Abstract:
An arrangement and a method for imaging, examining and processing a sample using electrons. The arrangement comprises an electron microscope for providing electrons, a chamber with a sample holder on which a sample is positionable such that it can be imaged, examined and processed using the electrons. A system for magnetic field compensation in at least one spatial direction, including a compensation coil, wherein a wall of the chamber has an accommodation area, in sections thereof, for a portion of the compensation coil. Generally, only the chamber in which the sample is arranged is considered as a compensation volume. It suffice to reduce the compensation volume to the sensitive region of the electron microscope, since it is in the chamber, shortly following a final focusing and filtering, where the electron beam is most sensitive in terms of image quality when subjected to external electromagnetic interference.
Abstract:
A method of making axial alignment of a charged particle beam starts with obtaining at least first through sixth image data while controlling the focal position of the beam on a sample in the direction of incidence, the excitation current in a first alignment coil, and the excitation current in a second alignment coil. Then, values of the excitation currents in the first and second alignment coils for the axial alignment of the beam are calculated from the at least first through sixth image data.
Abstract:
The invention relates to a charged particle multi-beamlet system for exposing a target using a plurality of beamlets. The system has a charged particle source, an aperture array, a beamlet manipulator, a beamlet blanker, and an array of projection lens systems. The charged particle source is configured to generate a charged particle beam. The aperture array is configured to define separate beamlets from the generated beam. The beamlet manipulator is configured to converge groups of the beamlets towards a common point of convergence for each group. The beamlet blanker is configured to controllably blank beamlets in the groups of beamlets. Finally, the array of projection lens systems is configured to project unblanked beamlets of the groups of beamlets on to the surface of the target. The beamlet manipulator is further adapted to converge each of the groups of beamlets towards a point corresponding to one of the projection lens systems.
Abstract:
A charged particle gun alignment assembly for emitting a charged particle beam along an optical axis of a charged particle beam device is described. The charged particle gun alignment assembly is configured to compensate for misalignment of the charged particle beam and includes a charged particle source having an emitter with a virtual source defining a virtual source plane substantially perpendicular to the optical axis; a condenser lens for imaging the virtual source; a final beam limiting aperture adapted for shaping the charged particle beam; and a double stage deflection assembly positioned between the condenser lens and the final beam limiting aperture, wherein the working distance of the condenser lens is 15 mm or less.
Abstract:
An electron beam device comprises: a beam emitter for emitting a primary electron beam; an objective electron lens for focusing the primary electron beam onto a specimen, the objective lens defining an optical axis; a beam separator having a first dispersion for separating a signal electron beam from the primary electron beam; and a dispersion compensation element. The dispersion compensation element has a second dispersion, the dispersion compensation element being adapted for adjusting the second dispersion independently of an inclination angle of the primary beam downstream of the dispersion compensation element, such that the second dispersion substantially compensates the first dispersion. The dispersion compensation element is arranged upstream, along the primary electron beam, of the beam separator.
Abstract:
A charged particle beam writing apparatus includes a stage on which a target object is placed; an emitting unit configured to emit a charged particle beam to the stage side; a blocking unit arranged between the emitting unit and the stage and configured to block the charged particle beam emitted; a deflector having electrodes through which a current flows by applying a voltage and configured to deflect the charged particle beam passing between the electrodes onto the blocking unit by applying a predetermined voltage across the electrodes; an optical axis adjusting unit configured to correct optical axis deviation of the charged particle beam generated by continuously repeating irradiation (beam-ON) of the charged particle beam on a target object and blocking (beam-OFF) of the beam by applying a two-step voltage to the deflector; and a control unit configured to control the optical axis adjusting unit such that an amount of the optical axis deviation is corrected.
Abstract:
An object of the present invention is to provide a charged particle beam apparatus and an alignment method of the charged particle beam apparatus, which make it possible to align an optical axis of a charged particle beam easily even when a state of the charged particle beam changes. The present invention comprises calculation means for calculating a deflection amount of an alignment deflector which performs an axis alignment for an objective lens, a plurality of calculation methods for calculating the deflection amount is memorized in the calculation means, and a selection means for selecting at least one of the calculation methods is provided.
Abstract:
The present invention aims to provide an axis alignment method, astigmatism correction method and SEM for implementing these methods, which can prevent an alignment or correction error attributable to conditions of a specimen. A first aspect is to obtain the difference between the optimal values acquired from an automatic axis alignment result on a standard sample and from each of automatic axis alignment results on a observation target sample, and to correct an optimal value adjusted using the standard sample by use of the difference thus obtained. A second aspect is to acquire an optimal stigmator value (astigmatism correction signal) by using the standard sample, to store the optimal stigmator value as a default value, to add the optimal stigmator value and the default value depending on the height of an observation target sample pattern, and to perform an astigmatism correction on the basis of the resultant stigmator value.
Abstract:
The invention provides a method for patterning a resist coated substrate carried on a stage, where the patterning utilizes a charged particle beam. The method comprises the steps of: moving the stage at a nominally constant velocity in a first direction; while the stage is moving, deflecting the charged particle beam in the first direction to compensate for the movement of the stage, the deflecting including: (a) compensating for an average velocity of the stage; and (b) separately compensating for the difference between an instantaneous position of the stage and a calculated position based on the average velocity. The separately compensating step uses a bandwidth of less than 10 MHz. The invention also provides a deflector control circuit for implementing the separate compensation functions.
Abstract:
An electron beam apparatus with an aberration corrector using multipole lenses is provided. The electron beam apparatus has a scan mode for enabling the operation of the aberration corrector and a scan mode for disabling the operation of the aberration corrector and the operation of each of the aberration corrector, a condenser lens, and the like is controlled such that the object point of an objective lens does not change in either of the scan modes. If a comparison is made between the secondary electron images of a specimen in the two modes, the image scaling factor and the focus remain unchanged and evaluation and adjustment can be performed by distinctly recognizing only the effect of the aberration corrector. This reduces the time required to adjust an optical axis which has been long due to an axial alignment defect inherent in the aberration corrector and an axial alignment defect in a part other than the aberration corrector which are indistinguishably intermingled with each other.