Disclosed herein is a composite charged particle beam apparatus including a focused ion beam column and an electron beam column, the apparatus preventing the electron beam column from being contaminated so as to emit an electron beam with high precision. The apparatus includes: a sample tray on which a sample is placed; a focused ion beam column irradiating the sample by using a focused ion beam; an electron beam column irradiating the sample by using an electron beam; a sample chamber receiving the sample tray, and the columns therein; an anti-contamination plate moving between an inserted position inserted into a space between a beam emission surface of the electron beam column and the sample tray, and an open position withdrawn from the space between the beam emission surface and the sample tray; and an operation unit operating the anti-contamination plate to move between the positions.

A charged particle detector with high detection efficiency is presented in this patent. This charged particle detector contains a grid electrode used for attracting charged particles, a convertor with the shape of particle entrance area smaller than the particle exit area, which is used for converging charged particles and converting ions into electrons in the ion detection mode, an electron detection unit used for detecting secondary electrons and amplifying the signal detected, and a metal shielding. This optimized detector has a simple construction, is easy to assemble and has a low manufacturing cost.

During electron beam imaging of a semiconductor wafer, the electron beam is adjusted to a first electron dose/nm.sup.2/time value below a damage threshold for an image frame grab of a site on the semiconductor wafer. Then the electron beam is adjusted to a second electron dose/nm.sup.2/time value different from the first electron dose/nm.sup.2/time value for a second image frame grab of the site. The second electron dose/nm.sup.2/time value can be above the damage threshold.

A multi-beam apparatus for observing a sample with oblique illumination is proposed. In the apparatus, a new source-conversion unit changes a single electron source into a slant virtual multi-source array, a primary projection imaging system projects the array to form plural probe spots on the sample with oblique illumination, and a condenser lens adjusts the currents of the plural probe spots. In the source-conversion unit, the image-forming means not only forms the slant virtual multi-source array, but also compensates the off-axis aberrations of the plurality of probe spots. The apparatus can provide dark-field images and/or bright-field images of the sample.

An improved charged particle beam inspection apparatus, and more particularly, a particle beam inspection apparatus including an improved alignment mechanism is disclosed. An improved charged particle beam inspection apparatus may include a second electron detection device to generate one or more images of one or more beam spots of the plurality of secondary electron beams during the alignment mode. The beam spot image may be used to determine the alignment characteristics of one or more of the plurality of secondary electron beams and adjust a configuration of a secondary electron projection system.

A scanning electron microscope includes a spin detector configured to measure secondary electron spin polarization of secondary electrons emitted from the sample, and an analysis device configured to analyze secondary electron spin polarization data measured by the spin detector. The analysis device evaluates the strain in the sample by calculating a difference in the secondary electron spin polarization data of adjacent pixels.

A computing unit generates a to-be-used-in-computation netlist on the basis of a to-be-used-in-calculation device model corresponding to a correction sample, estimates a first application result, on the basis of the to-be-used-in-computation netlist and an optical condition, when a charged particle beam is applied to the correction sample under the optical condition, compares the first application result and a second application result based on a detection signal when the charged particle beam is applied to the correction sample under the optical condition, and corrects the optical condition when the first application result and the second application result differ from each other.

A computing unit generates a to-be-used-in-computation netlist on the basis of a to-be-used-in-calculation device model corresponding to a correction sample, estimates a first application result, on the basis of the to-be-used-in-computation netlist and an optical condition, when a charged particle beam is applied to the correction sample under the optical condition, compares the first application result and a second application result based on a detection signal when the charged particle beam is applied to the correction sample under the optical condition, and corrects the optical condition when the first application result and the second application result differ from each other.

A scanning electron microscope includes a spin detector configured to measure secondary electron spin polarization of secondary electrons emitted from the sample, and an analysis device configured to analyze secondary electron spin polarization data measured by the spin detector. The analysis device evaluates the strain in the sample by calculating a difference in the secondary electron spin polarization data of adjacent pixels.

An electron beam device obtains contrast reflecting an electronic state of a sample with high sensitivity. The device includes an electron optical system which emits an electron beam to a sample and detects electrons emitted from the sample; a light pulse emission system that emits a light pulse to the sample; a synchronization processing unit that samples the emitted electrons; an image signal processing unit which forms an image by a detection signal output based upon the emitted electrons detected by the electron optical system; and a device control unit for setting a control condition of the electron optical system. The device control unit sets a sampling frequency for detection sampling of the emitted electrons to be greater than a value obtained by dividing the number of emissions of the light pulse per unit pixel time by the unit pixel time.