Patent Number: 
Section: claims

1. An X-ray imaging apparatus, comprising:an X-ray interferometer constituted by a splitting device for splitting an incident X-ray beam into a first X-ray beam and a second X-ray beam, a reflecting device for reflecting said first X-ray beam and said second X-ray beam, and a combining device for combining a first reflected X-ray beam and a second reflected X-ray beam,means for placing a sample in an optical path of an arbitrary beam of said first and second X-ray beams,means for placing a phase shifter in an optical path of an arbitrary beam of said first and second X-ray beams,a detector for detecting an interference X-ray beam emitted from said X-ray interferometer; anda processing portion for obtaining an image of said sample based on an output of said detector,wherein said processing portion generates an image based on a change of an interference amplitude caused by said sample, which is represented by an equation 2r′√{square root over ((I1+ΔI)·I2)}, and the equation is a part of an equation representing intensity I′ of the interference X-ray beam I′=(I1−ΔI)+I2+2r′√{square root over ((I1−ΔI)·I2)}·cos(φ+Δp) where I1 represents the intensity of one of said first and second X-ray beams in the optical path of which said sample is placed, I2 represents the intensity of the other of said first and second X-ray beams, ΔI represents the change in the intensity of one of said first and second X-ray beams in the optical path of which said sample is placed, r′ represents a changed degree of coherence according to a change in the direction of an X-ray caused by said sample placed in an optical path of one of said first and second X-ray beams, φ represents a phase difference between said first and second X-ray beams, and Δp represents phase-shift caused by the sample placed in an optical path of one of said first and second X-ray beams. 2. An X-ray imaging apparatus as set forth in claim 1, further comprising means for reproducing a cross sectional image of said sample from a plurality of sample images obtained by rotating said sample in a direction perpendicular to the optical path of an X-ray beam. 3. An X-ray imaging apparatus as set forth in claim 1, wherein said X-ray interferometer is a single crystal block comprising a plurality of sheets of crystal wafers formed monolithically with a groundsill holding these wafers. 4. An X-ray imaging apparatus as set forth in claim 1, wherein said X-ray interferometer comprises a combination of crystal blocks comprising a plurality of sheets of crystal wafers formed monolithically with a groundsill holding these wafers. 5. An X-ray imaging apparatus as set forth in claim 1, wherein a shape of said phase shifter is a wedge type. 6. An X-ray imaging apparatus, comprising:an X-ray interferometer constituted by a splitting device for splitting an incident X-ray beam into a first X-ray beam and a second X-ray beam, a reflecting device for reflecting said first X-ray beam and said second X-ray beam, and a combining device for combining a first reflected X-ray beam and a second reflected X-ray beam,means for placing a sample in an optical path of an arbitrary beam of said first and second X-ray beams,means for placing a phase shifter in an optical path of an arbitrary beam of said first and second X-ray beams,a detector for detecting an interference X-ray beam emitted from said X-ray interferometer; anda processing portion for obtaining an image of said sample based on an output of said detector,wherein said processing portion generates an image based on a change of an interference amplitude 2r′√{square root over ((I1−ΔI)·I2)}, which is caused by said sample, and a phase-shift Δp, which is caused by said sample placed in an optical path of one of said first and second X-ray beams, wherein said change of an interference amplitude and the phase-shift are parts of an equation representing intensity I′ of the intereference X-ray beam I′=(I1−ΔI)+I2+2r′√{square root over ((I1−ΔI)·I2)}·cos(φ+Δp) where I1 represents the intensity of one of said first and second X-ray beams in the optical path of which said sample is placed, I2 represents the intensity of the other of said first and second X-ray beams, ΔI represents the change in the intensity of one of said first and second X-ray beams in the optical path of which said sample is placed, r′ represents a changed degree of coherence according to a change in the direction of an X-ray caused by said sample placed in an optical path of one of said first and second X-ray beams, and φ represents a phase difference between said first and second X-ray beams. 7. An X-ray imaging apparatus as set forth in claim 6, further comprising means for reproducing a cross sectional image of said sample from a plurality of sample images obtained by rotating said sample in a direction perpendicular to the optical path of an X-ray beam. 8. An X-ray imaging apparatus as set forth in claim 6, wherein said X-ray interferometer is a single crystal block comprising a plurality of sheets of crystal wafers formed monolithically with a groundsill holding these wafers. 9. An X-ray imaging apparatus as set forth in claim 6, wherein said X-ray interferometer comprises a combination of crystal blocks comprising a plurality of sheets of crystal wafers formed monolithically with a groundsill holding these wafers. 10. An X-ray imaging apparatus as set forth in claim 6, wherein a shape of said phase shifter is a wedge type. 11. An X-ray imaging method for splitting an incident X-ray beam into a first interfering beam and second interfering beam, comprising: placing a sample in an optical path of said first interfering beam, combining the first interfering beam and the second interfering beam, and obtaining an image of said sample from an interference X-ray beam formed by said combining,wherein the image of said sample is generated based on a change of an interference amplitude caused by said sample, which is represented by an equation 2r′√{square root over ((I1−ΔI)·I2)}, and the equation is a part of an equation representing intensity I′ of the interference beam I′=(I1−ΔI)+I2+2r′√{square root over ((I1−ΔI)·I2)}·cos(φ+Δp) where I1 represents the intensity of one of said first and second interfering beams in the optical path of which said sample is placed, I2 represents the intensity of the other of said first and second interfering beams, ΔI represents the change in the intensity of one of said first and second interfering beams in the optical path of which said sample is placed, r′ represents a changed degree of coherence according to a change in the direction of an interfering beam caused by said sample placed in an optical path of one of said first and second interfering beams, φ represents a phase difference between said first and second interfering beams, and Δp represents phase-shift caused by the sample placed in an optical path of one of said first and second interfering beams. 