Abstract:
Provided is a charged particle beam apparatus which includes a charged particle source, a sample table on which a sample is placed, a charged particle beam optical system that includes an objective lens and emits a charged particle beam emitted from the charged particle source onto the sample, a plurality of detectors which detect secondary particles emitted from the sample when being irradiated with the charged particle beam, and a rotation member which magnetically, electrically, or mechanically changes a detected azimuth angle of the secondary particles emitted from the sample.
Abstract:
A lower pole piece of an electromagnetic superposition type objective lens is divided into an upper magnetic path and a lower magnetic path. A voltage nearly equal to a retarding voltage is applied to the lower magnetic path. An objective lens capable of acquiring an image with a higher resolution and a higher contrast than a conventional image is provided. An electromagnetic superposition type objective lens includes a magnetic path that encloses a coil, a cylindrical or conical booster magnetic path that surrounds an electron beam, a control magnetic path that is interposed between the coil and sample, an accelerating electric field control unit that accelerates the electron beam using a booster power supply, a decelerating electric field control unit that decelerates the electron beam using a stage power supply, and a suppression unit that suppresses electric discharge of the sample using a control magnetic path power supply.
Abstract:
A charged-particle-beam device is characterized in having a control value for an aligner coil (29) being determined by: a coil current and an electrode applied-voltage at a control value for objectives (30, 31), which is an electromagnetic-field superposition lens; a control value for image-shift coils (27, 28); and the acceleration voltage of the charged-particle-beam. By doing this, it has become possible to avoid image disturbances that occur on images to be displayed at boundaries between charged areas and non-charged areas, and provide a charged-particle-beam device that obtains clear images without any unevenness in brightness.
Abstract:
In the present invention, a charged particle beam device has a charged particle source (1), a first condenser lens (4) arranged downstream from the charged particle source (1), an aperture (5) arranged downstream from the first condenser lens (4), and a second condenser lens (6) arranged downstream from the aperture (5), wherein, when a sample (12) is to be irradiated at a second charged particle beam amount which is greater than a first charged particle beam amount, the first and second condenser lenses are controlled such that a charged particle beam is formed downstream from the aperture (5), and such that the focal point of the second condenser lens does not vary between the first charged particle beam amount and the second charged particle beam amount.
Abstract:
In order to provide a charged particle beam apparatus capable of high resolution measurement of a sample at any inclination angle, a charged particle beam apparatus for detecting secondary charged particles (115) generated by irradiating a sample (114) with a primary charged particle beam (110) is provided with a beam tilt lens (113) having: a yoke magnetic path member (132) and a lens coil (134) to focus the primary charged particle beam (110) on the sample (114); and a solenoid coil (133) configured to arrange the upper end on the side surface of the yoke magnetic path member (132) and arrange the bottom end between the tip end of the pole piece of the yoke magnetic path member (132) and the sample (114) in order to arbitrarily tilt the primary charged particle beam (110) on the sample (114).
Abstract:
A lower pole piece of an electromagnetic superposition type objective lens is divided into an upper magnetic path and a lower magnetic path. A voltage nearly equal to a retarding voltage is applied to the lower magnetic path. An objective lens capable of acquiring an image with a higher resolution and a higher contrast than a conventional image is provided. An electromagnetic superposition type objective lens includes a magnetic path that encloses a coil, a cylindrical or conical booster magnetic path that surrounds an electron beam, a control magnetic path that is interposed between the coil and sample, an accelerating electric field control unit that accelerates the electron beam using a booster power supply, a decelerating electric field control unit that decelerates the electron beam using a stage power supply, and a suppression unit that suppresses electric discharge of the sample using a control magnetic path power supply.
Abstract:
A lower pole piece of an electromagnetic superposition type objective lens is divided into an upper magnetic path and a lower magnetic path. A voltage nearly equal to a retarding voltage is applied to the lower magnetic path. An objective lens capable of acquiring an image with a higher resolution and a higher contrast than a conventional image is provided. An electromagnetic superposition type objective lens includes a magnetic path that encloses a coil, a cylindrical or conical booster magnetic path that surrounds an electron beam, a control magnetic path that is interposed between the coil and sample, an accelerating electric field control unit that accelerates the electron beam using a booster power supply, a decelerating electric field control unit that decelerates the electron beam using a stage power supply, and a suppression unit that suppresses electric discharge of the sample using a control magnetic path power supply.
Abstract:
In order to provide a charged particle beam apparatus capable of high resolution measurement of a sample at any inclination angle, a charged particle beam apparatus for detecting secondary charged particles (115) generated by irradiating a sample (114) with a primary charged particle beam (110) is provided with a beam tilt lens (113) having: a yoke magnetic path member (132) and a lens coil (134) to focus the primary charged particle beam (110) on the sample (114); and a solenoid coil (133) configured to arrange the upper end on the side surface of the yoke magnetic path member (132) and arrange the bottom end between the tip end of the pole piece of the yoke magnetic path member (132) and the sample (114) in order to arbitrarily tilt the primary charged particle beam (110) on the sample (114).