Method of producing a freestanding thin film of nano-crystalline graphite
US-2015151972-A1 · Jun 4, 2015 · US
US2016343536A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2016343536-A1 |
| Application number | US-201515112716-A |
| Country | US |
| Kind code | A1 |
| Filing date | Jan 21, 2015 |
| Priority date | Jan 21, 2014 |
| Publication date | Nov 24, 2016 |
| Grant date | — |
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A method of manipulating an electron beam is disclosed. The method comprises transmitting the beam through a phase mask selected to spatially modulate a phase of the beam over a cross-section thereof.
Opening claim text (preview).
1 . A method of manipulating a particle beam, comprising transmitting the beam through a phase mask selected to spatially modulate a phase of a wavefront of the beam over a cross-section thereof, wherein said phase mask is characterized by a thickness function that does not exceed a critical point in which the accumulated phase equals a predetermined threshold. 2 . The method of claim 1 , wherein said phase modulation is selected to at least partially compensate for aberrations generated by a beam focusing system. 3 . The method according to claim 2 , further comprising applying a multipole electromagnetic field to the beam. 4 . A phase mask, comprising a solid material being transmissive to a particle beam and being patterned such to spatially modulate a phase of a wavefront of said particle beam over a cross-section of said particle beam, the phase mask being characterized by a thickness function that does not exceed a critical point in which the accumulated phase equals a predetermined threshold. 5 . A system for manipulating a particle beam, comprising the phase mask according to claim 4 . 6 . The system of claim 5 , further comprising a beam focusing system, wherein said phase modulation is selected to at least partially compensate for aberrations generated by said beam focusing system. 7 . The system of claim 6 , wherein said beam focusing system is positioned in front or behind said phase mask. 8 . The system of claim 6 , wherein said beam focusing system is integrated with said phase mask. 9 . A particle beam system, comprising a particle beam source and a particle beam manipulation system, wherein said particle beam manipulation system comprises the system according to claim 5 . 10 . The system of claim 9 , being configured as one of a transmission electron microscope system, a scanning electron microscope system, an electron beam tomography (EBT) system, an electron beam lithography system, a spectroscopy system a mass spectroscopy system and a free electron laser system. 11 - 16 . (canceled) 17 . The system according to claim 6 , further comprising an electromagnetic or electrostatic lens. 18 . The system according to claim 6 , wherein said phase mask is selected to provide a predetermined pattern at an image plane of said beam focusing system. 19 . (canceled) 20 . The system according to claim 6 , wherein said phase mask is selected to provide a predetermined pattern at a diffraction plane of said beam focusing system. 21 - 22 . (canceled) 23 . The method according to claim 2 , wherein said aberrations comprise spherical aberrations. 24 . (canceled) 25 . The method according to claim 2 , wherein said aberrations comprise chromatic aberrations. 26 . (canceled) 27 . The method according to claim 2 , wherein said aberrations comprise at least one type of aberrations selected from the group consisting of astigmatism and trefoil. 28 . The method according to claim 1 , wherein said phase mask is discrete. 29 . (canceled) 30 . The method according to claim 1 , wherein said phase mask is continuous. 31 . (canceled) 32 . The method according to claim 1 , wherein said phase mask is characterized by a rectangular lattice. 33 - 34 . (canceled) 35 . The method according to claim 1 , wherein said phase mask is characterized by a non-rectangular lattice. 36 . The method according to claim 1 , wherein a thickness of said phase mask vary across a surface thereof. 37 - 40 . (canceled) 41 . The method according to claim 1 , wherein said predetermined threshold is selected from the group consisting of about π and about 2π. 42 . (canceled) 43 . The method according to claim 1 , wherein said phase mask is a binary thickness phase mask. 44 . The method according to claim 1 , wherein the particle beam is a substantially coherent particle beam. 45 . (canceled)
Contrast, resolution or power of penetration · CPC title
Electron or ion microscopes; Electron or ion diffraction tubes · CPC title
Details · CPC title
Holography or phase contrast, phase related imaging in general, e.g. phase plates · CPC title
Aberrations · CPC title
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