Abstract:
An aberration computing device (100) includes a fitting section (48) for fitting line profiles of a diffractogram taken in radial directions to a fitting function and finding fitting parameters of the fitting function and a computing section (49) for finding at least one of an amount of defocus and two-fold astigmatism, based on the fitting parameters.
Abstract:
An aberration computing device (100) includes a fitting section (48) for fitting line profiles of a diffractogram taken in radial directions to a fitting function and finding fitting parameters of the fitting function and a computing section (49) for finding at least one of an amount of defocus and two-fold astigmatism, based on the fitting parameters.
Abstract:
A method of adjusting a charged particle optical system in a charged particle beam apparatus provided with the charged particle optical system including an aberration corrector in which multipole elements disposed in three or more stages and transfer optical systems are alternately disposed. The method includes adjusting aberration using at least two of the multipole elements without using at least one of the multipole elements, and adjusting parameters of the charged particle optical system other than aberration using at least one of the transfer optical systems that is not disposed between the at least two of the multipole elements used.
Abstract:
A method of measuring an aberration in an electron microscope includes: acquiring an image for measuring the aberration in the electron microscope; and measuring the aberration by using the image. In measuring the aberration, a direction of defocusing is specified based on a residual aberration that is uniquely determined by a configuration of an optical system of the electron microscope and an optical condition of the optical system.
Abstract:
A method of measuring an aberration in an electron microscope includes: acquiring an image for measuring the aberration in the electron microscope; and measuring the aberration by using the image. In measuring the aberration, a direction of defocusing is specified based on a residual aberration that is uniquely determined by a configuration of an optical system of the electron microscope and an optical condition of the optical system.
Abstract:
An aberration corrector includes: a first multipole, a second multipole, a third multipole, and a fourth multipole arranged along an optical axis A; a first transfer lens system arranged between the first multipole and the second multipole; a second transfer lens system arranged between the second multipole and the third multipole; and a third transfer lens system arranged between the third multipole and the fourth multipole, wherein each of the first multipole, the second multipole, the third multipole, and the fourth multipole generates a three-fold symmetric field.
Abstract:
There are disclosed an aberration correction method and a charged particle beam system capable of correcting off-axis first order aberrations. The aberration correction method is for use in the charged particle beam system (100) equipped with an aberration corrector (30) which has plural stages of multipole elements (32a, 32b) and a transfer lens system (34) disposed between the multipole elements (32a, 32b). The method includes varying the excitation of the transfer lens system (34) and correcting off-axis first order aberrations.
Abstract:
There is provided an electron microscope capable of reducing variations of aberrations due to thermal variations. The electron microscope includes an electron optical system having a built-in aberration corrector equipped with multipole elements each for producing a multipolar field. Each multipole element includes a plurality of magnetic polepieces. Each polepiece includes a magnetic core, a first coil wound around the core, and a second coil wound around the core. The first coil and the second coil produce a first multipolar field and a second multipolar field, respectively, when energized. The first and second multipolar fields are identical in terms of symmetry.
Abstract:
An electron microscope includes an irradiation optical system that focuses electron beams and scans a specimen with the focused electron beams; a deflector that deflects the electron beams transmitted through the specimen; a detector that detects the electron beams transmitted through the specimen; and a control unit that controls the irradiation optical system and the deflector The control unit causes the irradiation optical system to scan the specimen with the electron beams so that the electron beams have a plurality of irradiation positions on the specimen. The control unit causes the deflector to repeatedly deflect the electron beams transmitted through each of the irradiation positions, so that a plurality of electron beams which have the same irradiation position and different incident angle ranges with respect to the specimen are caused to sequentially enter the detector.
Abstract:
In a scanning transmission electron microscope, a control unit performs: processing of calculating a first auto-correlation function that is an auto-correlation function of a first scanning transmission electron microscope image; processing of acquiring a first intensity profile along a straight line that passes through a center of the first auto-correlation function; processing of obtaining a position of an inflection point that is closest to the center of the first auto-correlation function in the first intensity profile and adopting an intensity at the position as a first reference intensity; processing of obtaining an aberration coefficient by fitting a first aberration function to an isointensity line that connects positions where intensity is equal to the first reference intensity in the first auto-correlation function and by fitting a second aberration function to an isointensity line that connects positions where intensity is equal to a second reference intensity in a second auto-correlation function; and processing of controlling an electron optical system based on the aberration coefficient.