Patent Number: 051270285
Section: claims

1. A Bragg diffractor for energetic radiation comprising: a diffracting structure means having doubly curved diffracting planes and a diffracting surface comprising a plurality of steps with surfaces parallel to said diffracting planes; said steps being configured so that the midpoint on the curved surface of each step intercepts the focal circle of a Johansson geometry relating positions of a radiation source, the diffractor and a radiation image point; the surfaces of the said steps having a curvature in the plane of the focal circle equal to twice the radius of the focal circle and the surfaces of the said steps having a curvature perpendicular to the plane of the focal circle corresponding to rotational symmetry about a line passing through the source and image points. 2. A Bragg diffractor as defined in claim 1 in which the diffracting planes comprise the atomic planes of doubly curved single crystal lamellae. 3. A Bragg diffractor as defined in claim 1 in which the diffracting planes are the atomic planes of pieces of doubly-deformed single crystal material affixed to the doubly-curved surface of the steps on a substrate, each of the said pieces having a size equal to the size of the corresponding step. 4. A Bragg diffractor as defined in claim 1 in which the diffracting planes comprise the atomic planes of flakes or grains of single crystal nature affixed to the doubly curved surfaces of steps on a substrate. 5. A Bragg diffractor as defined in claim 1 in which the diffracting planes comprise alternating layers of different x-ray scattering power obtained by sequential deposition of these layers on the doubly curved surfaces of steps on a substrate. 6. A Bragg diffractor for energetic radiation comprising: a diffracting structure means having doubly curved diffracting planes and a diffracting surface comprising a plurality of steps with surfaces parallel to said diffracting planes; said steps being configured so that a point on the curved surface of each step intercepts the focal circle of a Johansson geometry relating positions of a radiation source, the diffractor and a radiation image point for all radial planes about an axis of symmetry; the surfaces of the said steps having a curvature in the plane of the focal circle equal to twice the radius of the focal circle, and the surfaces of the said steps having a curvature perpendicular to the plane of the focal circle corresponding to rotational symmetry about a line passing through the source and image points. 7. A Bragg diffractor as defined in claim 6 in which the diffracting planes comprise the atomic planes of doubly bent single crystal lamellae. 8. A Bragg diffractor as defined in claim 6 in which the diffracting planes are the atomic planes of pieces of toroidally-curved single crystal material affixed to the doubly-curved surfaces of the steps on a substrate, each of the said pieces having a size equal to the size of the corresponding step. 9. A Bragg diffractor as defined in claim 6 in which the diffracting planes comprise the atomic planes of flakes or grains of single crystal nature affixed to the doubly curved surfaces of steps on a substrate. 10. A Bragg diffractor as defined in claim 6 in which the diffracting planes comprise alternating layers of different x-ray scattering power obtained by sequential deposition of these layers on the doubly curved surfaces of steps of a substrate. 11. A Bragg diffractor for energetic radiation comprising: a diffracting structure means having doubly curved diffracting planes and a diffracting surface comprising a plurality of steps with surfaces parallel to said diffracting planes; said steps being configured so that a point on the curved surface of each step intercepts the focal circle of a Johansson geometry relating positions of a radiation source, the diffractor and a radiation focus; the surfaces of the said steps having a curvature in the plane of the focal circle equal to twice the radius of the focal circle; the surfaces of the steps having a curvature perpendicular to the plane of the focal circle corresponding to rotational symmetry about a line passing through a point on the focal circle. 12. A Bragg diffractor as defined in claim 11 in which the point through which the axis of rotational symmetry passes is a point on the focal circle diametrically opposite the midpoint of the diffractor. 13. A Bragg diffractor as defined in claim 11 in which the diffracting planes comprise the atomic planes of doubly curved single crystal lamellae. 14. A Bragg diffractor as defined in claim 11 in which the diffracting planes are the atomic planes of a pieces of doubly-curved single crystal material affixed to the doubly-curved surfaces of the steps on a substrate, each of the said pieces having a size equal to the size of the corresponding step. 15. A Bragg diffractor as defined in claim 11 in which the diffracting planes comprise the atomic planes of flakes or grains of single crystal nature affixed to the doubly curved surfaces of steps on a substrate. 16. A Bragg diffractor as defined in claim 11 in which the diffracting planes comprise alternating layers of different x-ray scattering power obtained by sequential deposition of these layers on the doubly curved surfaces of steps on a substrate.