Holography or phase contrast, phase related imaging in general, e.g. phase plates - H01J 2237/262: Non-scanning techniques - H01J: ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS (spark-gaps H01T; electric arc lamps H05B31/00; particle accelerators H05H) ## Abstract A transmission electron microscope includes an electron beam source to generate an electron beam. Beam optics are provided to converge the electron beam. An aberration corrector comprising either a foil or a set of concentric elements corrects the electron beam for at least a spherical aberration. A specimen holder is provided to hold a specimen in the path of the electron beam. A detector is used to detect the electron beam transmitted through the specimen. The transmission electron microscope may be configured to operate in a dark-field mode in which a zero beam of the electron beam is not detected. The microscope may also be capable of operating in an incoherent illumination mode. ## Claims ### Claim 1 A transmission electron microscope comprising: an electron beam source to generate an electron beam; beam optics to converge the electron beam, the beam optics defining an optic axis of the microscope along which there is substantial cylindrical symmetry of the beam optics; an aberration corrector comprising a foil located approximately at the optic axis, the aberration corrector being adapted to correct the electron beam for at least a spherical aberration; a specimen holder to hold a specimen in the path of the electron beam; and a detector to detect the electron beam transmitted through the specimen. ### Claim 2 (depends on 1) The transmission electron microscope of claim 1, wherein the foil comprises a conductive grid, the conductive grid comprising a metal. ### Claim 3 (depends on 2) The transmission electron microscope of claim 2, wherein the conductive grid has a thickness of from about 0.1 nm to about 10 nm. ### Claim 4 (depends on 1) The transmission electron microscope of claim 1, wherein the foil comprises a material that changes at least one dimension in relation to temperature, and further comprising a temperature applicator to change the temperature of the foil to induce a change in an electric field created by the foil. ### Claim 5 (depends on 1) The transmission electron microscope of claim 1, wherein the foil comprises (i) two metal layers and (ii) an insulating layer between the two metal layers, and wherein the foil has an aperture passing through the metal layers and the insulating layer. ### Claim 6 (depends on 5) The transmission electron microscope of claim 5, wherein the foil further comprises a film comprising carbon on one of the metal layers, on the side of the metal layer that is opposite the insulating layer. ### Claim 7 (depends on 1) The transmission electron microscope of claim 1, wherein the aberration corrector is adapted to correct for a parasitic aberration. ### Claim 8 (depends on 7) The transmission electron microscope of claim 7, wherein the aberration corrector further comprises a multipole element to (i) predistort the electron beam before the electron beam enters the foil and (ii) undistort the electron beam after the electron beam has left the foil. ### Claim 9 (depends on 1) The electron beam assembly of claim 1, comprising an annular aperture to produce a dark-field mode in which a zero beam of the electron beam is not detected, the dark-field stop comprising (i) a circular-disc stop with a substantially circular cross-section approximately at the radial center of the electron beam to stop a central portion of the electron beam; and (ii) an outer stop concentric with, and spaced from, the circular-disc stop, such that there is an annular gap between the circular-disc stop and the outer stop. ### Claim 10 (depends on 9) The electron beam assembly of claim 9, wherein the annular aperture is adapted to limit transmission of electrons scattered from the specimen to an angular range between an inner angle and an outer angle, the inner angle being from about 0.1 mrad to about 20 mrad, and the outer angle being at least about 1 mrad. ### Claim 11 (depends on 1) The transmission electron microscope of claim 1, wherein the beam optics comprise an objective lens, and wherein the foil is positioned outside the objective lens. ### Claim 12 A transmission electron microscope comprising: an electron beam source to generate an electron beam; beam optics to converge the electron beam, the beam optics defining an optic axis of the microscope along which there is substantial cylindrical symmetry of the beam optics; an aberration corrector comprising a set of elements approximately concentric about the optic axis, the concentric elements being adapted to have different respective electric potentials applied to them, the aberration corrector being adapted to correct the electron beam for at least a spherical aberration; a specimen holder to hold a specimen in the path of the electron beam; and a detector to detect the electron beam transmitted through the specimen. ### Claim 13 (depends on 12) The transmission electron microscope of claim 12, wherein at least one of the concentric elements is approximately cylindrically symmetric. ### Claim 14 (depends on 13) The transmission electron microscope of claim 13, wherein the cylindrically symmetric concentric element has the shape of a conical section. ### Claim 15 (depends on 13) The transmission electron microscope of claim 13, wherein the cylindrically symmetric concentric element has a curved surface. ### Claim 16 (depends on 13) The transmission electron microscope of claim 13, wherein the set of elements of the aberration corrector comprises at least three elements, the three elements being adapted to have different respective electric potentials applied to them. ### Claim 17 (depends on 13) The transmission electron microscope of claim 13, wherein the cylindrically symmetric concentric element is a ring, and wherein the aberration corrector further comprises two or more spokes to support the ring. ### Claim 18 (depends on 12) The transmission electron microscope of claim 12, wherein the aberration corrector is adapted to correct for a parasitic aberration. ### Claim 19 (depends on 12) The transmission electron microscope of claim 12, wherein the beam optics comprise an objective lens, and wherein the set of elements of the aberration corrector is positioned outside the objective lens. ### Claim 20 A method for diagnosing aberrations in a transmission electron microscope that is adapted to operate in a dark-field mode in which a zero beam of the electron beam is not detected, the method comprising: acquiring one or more images, as a function of either illumination tilt or defocus, from the transmission electron microscope; extracting a value for the blurring effect of the tilt or defocus from the images; and calculating a value for defocus or astigmatism based on the value for the blurring effect and the value for either the illumination tilt or the defocus.