Ultrahigh resolution interferometric x-ray imaging

• US 5,812,629 A
• Filed: 04/30/1997
• Issued: 09/22/1998
• Est. Priority Date: 04/30/1997
• Status: Expired due to Term

• Current Assignee: John F. Clauser
• Original Assignee: John F. Clauser
• Inventors: Clauser, John F.
• Primary Examiner(s): Porta, David P.
• Assistant Examiner(s): Bruce, David Vernon
• Application Number:
  US08/846,742
• Time in Patent Office: 510 Days
• Field of Search: 378/2, 378/7, 378/37, 378/62, 378/71, 378/145, 378/147
• US Class Current: 378/62
• CPC Class Codes: A61B 6/032 Transmission computed tomography [CT]
• CPC Class Codes: A61B 6/4291 the detector being combined with a grid or grating
• CPC Class Codes: A61B 6/466 adapted to display 3D data
• CPC Class Codes: A61B 6/481 involving the use of contrast agents
• CPC Class Codes: A61B 6/482 involving multiple energy imaging
• CPC Class Codes: A61B 6/484 involving phase contrast X-ray imaging
• CPC Class Codes: A61B 6/502 for diagnosis of breast, i.e. mammography
• CPC Class Codes: A61B 6/504 for diagnosis of blood vessels, e.g. by angiography
• CPC Class Codes: G01N 23/041 Phase-contrast imaging, e.g. using grating interferometers
• CPC Class Codes: G21K 2207/005 Methods and devices obtaining contrast from non-absorbing interaction of the radiation with matter, e.g. phase contrast

Abstract

The Invention provides practical apparatus and methods for significant improvements to conventional radiography practice. It can image objects having negligible x-ray absorption contrast e.g. otherwise x-ray transparent low-Z artifacts such as human soft-tissue, by obtaining edge-enhanced contrast from an object'"'"'s (BDY) x-ray refractive-index gradients. In mammography, the contrast of small micro-calcifications is increased typically 4-fold, or more. It can be "tuned" to obtain element-selective refractive-index enhanced contrast to resonantly image minute quantities of a specific element with Z≈35-56 and only that element. With only a single brief x-ray exposure it can produce two independent images, e.g. of the object'"'"'s x-ray absorption and refractive-index distributions. It virtually eliminates the blurring and contrast reducing effects of x-ray scatter, especially of very small-angle scatter. It does not use a Bucky grid, and the associated increase in effective detector quantum efficiency results in a significant decrease in image quantum mottle. It can produce CT scan 3D images with a much reduced scanning time. The Invention provides radiograms with greatly improved resolution, contrast and versatility, and edge-enhanced features. It operates via the fractional Talbot effect using two pre-object microfabricated gratings (G1, G2) and a detector (D) preferably containing a periodic pixel array. It further includes an in-situ laser interferometer for aligning the gratings (G1, G2) to the detector (D). While the Invention has a wide range of application, it is ideally suited for medical imaging of biological soft-tissue, and especially for mammography, angiography, and CT (or CAT) scans.

Claims

1. Apparatus for producing an image that describes the internal structure of an object, comprising

a source of x-rays,

an x-ray image detector;

improved by its further comprising

three very-thin slab-shaped volumes, SV1, SV2, and SV3, each with substantially-planar slab faces oriented relative to each other to be substantially-mutually-parallel, and each containing an associated very-thin material structure that interacts with x-rays, and

means for limiting the energy-bandwidth of detected x-rays;

wherein said three contained structures are positioned between said source and said detector so that x-rays from said source propagate in the sequential order, first through said structure within slab-volume SV1, next through said structure within slab-volume SV2, next through said object, next into slab-volume SV3, and then are detected; and

wherein the directions x and y are both parallel to the substantially-parallel faces of said three slab-volumes; and

wherein said material structures within slab-volumes SV1, and SV2 are fabricated to be spatially-periodic within their associated useful x-direction widths, respectively with associated spatial periods a_1x and a_2x, and oriented within the apparatus so that each structure'"'"'s respective periodicity-direction that is associated with said respective period lies in the direction x; and

wherein the perpendicular distance between slab-volume SV1 and slab-volume SV2 is R₁ and the perpendicular distance between slab-volume SV2 and slab-volume SV3 is R₂ ; and

