Patent Number: 
Section: claims

1. A charged particle beam apparatus comprising:a source of a charged particle beam; a condenser optical system for irradiating a specimen with the charged particle beam emitted from the source; a specimen holder for holding the specimen irradiated with the charged particle beam; an imaging lens system for imaging the specimen; a device for observing or recording the specimen image; an objective lens system formed by one lens or a plurality of lenses capable of controlling focal lengths independently in the imaging lens system positioned on the downstream side on the traveling direction of the charged particle beam from the specimen position on an optical axis of the charged particle beam; an upper-stage biprism located in a plane orthogonal to the optical axis at a position of an image plane of the specimen determined by the objective lens system on the downstream side of the objective lens system; an intermediate-stage biprism located in a plane in parallel with the plane where the upper-stage biprism is placed formed on the downstream side of the upper-stage biprism through one or more lenses in the imaging lens system; and a lower-stage biprism located in a plane in parallel with the plane where the upper-stage biprism is placed on the downstream side of the intermediate-stage biprism through one or more lenses in the imaging lens system, the three biprisms being capable of moving of their positions and rotating of their azimuth in the respective plane independently, wherein voltages can be applied to the upper-stage biprism, the intermediate-stage biprism, and the lower-stage biprism independently to deflect the charged particle beam in an arbitrary direction, andwherein in a case that an azimuth angle between the intermediate-stage biprism and the upper-stage biprism is Φ1, and an azimuth angle between the intermediate-stage briprism and the lower-stage biprism is Φ3, the charged particle beam is deflected in a condition that Φ3 is not zero and Φ3 is not Φ1. 2. The charged particle beam apparatus according to claim 1, wherein the specimen image formed in an arbitrary magnification in a plane where the upper-stage biprism is positioned with orthogonal to the optical axis, by adjusting the focal lengths of the respective lenses of the objective lens system having the plurality of lenses. 3. The charged particle beam apparatus according to claim 1, wherein the lower-stage biprism is positioned on the downstream side of a lens placed on the downstream side of the intermediate-stage biprism on the optical axis of the charged particle beam, and is positioned on the downstream side of an image of the source formed by the lens. 4. The charged particle beam apparatus according to claim 1, wherein the lower-stage biprism is positioned on the downstream side of a lens placed on the downstream side of the intermediate-stage biprism on the optical axis of the charged particle beam, and is positioned between the lens and an image of the source formed by the lens. 5. A charged particle beam apparatus comprising: a source of a charged particle beam; a condenser optical system for irradiating a specimen with the charged particle beam emitted from the source; a specimen holder for holding the specimen irradiated with the charged particle beam; an imaging lens system for imaging the specimen; a device for observing or recording the specimen image; an objective lens system formed by one lens or a plurality of lenses capable of controlling focal lengths independently in the imaging lens system positioned on the downstream side on the traveling direction of the charged particle beam from the specimen position on an optical axis of the charged particle beam; an upper-stage quadrangular-pyramid prism located in a plane orthogonal to the optical axis at a position of an image plane of the specimen determined by the objective lens system on the downstream side of the objective lens system; and a lower-stage biprism located in a plane in parallel with the plane where the upper-stage quadrangular-pyramid prism is placed on the downstream side of the upper-stage quadrangular-pyramid prism through one or more lenses in the imaging lens system, the two prisms being capable of moving of the positions and rotating of their azimuth in the respective plane independently, wherein voltages can be applied to the upper-stage quadrangular-pyramid prism and the lower-stage biprism independently to deflect the charged particle beam in an arbitrary direction. 6. The charged particle beam apparatus according to claim 5, wherein the specimen image formed in an arbitrary magnification in a plane where the upper quadrangular-pyramid prism is positioned with orthogonal to the optical axis by adjusting the focal lengths of the respective lenses of the objective lens system having the plurality of lenses. 7. The charged particle beam apparatus according to claim 5, wherein the lower-stage biprism is positioned on the downstream side of a lens placed on the downstream side of the upper-stage quadrangular-pyramid prism on the optical axis of the charged particle beam, and is positioned on the downstream side of an image of the source formed by the lens. 8. The charged particle beam apparatus according to claim 5, wherein the lower-stage biprism is positioned on the downstream side of a lens placed on the downstream side of the upper-stage quadrangular-pyramid prism on the optical axis of the charged particle beam, and is positioned between the lens and an image of the source formed by the lens. 9. The charged particle beam apparatus according to claim 5, wherein the deflection direction of the charged particle beam by the quadrangular-pyramid prism can be controlled by adjusting an azimuth angle formed between filament electrodes of two electron biprisms in the same image plane constituting the quadrangular-pyramid prism. 10. The charged particle beam apparatus according to claim 5, wherein the deflection angle of the charged particle beam by the quadrangular-pyramid prism can be controlled independently in the vertical direction with respect to the filament electrodes by adjusting applied voltages to filament electrodes of two electron biprisms in the same image plane constituting the quadrangular-pyramid prism.