12. An X-ray imaging method as set forth in claim 11, wherein a cross sectional image of said sample is reproduced from a plurality of sample images obtained by rotating said sample in a direction perpendicular to the optical path of said first interfering beam. 13. An X-ray imaging method as set forth in claim 11, further comprising the steps of:placing a phase shifter in the optical path of the first interfering beam or the second interfering beam;shifting a phase of the first interfering beam or the second interfering beam by relatively moving or rotating said phase shifter with respect to said optical path and obtaining an interference X-ray beam at different phase shifts; andfinding the amount of change in the interference amplitude and an amount of change in a phase caused by said sample using a plurality of interference X-ray beams obtained by said shifting. 14. An X-ray imaging apparatus, comprising:an X-ray interferometer constituted by a splitting device for splitting an incident X-ray beam into a first X-ray beam and a second X-ray beam, a reflecting device for reflecting said first X-ray beam and said second split X-ray beam, and a combining device for combining a first reflected X-ray beam and a second reflected X-ray beam,means for placing a sample in an optical path of an arbitrary beam of said first and second X-ray beams,means for placing a phase shifter in an optical path of an arbitrary beam of said first and second X-ray beams,a detector for detecting an interference X-ray beam emitted from said X-ray interferometer; anda processing portion for obtaining an image of said sample by combining an amount of change in an amplitude and an amount of change in a phase of the interference X-ray beam caused by said sample from an output of said detector,wherein combining of an amount of change in an amplitude and an amount of change in a phase of the interference X-ray beam performed in said processing portion is carried out by using a compositional ratio calculated from magnitude of an amount of change in an amplitude. 15. An X-ray imaging method for splitting an incident X-ray beam into a first interfering beam and a second interfering beam, placing a sample in an optical path of said first interfering beam, combining the first interfering beam and the second interfering beam, and obtaining an image of said sample from an interference X-ray beam formed by said combining,wherein the image of said sample is formed by using an amount of change in an amplitude of said interference X-ray beam caused by said sample,wherein the image of said sample is formed by using an amount composed of an amount of change in an amplitude and an amount of change in a phase of said interference X-ray beam caused by said sample; andwherein the composition of the amount of the change in the amplitude and the amount of the change in the phase is carried out by using a compositional ratio calculated based on magnitude of an amount of change in an amplitude. 16. An X-ray imaging method as set forth in claim 15, wherein a cross sectional image of said sample is reproduced from a plurality of sample images obtained by rotating said sample in a direction perpendicular to the optical path of said first interfering beam. 17. An X-ray imaging method as set forth in claim 15, further comprising the steps of:placing a phase shifter in the optical path of the first interfering beam or the second interfering beam;shifting a phase of the first interfering beam or the second interfering beam by relatively moving or rotating said phase shifter with respect to said optical path and obtaining an interference X-ray beam at different phase shifts; andfinding the amount of change in the interference amplitude and an amount of change in a phase caused by said sample using a plurality of interference X-ray beams obtained by said shifting. 18. An X-ray imaging method for splitting an incident X-ray beam into a first interfering beam and a second interfering beam, placing a sample in an optical path of said first interfering beam, combining the first interfering beam and the second interfering beam, and obtaining an image of said sample from an interference X-ray beam formed by said combining,wherein the image of said sample is formed by using an amount of change in an amplitude of said interference X-ray beam caused by said sample, and further comprising the steps of:placing a wedge type phase shifter in the optical path of the first interfering beam or the second interfering beam;obtaining the interference beam;Fourier transforming said interference X-ray beam;shifting an obtained Fourier spectrum in a direction to an origin by a number of frequencies corresponding to an interval of Moire-image interferences fringes appearing in the interference X-ray beam;inverse Fourier transforming the shifted spectrum; andfinding the amount of change in an amplitude and an amount of change in a phase of said interference X-ray beam caused by said sample based on obtained data. 19. An X-ray imaging method for splitting an incident X-ray beam into a first interfering beam and a second interfering beam, placing a sample in an optical path of said first interfering beam, combining the first interfering beam and the second interfering beam, and obtaining an image of said sample from an interference X-ray beam formed by said combining,wherein the image of said sample is formed by using an amount of change in an amplitude of said interference X-ray beam caused by said sample,wherein the image of said sample is formed by using an amount composed of an amount of change in an amplitude and an amount of change in a phase of said interference X-ray beam caused by said sample, and further comprising the steps of:placing a wedge type phase shifter in the optical path of the first interfering beam and the second interfering beam;obtaining the interference beam;Fourier transforming said interference X-ray beam;shifting an obtained Fourier spectrum in a direction to an origin by a number of frequencies corresponding to an interval of Moire-image interference fringes appearing in the interference X-ray beam;inverse Fourier transforming the shifted spectrum; andfinding the amount of change in the amplitude and the amount of change in the phase of said interference X-ray beam caused by said sample based on obtained data.