wherein b, q, and p are positive integers; and

wherein a_1x is accurately related to a_2x by

space="preserve" listing-type="equation">a.sub.1x =b a.sub.2x (R.sub.1 +R.sub.2)(q p R.sub.2).sup.-1 ;

and

wherein, when said object is absent, and for x-rays with at least one specific energy value that lies within said energy-bandwidth, and throughout the associated useful x-direction width of said material structure within slab-volume SV3, then the two structures respectively within slab-volumes SV1 and SV2 acting together but not separately project onto slab-volume SV3 an x-ray intensity distribution that is substantially spatially-periodic in direction x with the spatial period a_Px and has a substantial spatial intensity variation; and

wherein when the greatest common integer divisor of b and q is 1, then the period a_Px is accurately related to a_2x by

space="preserve" listing-type="equation">a.sub.Px =a.sub.2x (R.sub.1 +R.sub.2)(q p R.sub.1).sup.-1.

2. Apparatus of claim 1 wherein, when said object is absent, and for said x-rays with said specific energy value that lies within said energy-bandwidth, then each of the two structures respectively within slab-volumes SV1 and SV2, acting alone with the other absent, projects onto slab-volume SV3 an x-ray intensity distribution that is different from said spatial distribution projected by said two structures acting together;

and

wherein any associated residual spatial periodicity in direction x of either of said two distributions projected by said two structures acting alone has a diminished spatial intensity variation relative to said spatial distribution projected by said two structures acting together, and/or has a dominant spatial period that is different from a_Px.

3. Apparatus of claim 1 wherein b and q are both equal to 1.

4. Apparatus of claim 1 wherein slab-volume SV1 is located near said x-ray source.

5. Apparatus of claim 1 further comprised of means for controlling the energy spectrum of x-rays that are projected onto slab-volume SV3.

6. Apparatus of claim 1 wherein a material structure within a slab-volume is spatially periodic with the spatial period a_SV in an associated periodicity-direction when the effects of said structure'"'"'s x-ray interaction properties are left substantially unchanged except at said structure'"'"'s edges if said structure is spatially translated in said associated periodicity-direction by a distance that is an integral multiple of the period a_SV ;

and

wherein said periodicity-direction for said structure provides a locally minimum spatial period measured in some fixed direction under an infinitesimal rotation of said structure within its containing slab-volume in which said structure'"'"'s periodicity-direction rotates relative to said fixed direction with an axis of said infinitesimal rotation that is perpendicular to said substantially-planar mutually-parallel slab faces.

7. Apparatus of claim 6 wherein when a material structure within a slab-volume is spatially periodic with the spatial period a_SV, then said structure is also spatially periodic with a longer spatial period that is an integral multiple of a_SV.

8. Apparatus of claim 7 wherein the periods a_1x and a_2x are the shortest fabricated periods for which the respective structures within slab-volumes SV1 and SV2 are spatially-periodic.

10. Apparatus of claim 1 further comprised of a thin substrate that provides structural support for a spatially-periodic material structure within a slab-volume;

wherein said substrate is made from a material that is minimally absorbing of light and x-rays, and

wherein said substrate has a substantially constant thickness.

11. Apparatus of claim 1 wherein the directions x and y are substantially perpendicular to each other.

12. Apparatus of claim 1 wherein said structure within slab-volume SV1 is fabricated and configured to be additionally spatially-periodic within its associated useful y-direction width with period a_1y and with the associated additional periodicity-direction lying in the direction y;

and

wherein said structure within slab-volume SV2 is fabricated and configured to be additionally spatially-periodic within its associated useful y-direction width with period a_2y and with the additional associated periodicity-direction lying in the direction y; and

wherein a_1y is accurately related to a_2y by

space="preserve" listing-type="equation">a.sub.1y =b a.sub.2y (R.sub.1 +R.sub.2)(q p R.sub.2).sup.-1 ;

and

wherein, when said object is absent, and for x-rays with at least one energy value that lies within said energy-bandwidth and throughout the associated useful y-direction width of said material structure within slab-volume SV3, then the structures within slab-volumes SV1 and SV2 acting together but not separately project onto slab-volume SV3 an x-ray intensity distribution that is additionally substantially spatially-periodic in direction y with the spatial period a_Py ; and

wherein when the greatest common integer divisor of b and q is 1, then the period a_Py is accurately related to a_2y by

space="preserve" listing-type="equation">a.sub.Py =a.sub.2y (R.sub.1 +R.sub.2)(q p R.sub.1).sup.-1.

