Phase gratings with odd symmetry for lensed optical sensing
US-9442228-B2 · Sep 13, 2016 · US
US9256068B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9256068-B2 |
| Application number | US-201414338542-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jul 23, 2014 |
| Priority date | Jul 24, 2013 |
| Publication date | Feb 9, 2016 |
| Grant date | Feb 9, 2016 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
A spherical aberration corrector is offered which permits a correction of deviation of the circularity of at least one of an image and a diffraction pattern and a correction of on-axis aberrations to be carried out independently. The spherical aberration corrector ( 100 ) is for use with a charged particle beam instrument ( 1 ) for obtaining the image and the diffraction pattern and has a hexapole field generating portion ( 110 ) for producing plural stages of hexapole fields, an octopole field superimposing portion ( 120 ) for superimposing an octopole on at least one of the plural stages of hexapole fields to correct deviation of the circularity of at least one of the image and diffraction pattern, and a deflection portion ( 130 ) for deflecting a charged particle beam.
Opening claim text (preview).
The invention claimed is: 1. A spherical aberration corrector for use with a charged particle beam instrument for obtaining an image and a diffraction pattern, said spherical aberration corrector comprising: a hexapole field generating portion for producing plural stages of hexapole fields; an octopole field superimposing portion for superimposing an octopole field on at least one of the hexapole fields to correct deviation of the circularity of at least one of the image and diffraction pattern; and a deflection portion for deflecting a charged particle beam. 2. The spherical aberration corrector as set forth in claim 1 , wherein said deflection portion adjusts a tilt of said charged particle beam within said at least one of said hexapole fields such that four-fold astigmatism induced by said octopole field is corrected. 3. A spherical aberration corrector for use with a charged particle beam instrument for obtaining an image and a diffraction pattern, said spherical aberration corrector comprising: a hexapole field generating portion for producing plural stages of hexapole fields; a quadrupole field superimposing portion for superimposing a quadrupole field on at least one of the plural stages of hexapole fields to correct deviation of the circularity of at least one of the image and diffraction pattern; and a deflection portion for deflecting a charged particle beam. 4. The spherical aberration corrector as set forth in claim 3 , wherein said deflection portion adjusts a tilt of said charged particle beam within said at least one of said plural stages of hexapole fields such that star aberration induced by said quadrupole field is corrected. 5. A spherical aberration corrector for use with a charged particle beam instrument for obtaining an image and a diffraction pattern, said spherical aberration corrector comprising: a hexapole field generating portion for producing plural stages of hexapole fields; a deflecting field superimposing portion for superimposing a deflecting field on at least one of the plural stages of hexapole fields to correct deviation of the circularity of at least one of the image and diffraction pattern; and a deflection portion for deflecting a charged particle beam. 6. The spherical aberration corrector as set forth in claim 5 , wherein said deflection portion adjusts a tilt of said charged particle beam within said at least one of said plural stages of hexapole fields such that star aberration induced by said deflecting field is corrected. 7. The spherical aberration corrector as set forth in any one of claims 1 to 6 , wherein said hexapole field generating portion has two stages of multipole elements. 8. The spherical aberration corrector as set forth in claim 7 , further comprising transfer lenses disposed between said two stages of multipole elements. 9. A method of spherical aberration correction implemented in a charged particle beam instrument for obtaining an image and a diffraction pattern, said method comprising the steps of: producing plural stages of hexapole fields; superimposing an octopole field on at least one of the hexapole fields to correct deviation of the circularity of at least one of said image and diffraction pattern; and deflecting a charged particle beam to adjust a tilt of the beam within the at least one of the hexapole fields such that four-fold astigmatism induced by the octopole field is corrected. 10. A method of spherical aberration correction implemented in a charged particle beam instrument for obtaining an image and a diffraction pattern, said method comprising the steps of: producing plural stages of hexapole fields; superimposing a quadrupole field on at least one of the hexapole fields to correct deviation of the circularity of at least one of said image and diffraction pattern; and deflecting a charged particle beam to adjust a tilt of the beam within the at least one of the hexapole fields such that star aberration induced by the quadrupole field is corrected. 11. A method of spherical aberration correction implemented in a charged particle beam instrument for obtaining an image and a diffraction pattern, said method comprising the steps of: producing plural stages of hexapole fields; superimposing a deflecting field on at least one of the hexapole fields to correct deviation of the circularity of at least one of said image and diffraction pattern; and deflecting a charged particle beam to adjust a tilt of the beam within the at least one of the hexapole fields such that star aberration induced by the deflecting field is corrected. 12. The method of spherical aberration correction as set forth in any one of claims 9 to 11 , wherein said plural stages of hexapole fields are two stages of hexapole fields. 13. A charged particle beam instrument including a spherical aberration corrector as set forth in any one of claims 1 to 6 .
Diffraction optics {, i.e. systems including a diffractive element being designed for providing a diffractive effect}(G02B27/60 takes precedence) · CPC title
Ion guns · CPC title
Arrangements for deflecting ray or beam · CPC title
having a diffractive optical element [DOE] contributing to image formation, e.g. whereby modulation transfer function MTF or optical aberrations are relevant · CPC title
with scanning beams {(H01J37/268, H01J37/292, H01J37/2955 take precedence)} · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.