Abstract:
Methods of inspecting a microstructure comprise: applying charged particles to the wafer to negatively charge up the wafer over a region having contact or via holes, scanning a charged-particle beam over the region while detecting secondary particles so as to produce a detector signal, determining from the detector signal an apparent dimension of a contact hole, and comparing the apparent dimension of the contact hole with reference information to identify a defect. The reference information can be a conventional voltage-contrast image or can be design data indicating expected physical size of the contact hole and expected electrical connectivity of material within or beneath the contact hole. The wafer can be charged up by directing a flood of electrons toward a surface of the wafer and/or by controlling potential of an energy filter so as to direct secondary electrons back to the wafer while directing a charged-particle beam at the wafer. Other methods of inspecting a microstructure comprise charging up a microstructure, interrogating the microstructure with a charged-particle beam to obtain apparent dimensional information for a feature of the microstructure, and comparing the apparent dimensional information with reference information about the microstructure to identify a defect. Apparatus for inspecting semiconductor wafers and other microstructures are also disclosed, as are computer program products comprising a computer usable media having computer-readable program code embodied therein for controlling a charged-particle-beam system for inspecting a microstructure.
Abstract:
An electron beam, which can transmit through part of a specimen and can reach a portion that is not exposed to the electron beam, is irradiated, and a scanning image is obtained on the basis of a signal secondarily generated from a portion irradiated with the electron beam. Dimension-measuring start and end points are set on the scanning image and a dimension therebetween is measured. A three-dimensional model is assumed, the three-dimensional model is modified so as to match the scanning image, and dimension measurement is carried out on the basis of a modified three-dimensional model.
Abstract:
In order to allow detecting backscattered electrons (BSEs) generated from the bottom of a hole for determining whether a hole with a super high aspect ratio is opened or for inspecting and measuring the ratio of the top diameter to the bottom diameter of a hole, which are typified in 3D-NAND processes of opening a hole, a primary electron beam accelerated at a high accelerating voltage is applied to a sample. Backscattered electrons (BSEs) at a low angle (e.g. a zenith angle of five degrees or more) are detected. Thus, the bottom of a hole is observed using “penetrating BSEs” having been emitted from the bottom of the hole and penetrated the side wall. Using the characteristics in which a penetrating distance is relatively prolonged through a deep hole and the amount of penetrating BSEs is decreased to cause a dark image, a calibration curve expressing the relationship between a hole depth and the brightness is given to measure the hole depth.
Abstract:
In an SEM provided with an ExB deflector for deflecting secondary electrons outside an optical axis of a primary electron beam between an electronic source and an object lens for condensing the primary electron beam and irradiating a sample with the beam, a unit to decelerate the secondary electrons deflected in the ExB deflector, and a magnetic generator for deflecting the decelerated secondary electron are provided, and a plurality of energy filters and detectors are arranged around the magnetic generator. That is, by separating loci of the secondary electrons incident on the energy filters and of the secondary electrons reflected at the energy filters by the magnetic generator, both of the secondary electrons are concurrently detected.
Abstract:
A seamless mold manufacturing method of the invention is a seamless mold manufacturing method having the steps of forming a thermal reaction type resist layer on a sleeve-shaped mold, and exposing using a laser and developing the thermal reaction type resist layer and thereby forming a fine mold pattern, and is characterized in that the thermal reaction type resist layer is comprised of a thermal reaction type resist having a property of reacting in predetermined light intensity or more in a light intensity distribution in a spot diameter of the laser.
Abstract:
Provided is a sample observation apparatus including a charged particle optical column that, irradiates a sample including an observation target portion that is a concave portion with a charged particle beam at an acceleration voltage, an image generation section that acquires an image including the observation target portion from a signal acquired with irradiation of the charged particle beam, a storage section that stores information representing a relationship between a brightness ratio of a concave portion and its neighboring portion of a reference sample that is irradiated with the charged particle beam at the acceleration voltage and a value that represents a structure of the concave portions of the reference sample in advance, a calculation section that acquires a brightness ratio of the concave portion and its neighboring portion of the image, and a determination section that determines whether or not a defect occurs in the observation target portion based on the information that represents the relationship and the brightness ratio of the image.
Abstract:
A system, method and a non-transitory compute readable medium for evaluating a high aspect ratio (HAR) hole having a nanometric scale width and formed in a substrate, including obtaining, during an illumination period, multiple measurement results by an electrostatic measurement device that comprises a probe tip that is placed in proximity to the HAR hole; wherein multiple locations within the HAR hole are illuminated with a beam of charged particles during the illumination period; and processing the multiple measurement results to determine a state of the HAR hole.
Abstract:
A charged particle beam device is described. In one aspect, the charged particle beam device includes a charged particle beam source, and a switchable multi-aperture for generating two or more beam bundles from a charged particle beam which includes: two or more aperture openings, wherein each of the two or more aperture openings is provided for generating a corresponding beam bundle of the two or more beam bundles; a beam blanker arrangement configured for individually blanking the two or more beam bundles; and a stopping aperture for blocking beam bundles. The device further includes a control unit configured to control the individual blanking of the two or more beam bundles for switching of the switchable multi-aperture and an objective lens configured for focusing the two or more beam bundles on a specimen or wafer.
Abstract:
The pattern observation method for observing a pattern which is formed on an insulating film, includes: irradiating an entirety of the pattern with a charged particle beam, to obtain a temporary image of the pattern which has region information of a convex pattern and a concave pattern; irradiating the convex and concave patterns with the charged particle beam having a first and second voltages based on the region information, to thereby form an electric field between a top surface of the convex pattern and a bottom surface of the concave pattern so that charged particles emitted from the bottom surface of the concave pattern may be drawn out to an outside of the pattern; and irradiating the entirety of the pattern with the charged particle beam to obtain an image of the pattern having the information of the bottom surface of the concave pattern.
Abstract:
As an aspect for realizing accurate observation, inspection, or measurement of the contact hole with large aspect ratio, a method and a device to scan a second electron beam after scanning a first electron beam to a sample to charge the sample are proposed wherein the beam diameter of the first electron beam is made larger than the beam diameter of the second electron beam.