13. Apparatus of claim 12 wherein a_2y is approximately equal to a_2x.

14. Apparatus of claim 12 wherein a material structure within a particular slab-volume is spatially-periodic with the spatial period a_SVx in the associated periodicity-direction x and is also spatially-periodic with the spatial period a_SVy in the associated periodicity-direction y;

and

wherein X_SV and y_SV are position coordinate values associated respectively with directions x and y that specify points on said particular spatially-periodic structure; and

wherein f(t;

a_SV) is a periodic function of dummy variable t that is parameterized by the period a_SV ; and

wherein j is an arbitrary integer; and

wherein the function f(t;

a_SV) has the periodic property given by

space="preserve" listing-type="equation">f(t;

a.sub.SV)f(t+ja.sub.SV ;

a.sub.SV);

and

wherein g is a constant; and

wherein the spatial dependence of the transmission properties of x-rays through particular said spatially-periodic material structure at coordinate values x_SV and y_SV can be evaluated approximately by using the function

space="preserve" listing-type="equation">g±

f(x.sub.SV ;

a.sub.SVx)f(y.sub.SV ;

a.sub.SVy);

and

wherein, when said particular slab-volume is slab-volume SV1, then the associations a_SVx =a_1x and a_SVy =a_1y hold; and

wherein, when said particular slab-volume is slab-volume SV2, then the associations a_SVx =a_2x and a_SVy =a_2y hold.

15. Apparatus of claim 12 wherein a material structure within a particular slab-volume is spatially-periodic with the spatial period a_SVx in the associated periodicity-direction x and is also spatially-periodic with the spatial period a_SVy in the associated periodicity-direction y;

and

wherein x_SV and y_SV are position coordinate values associated respectively with directions x and y that specify points on said particular spatially-periodic structure; and

wherein f(t;

a_SV) is a periodic function of dummy variable t that is parameterized by the period a_SV ; and

wherein j is an arbitrary integer; and

wherein the function f(t;

a_SV) has the periodic property given by

space="preserve" listing-type="equation">f(t;

a.sub.SV)=f(t+ja.sub.SV ;

a.sub.SV);

and

wherein g is a constant; and

wherein the spatial dependence of the transmission properties of x-rays through said particular spatially-periodic material structure at coordinate values x_SV and y_SV can be evaluated approximately by using the function

space="preserve" listing-type="equation">g±

f(x.sub.SV ;

a.sub.SVx)f(y.sub.SV ;

a.sub.SVy)±

f x.sub.SV +(a.sub.SVx /2);

a.sub.SVx !f y.sub.SV +(a.sub.SVy !;

and

wherein, when said particular slab-volume is slab-volume SV1, then the associations a_SV =a_1x and a_SVy =a_1y hold; and

wherein, when said particular slab-volume is slab-volume SV2, then the associations a_SVx =a_2x and a_SVy =a_2y hold.

16. Apparatus of claim 1 wherein the structure within slab-volume SV1 is made from a material that absorbs x-rays and is configured so that its structure acts as a spatially-periodic x-ray mask.

17. Apparatus of claim 1 wherein the structure within slab-volume SV2 is made from a material that absorbs x-rays and is configured so that its structure acts as a spatially-periodic x-ray mask.

18. Apparatus of claim 1 wherein the two structures respectively within slab-volumes SV1 and SV2 are each made from a material that absorb x-rays and are each configured so that their structures act as spatially-periodic x-ray masks;

and

wherein, when said object is absent, and for said x-rays with said specific energy value that lies within said energy-bandwidth, then said two structures acting together but not separately project said spatially periodic x-ray intensity distribution onto slab-volume SV3 as a geometric x-ray shadow.

19. Apparatus of claim 1 wherein, when said object is absent, and for said x-rays with said specific energy value that lies within said energy-bandwidth, then the two structures respectively within slab-volumes SV1 and SV2 acting together but not separately project said spatially periodic x-ray intensity distribution onto slab-volume SV3 by wave interference of the electromagnetic waves associated with said x-rays via the fractional Talbot effect;

and

wherein the Talbot effect is special case of the fraction Talbot effect; and

wherein the formation of spatially-periodic geometric shadows is a further special case of the Talbot effect.

