Abstract:
A charged particle beam exposure apparatus has a beam shaping optical system which forms an image of a charged particle source that emits charged particle beams, an aperture array and electrostatic lens which form a plurality of images of the charged particle source from the image of the charged particle source, a reduction electron optical system which reduces and projects the plurality of images of the charged particle source onto a wafer, and the first stigmator which generates astigmatism when the beam shaping optical system forms the image of the charged particle source in order to correct astigmatism generated in the reduction electron optical system. A charged particle beam exposure method of exposing a substrate by scanning with charged particle beams includes an adjustment step of making the size in the scanning direction of charged particle beams on the substrate smaller than the size in a direction perpendicular to the direction.
Abstract:
In an electron microscope to which a phase retrieval method is applied, an image size determined by a pixel size p of a diffraction pattern, a camera length L, and a wavelength λ of an illumination beam is allowed to have a certain relation with an illumination area on a specimen. Further, a beam illumination area or a scanning area of a deflector when a magnified image is observed is set by an illumination adjustment system, so that an image size when the magnified image is used for the phase retrieval method is allowed to have a certain relation with the image size determined by the pixel size of the diffraction pattern, the camera length, and the wavelength of the illumination beam. Accordingly, the information of the diffraction pattern is substantially equal to an object image to be reconstructed.
Abstract:
A plurality of primary beams are formed from a single electron source, the surface charge of a sample is controlled by at least one primary beam, and at the same time, the inspection of the sample is conducted using a primary beam other than this. Also, for an exposure area of the primary beam for surface charge control and an exposure area of the primary beam for the inspection, the surface electric field strength is set individually. Also, the current of the primary beam for surface charge control and the interval between the primary beam for surface charge control and the primary beam for inspection are controlled.
Abstract:
In an electron microscope to which a phase retrieval method is applied, an image size determined by a pixel size p of a diffraction pattern, a camera length L, and a wavelength λ of an illumination beam is allowed to have a certain relation with an illumination area on a specimen. Further, a beam illumination area or a scanning area of a deflector when a magnified image is observed is set by an illumination adjustment system, so that an image size when the magnified image is used for the phase retrieval method is allowed to have a certain relation with the image size determined by the pixel size of the diffraction pattern, the camera length, and the wavelength of the illumination beam. Accordingly, the information of the diffraction pattern is substantially equal to an object image to be reconstructed.
Abstract:
A charged particle beam lithography machine for exposing a target exposure surface by using a plurality of charged particle beams. The machine includes a charged particle source to emit a charged particle beam, an aperture substrate which has a plurality of apertures to divide the charged particle beam from the charged particle source into a plurality of charged particle beams, a plurality of electron optical systems which have the apertures as pupils, a charged particle beam optical system which projects, to the target exposure surface, charged particle source images formed by the plurality of electron optical systems, a unit adapted to set the apertures of the aperture substrate to an aperture for exposure and an aperture for aberration measurement to make the plurality of charged particle beams strike the charged particle beam optical system at different incident angles, and a detecting unit adapted to detect a position where the plurality of charged particle beams, which have passed through the aperture for aberration measurement, form images on an image surface of the charged particle beam optical system.
Abstract:
An electron gun includes a cathode portion which emits electrons, an anode portion which accelerates the emission electrons, a bias portion which is arranged between the cathode portion and the anode portion and controls trajectories of the emission electrons, a shielding portion which is arranged below the anode portion and shields some of the emission electrons, and a cooling portion which cools the shielding portion. The bias portion controls the trajectories of the electrons so as to form a crossover between the bias portion and the anode portion, and prevents the electrons from emitting on the anode portion.
Abstract:
The aberrations of a charged particle beam optical system in a lithography machine are measured. Control amounts to control optical elements included in the charged particle beam optical system are changed, the variations of the aberrations are obtained by executing the aberration measuring step, and the aberration sensitivities of the control amounts are obtained. The control amounts are decided on the basis of the aberrations of the charged particle beam optical system and the aberration sensitivities of the control amounts to set the aberrations of the charged particle beam optical system to target aberrations.
Abstract:
The dimension of the main field as a unit region for exposure is set to an integral submultiple of the arrangement pitch of the LSI to be exposed, by the control computer 62, and the exposure data stored in the form associated with electron beams from a data generation circuit 64 is limited to one-chip data alone in units of a stripe. This data is repeatedly read out to write the stripe. Further, a storage circuit 66 is provided to store the exposure data by means of a double buffer memory unit for each electron beam. While LSI is written according to one of the buffers, the next exposure stripe data is prepared on the other buffer, thereby bringing about a substantial reduction in the required speed of the exposure data generation circuit.
Abstract:
Electron beam writing equipment has an electron source and an electron optics system for scanning an electron beam emitted from the electron source on a sample via deflection means having at least two different deflection speeds. An objective lens is used to form a desired pattern on the sample The electron beam is moved by high speed scanning with the deflection means to repeat formation of a patterned beam. The electron beam is moved on the mark for beam correction by low speed scanning with the deflection means in synchronization with one cycle of the repetition. The position or the deflection distance of the electron beam or blanking time is corrected using detectors for back scattered or secondary electrons.
Abstract:
A technology capable of reducing the influence of the noise overlapped in a long transmission line when accurately measuring weak beam current in an electron beam writing system and capable of accurately and efficiently measuring weak beam current in a beam writing system using multiple beams is provided. With using a switch for connecting and disconnecting an electron beam detecting device and a detected signal line, the electron beam detecting device is disconnected from the detected signal line to accumulate the detected signals in the electron beam detecting device during the beam current measurement. Simultaneously with the finish of the measurement, the electron beam detecting device and the detected signal line are connected to measure the accumulated signals. Also, in order to simultaneously perform the measurement method, a plurality of electron beam detecting devices and switches are used to simultaneously measure a plurality of electron beams with high accuracy.