Abstract:
A system for ion beam neutralization includes a beamguide configured to transport an ion beam through a dipole field, a first array of magnets and a second array of magnets configured to generate a multi-cusp magnetic field, the first array of magnets being on a first side of the ion beam path and the second array of magnets being on a second side of the ion beam path. The system may further include a charged particle source having one or more apertures configured to inject charged particles into the ion beam. The system may furthermore align the one or more apertures with at least one of the first array of magnets and the second array of magnets to align the injected charged particles from the charged particle source with one or more magnetic regions for an effective charged particle diffusion into the ion beam.
Abstract:
A method and a device for determining the distance from the sample to be examined to at least one reference point which function independently of the type of sample. A signal is modulated to a first potential of a sample and a primary particle beam is directed at the sample, resulting in a secondary particle beam being formed by an interaction, the particles of this beam having the modulated signal. The particles of the secondary particle beam and the signal modulated to the potential of the particles of the secondary particle beam are detected. By comparing the detected modulated signal to a reference signal, the distance is determined from the relationship between the reference signal and the detected modulated signal. The device has the corresponding components for implementing the method.
Abstract:
Provided is a charged particle beam processing apparatus capable of improving yields by suppressing the spread of metal pollution to a semiconductor manufacturing process to a minimum. The charged particle beam processing apparatus includes an ion beam column 1 that is connected to a vacuum vessel 10 and irradiates a sample 35 with an ion beam 11 of nonmetal ion species, a microsampling unit 3 having a probe 16 that extracts a microsample 43 cut out from a sample 35 by the ion beam 11, a gas gun 2 that discharges a gas for bonding the microsample 43 and the probe 16, a pollution measuring beam column 6A that is connected to the same vacuum vessel 10 to which the ion beam column 1 is connected and irradiates an ion beam irradiation traces by the ion beam column 1 with a pollution measuring beam 13, and a detector 7 that detects characteristic X-rays emitted from the ion beam irradiation traces by the ion beam column 1 upon irradiation with the pollution measuring beam 13.
Abstract:
There is disclosed an electron microscope that achieves low-magnification imaging while the objective lens is kept at high excitation in the same way as during high-magnification imaging. An objective minilens located immediately behind the objective lens demagnifies a specimen image magnified by the objective lens. Consequently, a sharply focused electron beam enters the first intermediate lens. This greatly reduces the effects of off-axis aberrations in the intermediate lenses. The first, second, and third intermediate lenses create a crossover image and a microscope image in the entrance window plane and entrance image plane, respectively, of an energy filter. The energy filter focuses the microscope image and crossover image onto the exit image plane and exit window plane, respectively. The output image from the filter is projected onto the final image plane by first and second projector lenses.
Abstract:
An imaging system that selectively alternates between a first, non-destructive imaging mode and a second, destructive imaging mode to analyze a specimen so as to determine an atomic structure and composition of the specimen is provided. The field ionization mode can be used to acquire first images of ionized atoms of an imaging gas present in a chamber having the specimen disposed therein, and the field evaporation mode can be used to acquire second images of ionized specimen atoms evaporated from a surface of the specimen with the imaging gas remaining in the chamber. The first and second image data can be analyzed in real time, during the specimen analysis, and results can be used to dynamically adjust operating parameters of the imaging system.
Abstract:
When an electrode (29) such as a grid applied with a negative voltage is installed in front of an objective lens (23), low energy electrons among secondary electrons (25) generated from a sample (24) by an electron beam or the like is reflected by the electrode to come into a detector (22) installed in the sample (24) side, while electrons of higher energy are not detected, since they are not reflected by the electrode. Accordingly, since only the electrons of lower energy of the secondary electrons can be detected by discriminating the secondary electrons by the energy, it is possible to obtain a detection signal, e.g., rich in the information on the surface state of the sample.
Abstract:
An imaging system that selectively alternates a first, non-destructive imaging mode and a second, destructive imaging mode to analyze a specimen so as to determine an atomic structure and composition of the specimen is provided. The field ionization mode can be used to acquire first images of ionized atoms of an imaging gas present in a chamber having the specimen disposed therein, and the field evaporation mode can be used to acquire second images of ionized specimen atoms evaporated from a surface of the specimen with the imaging gas remaining in the chamber. The first and second image data can be analyzed in real time, during the specimen analysis, and results can be used to dynamically adjust operating parameters of the imaging system.
Abstract:
A laser atom probe system and a method for analysing a specimen by laser atom probe tomography are disclosed. The system includes a specimen holder whereon a specimen to be analyzed may be mounted, the specimen having a tip shape. The system further includes a detector, an electrode arranged between the specimen holder and the detector, and a voltage source configured to apply a voltage difference between the specimen tip and the electrode. The system also includes at least one laser system configured to direct a laser beam laterally at the specimen tip and a tip shape monitoring means configured to detect and monitor the tip shape, and/or a means for altering and/or controlling one or more laser parameters of said laser beam(s) so as to maintain, restore or control said specimen tip shape.
Abstract:
A detector system for a transmission electron microscope includes a first detector for recording a pattern and a second detector for recording a position of a feature of the pattern. The second detector is preferably a position sensitive detector that provides accurate, rapid position information that can be used as feedback to stabilize the position of the pattern on the first detector. In one embodiment, the first detector detects an electron energy loss electron spectrum, and the second detector, positioned behind the first detector and detecting electrons that pass through the first detector, detects the position of the zero-loss peak and adjusts the electron path to stabilize the position of the spectrum on the first detector.
Abstract:
There is disclosed an electron microscope that achieves low-magnification imaging while the objective lens is kept at high excitation in the same way as during high-magnification imaging. An objective minilens located immediately behind the objective lens demagnifies a specimen image magnified by the objective lens. Consequently, a sharply focused electron beam enters the first intermediate lens. This greatly reduces the effects of off-axis aberrations in the intermediate lenses. The first, second, and third intermediate lenses create a crossover image and a microscope image in the entrance window plane and entrance image plane, respectively, of an energy filter. The energy filter focuses the microscope image and crossover image onto the exit image plane and exit window plane, respectively. The output image from the filter is projected onto the final image plane by first and second projector lenses.