Abstract:
Process and apparatus for varying the deflection of the path of a charged particle beam over a path of length l in a space volume V, where there is a magnetic induction B (x,y,z), wherein a relative displacement of volume V with respect to the beam is produced in such a way as to vary the magnitude .intg.BDl calculated along the path and characterizing the deflection undergone by the beam on passing through volume V. In some of the embodiments rotating magnetic pole pieces are employed to vary the path. Fixed inclined faced pole pieces are also employed.
Abstract:
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.
Abstract:
A deceleration apparatus capable of decelerating a short spot beam or a tall ribbon beam is disclosed. In either case, effects tending to degrade the shape of the beam profile are controlled. Caps to shield the ion beam from external potentials are provided. Electrodes whose position and potentials are adjustable are provided, on opposite sides of the beam, to ensure that the shape of the decelerating and deflecting electric fields does not significantly deviate from the optimum shape, even in the presence of the significant space-charge of high current low-energy beams of heavy ions.
Abstract:
A ion source comprises: a chamber, an injection to inject matter into the chamber, wherein said matter comprises at least a first species, a tip with an apex located in the chamber, wherein the apex has a surface made of a metallic second species, a generator to generate ions of said species, and a regulation system adapted to set operative conditions of the chamber to alternatively generate ions from the gaseous first species, and ions from the non-gaseous metallic second species.
Abstract:
The present disclosure provides for various advantageous methods and apparatus of controlling electron emission. One of the broader forms of the present disclosure involves an electron emission element, comprising an electron emitter including an electron emission region disposed between a gate electrode and a cathode electrode. An anode is disposed above the electron emission region, and a voltage set is disposed above the anode. A first voltage applied between the gate electrode and the cathode electrode controls a quantity of electrons generated from the electron emission region. A second voltage applied to the anode extracts generated electrons. A third voltage applied to the voltage set controls a direction of electrons extracted through the anode.
Abstract:
A cathode operating temperature adjusting method includes acquiring an approximate equation approximating a correlation between an emission current value in an electron beam source using a cathode and an operating temperature of the cathode at which a bias voltage becomes saturated at the emission current, measuring a current density of an electron beam from the cathode when in the state where an n-th emission current value and an n-th cathode operating temperature are set in the electron beam source, determining whether the measured current density is within a first tolerance range, changing the n-th emission current value to an (n+1)th emission current value when the measured current density is not within the first tolerance range, calculating an operating temperature of the cathode corresponding to the (n+1)th emission current value by the approximate equation, and setting the calculated operating temperature, as an (n+1)th cathode operating temperature, in the electron beam source.
Abstract:
An apparatus includes an irradiation device configured to irradiate an object with charged particle beams, a measurement device configured to measure a characteristic of each of charged particle beams, and a controller. The measurement device includes a plate including knife edges, and a sensor configured to detect a charged particle beam incident thereon via the plate. The controller causes one charged particle beam, selected from the charged particle beams, to perform a scan relative to the measurement device so that the one charged particle beam traverses at least two knife edges among the plurality of knife edges, and to generate correction information for correcting a measurement error of the measurement device due to deformation of the plate, based on an output from the sensor upon the scan.
Abstract:
An ion beam system comprises a voltage supply system 7 and at least one beam deflector 39 having a plurality of first defection electrodes 51a, 51b, 51c and a plurality of second deflection electrodes 52a, 52b, 52c wherein the voltage supply system is configured to supply different adjustable deflection voltages to the plurality of second deflection electrodes such that electric deflection fields between the plurality of second deflection electrodes and the plurality of opposite first deflection electrodes have a common orientation. The ion beam system has a high kinetic energy mode in which a distribution of the electric deflection fields has a greater width, and a low kinetic energy mode in which a distribution of the electric deflection fields has a smaller width.
Abstract:
An improved method of directing a charged particle beam that compensates for the time required for the charged particles to traverse the system by altering one or more of the deflector signals. According to one embodiment of the invention, a digital filter is applied to the scan pattern prior to digital-to-analog (D/A) conversion in order to reduce or eliminate over-shoot effects that can result from TOF errors. In other embodiments, analog filters or the use of signal amplifiers with a lower bandwidth can also be used to compensate for TOF errors. By altering the scan pattern, over-shoot effects can be significantly reduced or eliminated.
Abstract:
The present invention relates to a projection lens assembly module for directing a multitude of charged particle beamlets onto an image plane located in a downstream direction, and a method for assembling such a projection lens assembly. In particular the present invention discloses a modular projection lens assembly with enhanced structural integrity and/or increased placement precision of its most downstream electrode.