Abstract:
The purpose of the present invention is to provide a charged particle ray device which is capable of simply estimating the cross-sectional shape of a pattern. The charged particle ray device according to the present invention acquires a detection signal for each different discrimination condition of an energy discriminator, and estimates the cross-sectional shape of a sample by comparing the detection signal for each discrimination condition with a reference pattern (see FIG. 5).
Abstract:
Provided is a charged particle beam device that enables, even if a visual field includes therein a plurality of regions having different secondary electron emission conditions, the setting of appropriate energy filter conditions adapted to each of these regions. The charged particle beam device is equipped with a detector for detecting charged particles obtained on the basis of scanning, over a sample, a charged particle beam emitted from a charged particle source, and an energy filter for filtering by energy the charged particles emitted from the sample. Index values are determined for the plurality of regions contained within the scanning region of the charged particle beam, and, for each of a plurality of energy filter conditions, differences are calculated between the plurality of index values and the reference index values that have been set for each of the plurality of regions.
Abstract:
Provided is a charged-particle-beam device capable of simultaneously cancelling out a plurality of aberrations caused by non-uniform distribution of the opening angle and energy of a charged particle beam. The charged-particle-beam device is provided with an aberration generation lens for generating an aberration due to the charged particle beam passing off-axis, and a corrective lens for causing the trajectory of the charged particle beam to converge on the main surface of an objective lens irrespective of the energy of the charged particle beam. The main surface of the corrective lens is disposed at a crossover position at which a plurality of charged particle beams having differing opening angles converge after passing through the aberration generation lens.
Abstract:
An object of the present invention is to realize both of the accuracy of measuring the amount of secondary electron emissions and the stability of a charged particle beam image in a charged particle beam device. In a charged particle beam device, extraction of detected signals is started by a first trigger signal, the extraction of the detected signals is completed by a second trigger signal, the detected signals are sampled N times using N (N is a natural number) third trigger signals that equally divide an interval time T between the first trigger signal and the second trigger signal, secondary charged particles are measured by integrating and averaging the signals sampled in respective division times ΔT obtained by equally dividing the interval time T, and the division time ΔT is controlled in such a manner that the measured number of secondary charged particles becomes larger than the minimum number of charged particles satisfying ergodicity.
Abstract:
The scanning charged particle beam microscope according to the present application is characterized in that, in acquiring an image of the FOV (field of view), interspaced beam irradiation points are set, and then, a deflector is controlled so that a charged particle beam scan is performed faster when the charged particle beam irradiates a position on the sample between each of the irradiation points than when the charged particle beam irradiates a position on the sample corresponding to each of the irradiation points (a position on the sample corresponding to each pixel detecting a signal). This allows the effects from a micro-domain electrification occurring within the FOV to be mitigated or controlled.
Abstract:
The scanning electron microscope includes: an electron source; a first deflector for deflecting a primary electron beam emitted from the electron source; a second deflector for focusing the primary electron beam deflected by the first deflector and deflecting a second electron from a sample, which is generated the focused primary electron beam, to the outside of the optical axis; a voltage applying unit for applying a negative voltage to the sample to decelerate the primary electron beam; a spectrometer for dispersing the secondary electron; a detector for detecting the secondary electron passing through the spectrometer; an electrostatic lens provided between the second deflector and the spectrometer; and a voltage control unit that controls the voltage applied to the electrostatic lens based on the negative voltage applied to the sample. The electrostatic lens allows the deflecting action to be overlapped with the converging action.
Abstract:
The charged particle beam application device is provided with a charged particle source and an objective lens that converges charged particle beam generated by the charged particle source onto a sample. In this case, the charged particle beam application device is further provided with an aberration generating element installed between the charged particle beam source and the objective lens, a tilt-use deflector installed between the aberration generating element and the objective lens, a deflection aberration control unit for controlling the aberration generating element, a first electromagnetic field superposing multipole installed between the aberration generating element and the objective lens, and an electromagnetic field superposing multipole control unit for controlling the first electromagnetic field superposing multipole. The aberration generating element has such a function that when the charged particle beam is tilted relative to the sample by the tilt-use deflector, a plurality of resulting aberrations are cancelled with one another. Moreover, the first electromagnetic field superposing multipole has a function to change the orbit of a charged particle beam having energy different from that of the main charged particle beam in the charged particle beam.
Abstract:
An object of the present invention is to provide a method and an apparatus capable of measuring a potential of a sample surface by using a charged particle beam, or of detecting a compensation value of a variation in an apparatus condition which changes due to sample charging, by measuring a sample potential caused by irradiation with the charged particle beam. In order to achieve the object, a method and an apparatus are provided in which charged particle beams (2(a), 2(b)) emitted from a sample (23) are deflected by a charged particle deflector (33) in a state in which the sample (23) is irradiated with a charged particle beam (1), and information regarding a sample potential is detected by using a signal obtained at that time.
Abstract:
There is proposed a charged particle beam device that generates a first signal waveform on the basis of scanning, the number of scanning lines of which is one or more, the scanning intersecting an edge of a pattern on a sample, generates a second signal waveform for a first area that is wider than the one scanning line on the basis of scanning, the number of scanning lines of which is larger than that of scanning for generating the first signal waveform, then determines a deviation between the generated first and second signal waveforms, and thereby determines, from the deviation, correction data used at the time of dimensional measurement.
Abstract:
An objective of the present invention is to provide a charged particle beam device with which information based on a charged particle which is discharged from a bottom part of high-aspect structure is revealed more than with previous technology. To achieve the objective, proposed is a charged particle beam device comprising: a first orthogonal electromagnetic field generator which deflects charged particles which are discharged from a material; a second orthogonal electromagnetic field generator which further deflects the charged particles which are deflected by the first orthogonal electromagnetic field generator; an aperture forming member having a charged particle beam pass-through aperture; and a third orthogonal electromagnetic field generator which deflects the charged particles which have passed through the aperture forming member.