Patent Number: 
Section: claims

1. A monochromator for charged particle optics or for electron microscopy, the charged particles emanating from a radiation source disposed upstream of the monochromator, the radiation source having an image into which the charged particles virtually enter at a first angle with respect to an optical axis in a first plane and at a second angle with respect to the optical axis in a second plane, the monochromator comprising:a selection aperture having a selection aperture plane;at least one first deflection element disposed upstream of said selection aperture and having first electrodes generating a first electrostatic deflecting field, said first deflecting field producing a dispersion of the charged particles in the selection aperture plane for selecting charge particles of a desired energy interval; andat least one second deflection element disposed downstream of said selection aperture and having second electrodes generating a second electrostatic deflection field which eliminates the dispersion of said at least one first deflecting field, said first and said second deflection elements having a design other than spherically shaped, wherein potentials applied to said first and said second electrodes cause charged particles which virtually enter the image of the radiation source at respective first angles in the first plane to be differently focused than charged particles which virtually enter the image of the radiation source at respective second angles in the second plane, with charged particles of one energy being point focused exclusively in said selection aperture plane, wherein zero-crossings of deflections of the charged particles in the first and the second planes only coincide at a same axial position at said selection aperture plane. 2. The monochromator of claim 1, wherein said first and said second deflecting fields are designed in such a fashion that there are no further focuses in the monochromator except for the zero-crossings of the deflections of the charged particles in the first and the second planes at said selection aperture plane. 3. The monochromator of claim 1, wherein said first and said second deflection elements are designed in such a fashion that said first and said second deflecting fields cause reversal points in deflections of the charged particles in an x direction extending within said first plane with intermediate zero-crossings through the optical axis of the deflection path, said first and said second deflecting fields only causing changes of path curvatures having one single zero-crossing through the optical axis in the area of said selection aperture in a y direction extending perpendicularly to the x direction within said second plane. 4. The monochromator of claim 3, wherein said first and said second electrodes are substantially designed as sections of toroids, whose surfaces extend symmetrically to an xz plane in a coordinate system which is orthogonal and curved along a z axis and in which the z axis corresponds to the optical axis of the monochromator, have same separations from the z axis at any location thereon, and have a shape in an xy plane which differs from straight lines, such that dipoles formed by said first and said second electrodes are superposed by multipoles, wherein surfaces of said first and said second electrodes are designed in such a fashion that aperture aberrations caused by the monochromator can be compensated by said multipoles. 5. The monochromator of claim 4, wherein said multipoles are quadrupoles. 6. The monochromator of claim 4, wherein said multipoles are hexapoles. 7. The monochromator of claim 4, wherein said surfaces of said first and said second electrodes are curved. 8. The monochromator of claim 4, wherein said first and said second electrodes have surfaces in a form of a section of a truncated cone. 9. The monochromator of claim 8, wherein said surfaces form two “V”s having tips pointing in a same direction. 10. The monochromator of claim 8, wherein said surfaces form two “V”s having openings facing towards each other. 11. The monochromator of claim 1, wherein the monochromator is symmetrical with respect to said selection aperture plane. 12. The monochromator of claim 1, wherein the optical axis of the monochromator has substantially a shape of a closed loop. 13. The monochromator of claim 12, wherein a virtual input crossover and a virtual output crossover of the monochromator coincide in said selection aperture plane. 14. The monochromator of claim 1, wherein the optical axis at an exit of the monochromator corresponds to an extension of the optical axis at an entry of the monochromator. 15. The monochromator of claim 14, wherein the optical of the monochromator has substantially a shape of an Ω. 16. The monochromator of claim 15, wherein said Ω shape is formed by two deflection segments of said first deflection element and two deflection segments of said second deflection element, wherein said deflection segments have circular arc shaped deflection paths which each have an arc angle between 120° and 150°. 17. The monochromator of claim 14, wherein said first and said second deflection elements define a beam passage in a direction of input and output axes of the monochromator such that, when the monochromator is switched off, the charged particles also move along the optical axis at the output of the monochromator. 18. The monochromator of claim 1, wherein said first and said second electrodes are externally shielded with plates at extractor potential, said plates being oriented parallel to the optical axis. 19. The monochromator of claim 18, wherein said first and said second electrodes have surfaces which are oriented perpendicularly to the optical axis, said first and said second electrodes comprising shielding plates at extractor potential having passage openings for charged particle current. 20. The monochromator of claim 19, wherein said first and said second electrodes have box-shaped shieldings at extractor potential with passage openings for charged particle current. 21. A radiation source for the monochromator of claim 1, the radiation source having an electrostatic lens and an aperture disposed upstream of the monochromator for regulating and limiting a charged particle current, wherein said lens generates a virtual image of the radiation source which is downstream of an entrance of the monochromator.