20. Apparatus of claim 19 wherein n and m are positive integers;

and

wherein the greatest common integer divisor of n and m is 1; and

wherein the average energy of said energy-bandwidth-limited x-rays projected onto slab-volume SV3 is E_X ; and

wherein the product hc is Planck'"'"'s constant times the speed of light; and

wherein a_2x is approximately equal to the value given by

space="preserve" listing-type="equation">(m/n).sup.1/2 (hc R.sub.1 R.sub.2 /E.sub.X).sup.1/2 (R.sub.1 +R.sub.2).sup.-1/2.

21. Apparatus of claim 19 wherein the energy spectrum of said energy-bandwidth-limited x-rays includes a multiplicity of component energy values;

and

wherein the average energy of said bandwidth limited x-rays projected onto slab-volume SV3 is E_X ; and

wherein said multiplicity of component energy values includes component energy values that are both substantially above and substantially below E_X ; and

wherein said multiplicity of component energy values may be comprised of a continuum of energy values; and

wherein, when said object is absent, then the spatial distribution of x-ray intensities projected onto slab-volume SV3 by x-rays with component energy values substantially above E_X is substantially different from the spatial distribution of x-ray intensities projected onto slab-volume SV3 by x-rays with component energy values substantially below E_X.

22. Apparatus of claim 21 wherein E_X is approximately equal to the energy of an x-ray absorption edge of some chemical element, and

wherein said chemical element is present within said object, and

wherein said presence of said chemical element within said object is anisotropic.

23. Apparatus of claim 1 wherein a material structure within a selected slab-volume is divided into discrete portions;

and

wherein each of said discrete portions of material within said slab-volume has an associated finite surface-projected area formed by perpendicularly projecting boundaries of said discrete portion on to a slab face of said selected slab-volume; and

wherein each of said discrete portions of material within said selected slab-volume has a thickness measured perpendicularly to said slab face that is approximately locally constant throughout said associated surface-projected area; and

wherein the thicknesses of discrete portions encountered in passing spatially along a straight line through various discrete portions step in a spatially periodic fashion among different discrete values; and

wherein said different discrete values include at least one significant finite value and possibly, but not necessarily, include the value approximate-zero; and

wherein the thickness of each said discrete portion provides an approximately locally-constant magnitude for the interaction of x-rays with said material when said x-ray propagation is along a single very thin path that is incident on a discrete portion'"'"'s associated surface-projected area; and

wherein said possible approximately zero-thickness portions of material provide negligible interaction with x-rays when said x-rays are incident along said very thin path on an approximately zero-thickness portion'"'"'s associated surface-projected area.

24. Apparatus of claim 23 wherein slab-volume SV2 is a selected slab-volume that is divided into discrete portions;

and

wherein said structure within slab-volume SV2 is made from a material that refracts x-rays; and

wherein said refraction induces a phase shift of the electromagnetic field amplitudes of x-rays incident on slab-volume SV2 that occurs in addition to the phase shift experienced by propagation of said x-rays the same distance in vacuum; and

wherein said phase shift may be negative; and

wherein said phase shift for x-rays incident on a discrete portion'"'"'s associated surface-projected area is approximately locally constant and approximately proportional to the associated thickness of said discrete portion; and

wherein the quantity m_* is an integer that is greater than 1; and

wherein the quantity n_* is a positive integer; and

wherein the integers n_* and m_* have a greatest common integer divisor of 1; and

wherein there is an imaginary line-segment with the length a_2x oriented in the direction x on slab-volume SV2 that thereby spans one x-direction period of said structure within slab-volume SV2; and

wherein said x-directed line-segment starts and ends on boundaries of said surface-projected areas; and

wherein said x-directed line-segment crosses through m_* of said surface-projected areas; and

wherein, in crossing surface-projected area boundaries between associated discrete portions, said x-directed line-segment is divided approximately equally into m_* x-directed line-segment fractions by said area boundaries; and

wherein each of said x-directed line-segment fractions has approximately the length a_2x /M_* ; and

wherein said crossed associated discrete portions are numbered sequentially and monotonically starting with the value 0 by the associated integer index j_x in passing from one end of said x-directed line-segment to the other end; and

wherein said indices j_x form a monotonic integer sequence starting at the value 0 and ending with the value m_* -1; and

wherein index j_x assumes only discrete values that are greater than -1 and are less than m_* ; and

