Abstract:
In a particle-optical projection system a pattern is imaged onto a target by means of energetic electrically charged particles. The pattern is represented in a patterned beam of said charged particles emerging from the object plane through at least one cross-over; it is imaged into an image with a given size and distortion. To compensate for the Z-deviation of the image position from the actual positioning of the target (Z denotes an axial coordinate substantially parallel to the optical axis), without changing the size of the image, the system includes a position detector for measuring the Z-position of several locations of the target, and a controller for calculating modifications of selected lens parameters of the final particle-optical lens and controlling said lens parameters according to said modifications.
Abstract:
Particle-optical apparatus are normally embodied with a magnetic or electrostatic lens so as to focus a beam 1 of charged particles onto a sample 8. It is desirable to be able to use these apparatus at different beam energies. It is, however, undesirable that the focus position 9 of the beam, as a result hereof, should shift with respect to the sample 8. Use of a permanent-magnetic material 6 in a magnetic lens has advantages as regards compact construction, but is normally avoided because it is not easily possible to adjust the lens power to match varying beam energies. The invention shows how it is possible to keep constant the focus position 9, independent of the energy of the particles in the beam 1, by combining a magnetic lensnullthat has been furnished with permanent-magnetic materialnullwith an electrostatic lens. The electrostatic lens is embodied in that case as an accelerating lens.
Abstract:
Disclosed is a charged particle optical apparatus, which includes a particle optical arrangement, configured to define a particle beam path for inspecting an object. The object is accommodated in a pressure-controlled interior of a specimen chamber during the inspection of the object. The charged particle optical apparatus further includes a differential pressure module having a differential pressure aperture. A positioning arm is arranged in the specimen chamber for selectively position the differential pressure module within the pressure-controlled interior of the specimen chamber into an operating position in which the particle beam path passes through the differential pressure aperture. The selective positioning includes an advancing movement of the differential pressure module toward the primary particle beam path. The advancing movement is transmitted to the differential pressure module by a track-guided movement of the positioning arm.
Abstract:
An ion implantation apparatus includes: a plurality of units for accelerating an ion beam generated in an ion source; and a plurality of units for adjusting a scan beam and implanting ions into a wafer. A horizontal U-shaped folder type beamline having opposite long straight portions includes the plurality of units for adjusting the scan beam in a long straight portion to have substantially the same length as the ion source and the plurality of units for accelerating the ion beam.
Abstract:
One embodiment relates to a method of automated inspection of scattered hot spot areas on a manufactured substrate using an electron beam apparatus. A stage holding the substrate is moved along a swath path so as to move a field of view of the electron beam apparatus such that the moving field of view covers a target area on the substrate. Off-axis imaging of the hot spot areas within the moving field of view is performed. A number of hot spot areas within the moving field of view may be determined, and the speed of the stage movement may be adjusted based on the number of hot spot areas within the moving field of view. Another embodiment relates to an electron beam apparatus for inspecting scattered areas on a manufactured substrate. Other embodiments, aspects and features are also disclosed.
Abstract:
In one aspect, an ion implantation system is disclosed, which comprises a deceleration system configured to receive an ion beam and decelerate the ion beam at a deceleration ratio of at least 2, and an electrostatic bend disposed downstream of the deceleration system for causing a deflection of the ion beam. The electrostatic bend includes three tandem electrode pairs for receiving the decelerated beam, where each electrode pair has an inner and an outer electrode spaced apart to allow passage of the ion beam therethrough. Each of the electrodes of the end electrode pair is held at an electric potential less than an electric potential at which any of the electrodes of the middle electrode pair is held and the electrodes of the first electrode pair are held at a lower electric potential relative to the electrodes of the middle electrode pair.
Abstract:
Disclosed is a charged particle optical apparatus, which includes a particle optical arrangement, configured to define a particle beam path for inspecting an object. The object is accommodated in a pressure-controlled interior of a specimen chamber during the inspection of the object. The charged particle optical apparatus further includes a differential pressure module having a differential pressure aperture. A positioning arm is arranged in the specimen chamber for selectively position the differential pressure module within the pressure-controlled interior of the specimen chamber into an operating position in which the particle beam path passes through the differential pressure aperture. The selective positioning includes an advancing movement of the differential pressure module toward the primary particle beam path. The advancing movement is transmitted to the differential pressure module by a track-guided movement of the positioning arm.
Abstract:
An image acquisition method and system for use in transmission electron microscopy and capable of providing information about a wide range of frequency range. The method is initiated with setting at least one of the spherical aberration coefficient and chromatic aberration coefficient of the imaging system of the microscope to suppress attenuation of a contrast transfer function due to an envelope function. Then, an image is obtained by the imaging system placed in defocus conditions.
Abstract:
The invention relates to a charged particle lithography system for transferring a pattern onto a target, said system comprising:a target positioning device comprising a target holder having a first side for holding the target,a charged particle optical unit for generating a charged particle beam, modulating said charged particle beam, and directing said charged particle beam towards the first side of the target holder, anda sensor assembly comprising a converter element for converting charged particles which impinge on said converter element into light, wherein the converter element is arranged on said target positioning device, a light sensor for detecting the light, wherein the light sensor is arranged at a distance from said target positioning device, and a light optical lens which is arranged between the converter element and the light sensor for directing light originating from said converter element to said sensor.
Abstract:
A multi-beam apparatus for inspecting or processing a sample with a multitude of focused beams uses a multitude of detectors for detecting secondary radiation emitted by the sample when is irradiated by the multitude of beams. Each detector signal comprises information caused by multiple beams, the apparatus equipped with a programmable controller for processing the multitude of detector signals to a multitude of output signals, using weight factors so that each output signal represents information caused by a single beam. The weight factors are dynamic weight factors depending on the scan position of the beams with respect to the detectors and the distance between sample and detectors.