Patent classifications
H01J37/28
Electron Microscope and Method of Correcting Aberration
Prior to execution of primary correction, a first centering process, an in-advance correction of a particular aberration, and a second centering process are executed stepwise. In the first centering process and the second centering process, a ronchigram center is identified based on a ronchigram variation image, and is matched with an imaging center. In the in-advance correction and the post correction of the particular aberration, a particular aberration value is estimated based on a ronchigram, and the particular aberration is corrected based on the particular aberration value.
LATERAL RECESS MEASUREMENT IN A SEMICONDUCTOR SPECIMEN
There is provided a system and method of measuring a lateral recess in a semiconductor specimen, comprising: obtaining a first image acquired by collecting SEs emitted from the surface of the specimen, and a second image acquired by collecting BSEs scattered from an interior region of the specimen between the surface and a target second layer, the specimen scanned using an electron beam with a landing energy selected to penetrate to a depth corresponding to the target second layer; generating a first GL waveform based on the first image, and a second GL waveform based on the second image; estimating a first width of the first layers based on the first GL waveform, and a second width with respect to at least the target second layer based on the second GL; and measuring a lateral recess based on the first width and the second width.
LATERAL RECESS MEASUREMENT IN A SEMICONDUCTOR SPECIMEN
There is provided a system and method of measuring a lateral recess in a semiconductor specimen, comprising: obtaining a first image acquired by collecting SEs emitted from the surface of the specimen, and a second image acquired by collecting BSEs scattered from an interior region of the specimen between the surface and a target second layer, the specimen scanned using an electron beam with a landing energy selected to penetrate to a depth corresponding to the target second layer; generating a first GL waveform based on the first image, and a second GL waveform based on the second image; estimating a first width of the first layers based on the first GL waveform, and a second width with respect to at least the target second layer based on the second GL; and measuring a lateral recess based on the first width and the second width.
TEMPERATURE-CONTROLLED SURFACE WITH A CRYO-NANOMANIPULATOR FOR IMPROVED DEPOSITION RATE
A method of depositing material over a sample in a deposition region of the sample with a charged particle beam column, the method comprising: positioning a sample within a vacuum chamber such that the deposition region is under a field of view of the charged particle beam column; cooling the deposition region by contacting the sample with a cyro-nanomanipulator tool in an area adjacent to the deposition region; injecting a deposition precursor gas into the vacuum chamber at a location adjacent to the deposition region; generating a charged particle beam with a charged particle beam column and focusing the charged particle beam on the sample; and scanning the focused electron beam across the localized region of the sample to activate molecules of the deposition gas that have adhered to the sample surface in the deposition region and deposit material on the sample within the deposition region
TEMPERATURE-CONTROLLED SURFACE WITH A CRYO-NANOMANIPULATOR FOR IMPROVED DEPOSITION RATE
A method of depositing material over a sample in a deposition region of the sample with a charged particle beam column, the method comprising: positioning a sample within a vacuum chamber such that the deposition region is under a field of view of the charged particle beam column; cooling the deposition region by contacting the sample with a cyro-nanomanipulator tool in an area adjacent to the deposition region; injecting a deposition precursor gas into the vacuum chamber at a location adjacent to the deposition region; generating a charged particle beam with a charged particle beam column and focusing the charged particle beam on the sample; and scanning the focused electron beam across the localized region of the sample to activate molecules of the deposition gas that have adhered to the sample surface in the deposition region and deposit material on the sample within the deposition region
CHARGED PARTICLE ASSESSMENT TOOL, INSPECTION METHOD
A multi-beam electron-optical system for a charged-particle assessment tool, the system comprising: a plurality of control lenses, a plurality of objective lenses and a controller. The plurality of control lenses are configured to control a parameter of a respective sub-beam. The plurality of objective lenses are configured to project one of the plurality of charged-particle beams onto a sample. The controller controls the control lenses and the objective lenses so that the charged particles are incident on the sample with a desired landing energy, demagnification and/or beam opening angle.
CHARGED PARTICLE ASSESSMENT TOOL, INSPECTION METHOD
A multi-beam electron-optical system for a charged-particle assessment tool, the system comprising: a plurality of control lenses, a plurality of objective lenses and a controller. The plurality of control lenses are configured to control a parameter of a respective sub-beam. The plurality of objective lenses are configured to project one of the plurality of charged-particle beams onto a sample. The controller controls the control lenses and the objective lenses so that the charged particles are incident on the sample with a desired landing energy, demagnification and/or beam opening angle.
METHODS FOR ANALYZING INTERMOLECULAR INTERACTIONS IN MICROCRYSTALS
Methods of introducing a small molecule into a crystal of a macromolecule, of obtaining a microcrystal having a macromolecule and a small molecule from a crystal of the macromolecule, of determining a structural model for a complex having a macromolecule and a small molecule, of identifying a small molecule that complexes with a macromolecule, and of screening a library of small molecules for their binding to a macromolecule are disclosed.
CHARGED PARTICLE BEAM DEVICE, AND METHOD FOR ADJUSTING IMAGE CAPTURING CONDITIONS IN SAID CHARGED PARTICLE BEAM DEVICE
This charged particle beam device comprises: a charged particle beam source that generates charged particle beams; an objective lens in which coil current is inputted to focus the charged particle beams on a sample; a control unit that controls the coil current; a hysteresis characteristics storage unit that stores hysteresis characteristics information of the objective lens; a history information storage unit that stores history information relating to the coil current; and an estimating unit that estimates the magnetic field generated by the objective lens based on the coil current, the history information, and the hysteresis characteristic information, and has a magnetic field correction unit that, when the absolute value of the change amount of the coil current is greater than a prescribed value, further adds to the magnetic field estimated by the estimating unit a correction value according to the coil current and its change amount, correcting the magnetic field generated by the objective lens.
CHARGED PARTICLE BEAM DEVICE, AND METHOD FOR ADJUSTING IMAGE CAPTURING CONDITIONS IN SAID CHARGED PARTICLE BEAM DEVICE
This charged particle beam device comprises: a charged particle beam source that generates charged particle beams; an objective lens in which coil current is inputted to focus the charged particle beams on a sample; a control unit that controls the coil current; a hysteresis characteristics storage unit that stores hysteresis characteristics information of the objective lens; a history information storage unit that stores history information relating to the coil current; and an estimating unit that estimates the magnetic field generated by the objective lens based on the coil current, the history information, and the hysteresis characteristic information, and has a magnetic field correction unit that, when the absolute value of the change amount of the coil current is greater than a prescribed value, further adds to the magnetic field estimated by the estimating unit a correction value according to the coil current and its change amount, correcting the magnetic field generated by the objective lens.