wherein index j_x assumes any one such discrete value once and only once in said sequence; and

wherein each value of index j_x has an associated accompanying index k_x ; and

wherein said association of index j_x with index k_x associates index k_x with said numbered discrete portion; and

wherein said accompanying index k_x also has only m_* possible discrete values; and

wherein said sequence of values for index j_x and said association of each index j_x with index k_x provides an associated sequence of values for k_x ; and

wherein the set of discrete values assumed by the index k_x is the same set of discrete values assumed by the integer j_x so that index k_x assumes only discrete values that are greater than -1 and are less than m_*, and so that index k_x assumes any one value within said set once and only once; and

wherein the relationship between k_x and j_x is j_x = (n_* k_x) modulo m_* !; and

wherein said relationship between k_x and j_x provides that said sequence of values for j_x and said associated sequence of values for k_x are either the same sequence as each other or are a permutation of each other; and

wherein each and every discrete portion of said structure within slab-volume SV2 has an associated pair of indices j_x and k_x that are arranged

so that the values of the indices j_x and k_x are associated with said discrete portions and have a spatially periodic arrangement, and

so that the associated sequences of j_x and k_x values, encountered on any two such x-directed imaginary line-segments that are each of length a_2x and are each starting and ending on boundaries of said surface-projected areas, are the same as each other when said two x-directed line-segments are aligned on the same straight line and spaced from each other by a distance that is an integral multiple of a_2x ; and

wherein the product hc is Planck'"'"'s constant times the speed of light; and

wherein the quantity r_* is a chosen non-zero integer; and

wherein the energy E_* is defined by

space="preserve" listing-type="equation">E.sub.* =(m.sub.* /n.sub.*)hc R.sub.1 R.sub.2 (R.sub.1 +R.sub.2).sup.-1 a.sub.2x.sup.-1 ;

and

wherein φ

_* is a spatially constant phase shift.

25. Apparatus of claim 24 wherein, when x-rays with the approximate energy E_* propagate along a single very thin path through slab-volume SV2, and when said very thin path is through a surface-projected area with associated index k_x,

then said x-rays obtain a value for said refraction-induced phase shift that occurs in addition to the phase shift experienced in vacuum has a value that is approximately equal to the value given in radians by π

n_* r_* k_x -(k_x² m_*^-1)!-φ

_*.

26. Apparatus of claim 24 wherein the integer m_* is even, and wherein the value of φ

_* in radians is approximately equal to

space="preserve" listing-type="equation">π

n.sub.* r.sub.* m.sub.* /4.

27. Apparatus of claim 24 wherein the integer m_* is odd, and wherein the value of φ

_* in radians is approximately equal to

space="preserve" listing-type="equation">π

n.sub.* r.sub.* (m.sub.* -1).sup.2 (4m.sub.*).sup.-1.

28. Apparatus of claim 24 wherein a_2x is approximately equal to

29. Apparatus of claim 24 wherein n is a positive integer, and wherein a_2x is approximately equal to

30. Apparatus of claim 24 wherein n is a positive integer, and wherein a_2x is approximately equal to

31. Apparatus of claim 24 wherein said structure within slab-volume SV2 is fabricated and configured to be additionally spatially-periodic within its associated useful y-direction width with period a_2y and with the additional associated periodicity-direction lying in the direction y;

and

wherein there is an imaginary line-segment with the length a_2y oriented in the direction y on slab-volume SV2 that thereby spans one y-direction period of said structure within slab-volume SV2; and

wherein said y-directed line-segment starts and ends on boundaries of said surface-projected areas; and

wherein said y-directed line-segment crosses through m_* of said surface-projected areas; and

wherein, in crossing surface-projected area boundaries between associated discrete portions, said y-directed line-segment is divided approximately equally into m_* y-directed line-segment fractions by said area boundaries; and

wherein each said y-directed line-segment fraction has approximately the length a_2y /m_* ; and

wherein said crossed associated discrete portions are numbered sequentially and monotonically starting with the value 0 by the associated integer index j_y in passing from one end of said y-directed line-segment to the other end; and

wherein said indices j_y form a monotonic integer sequence starting the value 0 and ending with the value m_* -1; and

wherein index j_y assumes only discrete values that are greater than -1 and are less than m_* ; and

wherein index j_y assumes any one such discrete value once and only once in said sequence; and

