Abstract:
This invention is a multi-beam charged particle instrument that can simultaneously focus electrons and a variety of positive and negative ions, such as Gallium, Oxygen and Cesium ions, onto the same material target. In addition, the instrument has provision to simultaneously capture the spectrum of both secondary electrons and ions. The highly dispersive, high resolution mass spectrometer portion of the instrument is expected to detect and identify secondary ion species across the entire range of the periodic table, and also record a portion of their emitted energy spectrum. The electron energy spectrometer part of the instrument is designed to acquire the entire range of scattered electrons, from the low energy secondary electrons through to the elastic backscattered electrons.
Abstract:
An aberration-correcting microscopy instrument is provided. The instrument has a first magnetic deflector disposed for reception of a first non-dispersed electron diffraction pattern. The first magnetic deflector is also configured for projection of a first energy dispersed electron diffraction pattern in an exit plane of the first magnetic deflector. The instrument also has an electrostatic lens disposed in the exit plane of a first magnetic deflector, as well as a second magnetic deflector substantially identical to the first magnetic deflector. The second magnetic deflector is disposed for reception of the first energy dispersed electron diffraction pattern from the electrostatic lens. The second magnetic deflector is also configured for projection of a second non-dispersed electron diffraction pattern in a first exit plane of the second magnetic deflector. The instrument also has an electron mirror configured for correction of one or more aberrations in the second non-dispersed electron diffraction pattern. The electron mirror is disposed for reflection of the second non-dispersed electron diffraction patter to the second magnetic deflector for projection of a second energy dispersed electron diffraction pattern in a second exit plane of the second magnetic deflector.
Abstract:
A method and apparatus satisfying growing demands for improving the intensity of implanting ions that impact a semiconductor wafer as it passes under an ion beam. The method and apparatus are directed to the design and combination together of novel magnetic ion-optical transport elements for implantation purposes for combating the disruptive effects of ion-beam induced space-charge forces. The design of the novel optical elements makes possible: (1) Focusing of a ribbon ion beam as the beam passes through uniform or non-uniform magnetic fields; (2) Reduction of the losses of ions comprising a d.c. ribbon beam to the magnetic poles when a ribbon beam is deflected by a magnetic field.
Abstract:
The present invention relates to e.g. a charged particle beam energy width reduction system for a charged particle beam with a z-axis along the optical axis and a first and a second plane, comprising, a first element (110) acting in a focusing and dispersive manner, a second element (112) acting in a focusing and dispersive manner, a first quadrupole element (410) being positioned such that, in operation, a field of the first quadrupole element overlaps with a field of the first element acting in a focusing and dispersive manner, a second quadrupole element (412) being positioned such that, in operation, a field of the second quadrupole element overlaps with a field of the second element acting in a focusing and dispersive manner, a first charged particle selection element (618) being positioned, in beam direction, before the first element acting in a focusing and dispersive manner, and a second charged particle selection element (616;716) being positioned, in beam direction, after the first element acting in a focusing and dispersive manner. Thereby, a virtually dispersive source-like location without an inherent dispersion limitation can be realized.
Abstract:
The present invention provides a charged particle beam energy width reduction system. The system comprises a first element (110) acting in a focusing and dispersive manner in an x-z-plane; a second element (112) acting in a focusing and dispersive manner in the x-z-plane; a charged particle selection element (116; 116a; 116b) positioned between the first and the second element acting in a focusing and dispersive manner; and a focusing element (114; 314, 712; 714) positioned between the first and the second element acting in a focusing and dispersive manner.
Abstract:
A particle optical apparatus including an aperture plate for shaping a particle beam before the particle beam enters a monochromator filter assembly. The aperture plate has at least one aperture and is adjustable with respect to the monochromator filter assembly, in normal operating conditions, so that the size of the aperture used to shape the particle beam can be varied, and therefore the beam current entering the filter assembly can be varied.
Abstract:
An atom probe includes one or more intermediate electrodes between its local electrode and its detector, wherein the intermediate electrode(s) are charged to potentials such that they filter spurious ions and prevent them from reaching the detector, and/or adapt (focus) the flight cone of the ions to have a narrower or wider angle, thereby adjusting the magnification and field of view of the image provide by the atom probe. A preferred arrangement is to provide both filtering electrodes and focusing electrodes which are movable with respect to each other, and which may be telescopically interfit, so as to provide a range of filtering and focusing effects.
Abstract:
The invention relates to an energy filter image generator for filtering electrically charged particles. The inventive energy filter comprises at least two toroidal energy analysers (30, 40) arranged one inside the other. A transfer lens device (20) is disposed between the plane of emergence (5) of the first energy analyser (30) and the plane of incidence of the second energy analyser (40), thereby making it possible to obtain the perfect energy filtered reproduction of the surface (1') of a sample on a detector (10).
Abstract:
An electron beam column includes an electron gun (186), an accelerating region (170), scaning deflectors (160), focusing lenses (150), secondary electron detectors (130), and an asymmetrical detector which is defined by a field-free tube (140) and a voltage contrast plate (120).
Abstract:
An electron beam (4) applied to a specimen (10) is two-dimensionally scanned by a scanning coil (9), and secondary electrons produced from the specimen (10) are detected by a secondary electron detector (13). A deflecting coil (15) for image shifting electrically deflects a primary electron beam to shift the visual field in a given direction by a given distance by image shifting. This image shifting causes energy dispersion of the primary electron beam (4) applied to the specimen, thereby degrading the resolution. However, an ExB field generator (30) for dispersion control provides energy dispersion whose direction is opposite to that caused by the primary electron beam and whose magnitude is equal to that caused by the same, so that the energy dispersion caused by the primary electron beam is automatically corrected by image shifting.