Abstract:
To improve the workability of the task of adjusting the position of a limit field diaphragm. An electron microscope provided with an image-capturing means for capturing an image of an observation visual field prior to insertion of a limit field diaphragm as a map image, a recording means for recording the map image, an extraction means for capturing an image of the observation visual field after insertion of the limit field diaphragm and extracting the outline of the diaphragm, a drawing means for drawing the outline on the map image, and a display means for displaying the image drawn by the drawing means.
Abstract:
In one embodiment, a charged particle beam drawing apparatus deflects a charged particle beam with a deflector to draw a pattern. The apparatus includes a storage unit that stores an approximate formula indicating a correspondence relationship between a settling time for a DAC amplifier that controls the deflector, and a position shift amount, from a design position, of a drawn position of each evaluation pattern drawn on a first substrate while the settling time and an amount of deflection by the deflector are changed, a shot position correction unit that creates a correction formula indicating a relationship between an amount of deflection and a shot position shift amount at the settling time, from the approximate formula and the settling time for the DAC amplifier based on an amount of deflection of a shot, obtains a position correction amount by using the amount of deflection of the shot and the correction formula, and corrects a shot position defined by the shot data based on the position correction amount, and a drawing unit that performs drawing by using the shot data with a corrected shot position.
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 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:
A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit forms plural and parallel images of one single electron source by deflecting plural beamlets of a parallel primary-electron beam therefrom, and one objective lens focuses the plural deflected beamlets onto a sample surface and forms plural probe spots thereon. A movable condenser lens is used to collimate the primary-electron beam and vary the currents of the plural probe spots, a pre-beamlet-forming means weakens the Coulomb effect of the primary-electron beam, and the source-conversion unit minimizes the sizes of the plural probe spots by minimizing and compensating the off-axis aberrations of the objective lens and condenser lens.
Abstract:
This scanning electron microscope is provided with: a deceleration means that decelerates an electron beam (5) when the electron beam is passing through an objective lens; and a first detector (8) and a second detector (7) that are disposed between the electron beam and the objective lens and have a sensitive surface having an axially symmetric shape with respect to the optical axis of the electron beam. The first detector is provided at the sample side with respect to the second detector, and exclusively detects the signal electrons having a high energy that have passed through a retarding field energy filter (9A). When the distance between the tip (13) at the sample side of the objective lens and the sensitive surface of the first detector is L1 and the distance between the tip at the sample side of the objective lens and the sensitive surface of the second detector is L2, then L1/L2≦5/9. As a result, when performing low-acceleration observation using a deceleration method by means of a scanning electron microscope, it is possible to detect signal electrons without the effect of shading in a magnification range of a low magnification on the order of hundreds of times to a high magnification of at least 100,000×. Also, it is possible to highly efficiently detect backscattered electrons, of which the amount generated is less than that of secondary electrons.
Abstract:
This scanning electron microscope is provided with: a deceleration means that decelerates an electron beam (5) when the electron beam is passing through an objective lens; and a first detector (8) and a second detector (7) that are disposed between the electron beam and the objective lens and have a sensitive surface having an axially symmetric shape with respect to the optical axis of the electron beam. The first detector is provided at the sample side with respect to the second detector, and exclusively detects the signal electrons having a high energy that have passed through a retarding field energy filter (9A). When the distance between the tip (13) at the sample side of the objective lens and the sensitive surface of the first detector is L1 and the distance between the tip at the sample side of the objective lens and the sensitive surface of the second detector is L2, then L1/L2≦5/9. As a result, when performing low-acceleration observation using a deceleration method by means of a scanning electron microscope, it is possible to detect signal electrons without the effect of shading in a magnification range of a low magnification on the order of hundreds of times to a high magnification of at least 100,000×. Also, it is possible to highly efficiently detect backscattered electrons, of which the amount generated is less than that of secondary electrons.
Abstract:
Apparatus having a magnetic lens configured to diverge an electron beam are useful in three-dimensional imaging using an electron microscope. The magnetic lens includes a body member having a core and defining a gap, and a winding surrounding a portion of the core. The body member and winding are configured such that an electrical current through the winding produces a magnetic field proximate to the gap.
Abstract:
A device for deflecting a particle beam out of a beam axis, or for guiding a particle beam into the beam axis, has a simple design, requires little space, and additionally ensures that no area of an object that is not to be struck is struck by a particle beam. The device may include components in the following sequence along the beam axis: first deflection element, a magnetic apparatus for providing a magnetic field axially to the beam axis, and a second deflection element. A particle beam apparatus may have a device of this type.
Abstract:
Deflectors are disclosed that are suitable for use in various charged-particle-beam (CPB) optical systems as used, for example, in CPB microlithography systems. The deflectors produce a strong magnetic beam-deflecting field when energized with a relatively small electrical current. The beam-deflecting field thus produced is stable with respect to temperature changes, is little affected by eddy currents, and exhibits low aberration caused by manufacturing tolerances of the coil and core. In an exemplary method for manufacturing such a deflector, a magnetic-tape laminate is used as the core. Also, high-precision positioning of the coil and the magnetic-tape laminate is performed using photolithography and electrocasting. Positioning of the magnetic-tape laminate can be performed using a resist pattern formed by photolithography.