Abstract:
The present invention enlarges a range of movement of field of view by beam deflection with a simple deflector configuration and suppresses deterioration of a signal electron detection rate caused by the beam deflection. A scanning electron microscope according to the present invention is provided with a first deflection field setting module that sets plural deflectors to move a scanning area on a specimen by a primary electron beam to a position deviated from an axis extended from an electron source toward the center of an objective lens and a second deflection field setting module that sets the plural deflectors so that trajectories of signal electrons are corrected without changing the scanning area set by the first deflection field setting module. The control unit controls the plural deflectors by adding a setting value set by the second deflection field setting module to a setting value set by the first deflection field setting module.
Abstract:
A scanning electron beam device having: a deflector (5) for deflecting an electron beam (17) emitted from an electron source (1); an objective lens (7) for causing the electron beam to converge; a retarding electrode; a stage (9) for placing a wafer (16); and a controller (15); wherein the stage can be raised and lowered. In the low acceleration voltage region, the controller performs rough adjustment and fine adjustment of the focus in relation to the variation in the height of the wafer using electromagnetic focusing performed through excitation current adjustment of the objective lens. In the high acceleration voltage region, the controller performs rough adjustment of the focus in relation to the variation in the height of the wafer by mechanical focusing performed through raising and lowering of the stage, and performs fine adjustment by electrostatic focusing performed through adjustment of the retarding voltage. It thereby becomes possible to provide a scanning electron beam device that measures, in a highly accurate manner, both the upper part and the bottom part of a groove or a hole having a high aspect ratio.
Abstract:
In order to provide a charged particle beam apparatus enabling reduction of deflecting coma aberration in cases such as where wide field-of-view scanning is carried out, a charged particle beam apparatus is provided with an electromagnetic objective lens and a stage on which a sample is placed, wherein the electromagnetic objective lens is provided with the following: a plurality of magnetic paths; an objective lens coil; an opening disposed so as to face the sample; an inner lens deflector disposed more on the objective lens coil side than the end of the opening.
Abstract:
The present invention enlarges a range of movement of field of view by beam deflection with a simple deflector configuration and suppresses deterioration of a signal electron detection rate caused by the beam deflection. A scanning electron microscope according to the present invention is provided with a first deflection field setting module that sets plural deflectors to move a scanning area on a specimen by a primary electron beam to a position deviated from an axis extended from an electron source toward the center of an objective lens and a second deflection field setting module that sets the plural deflectors so that trajectories of signal electrons are corrected without changing the scanning area set by the first deflection field setting module. The control unit controls the plural deflectors by adding a setting value set by the second deflection field setting module to a setting value set by the first deflection field setting module.
Abstract:
Pattern critical dimension measurement equipment includes an electron source configured to generate a primary electron beam, a deflector configured to deflect the primary electron beam emitted from the electron source, a focusing lens configured to focus the primary electron beam deflected by the deflector, a decelerator configured to decelerate the primary electron beam that irradiates the sample, a first detector located between the electron source and the focusing lens, the first detector being configured to detect electrons at part of azimuths of electrons generated from the sample upon irradiation of the sample with the primary electron beam, and a second detector located between the electron source and the first detector, the second detector being configured to detect electrons at substantially all azimuths of the electrons generated from the sample.
Abstract:
This charged-particle beam device changes conditions for combining an intensity ratio between upper and lower deflectors and rotation angles of the deflectors in multiple ways when obtaining images having different pixel sizes in the vertical and horizontal directions. Then, the charged-particle beam device determines an optimal intensity ratio between the upper and lower deflectors and rotation angles of the deflectors on the basis of variations in size value measured in the larger pixel size direction (Y-direction) of the image. As a result, it is possible to extend the field of view in the Y-direction while reducing deflection aberrations when measuring at high precision in the X-direction.
Abstract:
In order to provide a charged particle beam apparatus enabling reduction of deflecting coma aberration in cases such as where wide field-of-view scanning is carried out, a charged particle beam apparatus is provided with an electromagnetic objective lens and a stage on which a sample is placed, wherein the electromagnetic objective lens is provided with the following: a plurality of magnetic paths; an objective lens coil; an opening disposed so as to face the sample; an inner lens deflector disposed more on the objective lens coil side than the end of the opening.
Abstract:
A scanning electron microscope according to the present invention includes: an electron source that produces an electron beam; a trajectory dispersion unit that disperses the trajectory of an electron beam of electrons with a different energy value; a selection slit plate having a selection slit that selects the energy range of the dispersed electron beam; and a transmittance monitoring unit that monitors the transmittance of an electron beam, which is being transmitted through the selection slit. Accordingly, there can be provided a scanning electron microscope equipped with an energy filter that implements a stable reduction in energy distribution.
Abstract:
A charged-particle-beam device used for measuring the dimensions, etc., of fine circuit patterns in a semiconductor manufacturing process, wherein corrections are made in the defocusing and astigmatism generated during changes in the operating conditions of a Wien filter acting as a deflector of secondary signals such as secondary electrons, and the display dimensions of obtained images are kept constant. In the charged-particle-beam device, the Wien filter (23) is arranged between a detector and a lens (11) arranged on the test-sample side among two stages of lenses for converging a charged-particle beam, and a computing device (93) is provided for the interlocked control of the Wien filter (23) and a lens (12) arranged on the charged-particle-source side among the two stages of lenses.
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.