wherein each value of index j_y has an associated accompanying index k_y ; and

wherein said association of index j_y with index k_y associates index k_y with said numbered discrete portion; and

wherein said accompanying index k_y also has only m_* possible discrete values; and

wherein said sequence of values for index j_y and said association of each index j_y with index j_y provides an associated sequence of values for k_y ; and

wherein the set of discrete values assumed by the index k_y is the same set of discrete values assumed by the integer j_y so that index k_y assumes only discrete values that are greater than -1 and are less than m_*, and so that index k_y assumes any one value within said set once and only once; and

wherein the relationship between k_y and j_y is j_y = (n_* k_y) modulo m_* !; and

wherein said relationship between k_y and j_y provides that said sequence of values for j_y and said associated sequence of values for k_y are either the same sequence as each other or are a permutation of each other; and

wherein each and every discrete portion of said structure within slab-volume SV2 each has an additional associated pair of indices j_y and k_y

so that each and every discrete portion of said structure within slab-volume SV2 thereby has four associated indices j_x, k_x, j_y, and k_y ; and

wherein the indices j_y and k_y are arranged so that the values of the indices j_y and k_y are associated with said discrete portions in a spatially periodic arrangement, and

so that the associated sequences of j_y and k_y values, encountered on any two such y-directed imaginary line-segments that are each of length a_2y and are each starting and ending on boundaries of said surface-projected areas, are the same as each other when said two y-directed line-segments are aligned on the same straight line and spaced from each other by a distance that is an integral multiple of a_2y ; and

wherein, when x-rays with the approximate energy E_* propagate along a single very thin path through slab-volume SV2, and when said very thin path is through a surface-projected area with associated indices k_x and k_y,

then said x-rays obtain a value for said refraction-induced phase shift that occurs in addition to the phase shift experienced in vacuum has a value that is approximately equal to the value given in radians by

space="preserve" listing-type="equation">π

n.sub.* r.sub.* k.sub.x -(k.sub.x.sup.2 m.sub.*.sup.-1)+k.sub.y -(k.sub.y.sup.2 m.sub.*.sup.-1)!-2φ

.sub.*.

32. Apparatus of claim 1 wherein v is a positive integer.

33. Apparatus of claim 32 wherein said x-ray image detector is comprised of a spatially-periodic array of detector-pixels whose front surface is substantially planar;

and

wherein the detector-pixel front surfaces interact with x-rays in a manner that results in the detection and measurement of the spatial distribution of the intensity of said x-rays incident on said image detector; and

wherein said array of detector-pixels is spatially periodic in direction x so that centroids of the front surfaces of adjacent detector-pixels within said spatially-periodic array are periodically spaced from each other in the direction y by the distance a_Dx ; and

wherein u is a positive even integer.

34. Apparatus of claim 33 wherein a_Dx is accurately related to a_Px by a_Dx =(v/u) a_Px ;

and

wherein the spatial phase of said spatially periodic x-ray intensity distribution projected, when said object is absent, onto slab-volume SV3 with period a_Px is carefully aligned with the phase of said detector-pixel array.

35. Apparatus of claim 33 wherein u equals 2 and v equals 1.

36. Apparatus of claim 33 wherein the front surface of said spatially-periodic array of detector-pixels is said spatially-periodic structure within slab-volume SV3.

37. Apparatus of claim 33 wherein said array of detector-pixels is also spatially periodic in direction y so that centroids of the front surfaces of adjacent detector-pixels within said spatially-periodic array are periodically spaced from each other in the direction y by the distance a_Dy.

38. Apparatus of claim 37 wherein said structure within slab-volume SV2 is fabricated and configured to be additionally spatially-periodic within its associated useful y-direction width with period a_2y and with the additional associated periodicity-direction lying in the direction y;

and

wherein, when said object is absent, and for x-rays with at least one energy value that lies within said energy-bandwidth and throughout the associated useful y-direction width of said material structure within slab-volume SV3, then the structures within slab-volumes SV1 and SV2 acting together but not separately project onto slab-volume SV3 an x-ray intensity distribution that is additionally substantially spatially-periodic in direction y with the spatial period a_Py ; and

wherein when the greatest common integer divisor of b and q is 1, then the period a_Py is accurately related to a_2y by

space="preserve" listing-type="equation">a.sub.Py =a.sub.2y (R.sub.1 +R.sub.2)(q p R.sub.1).sup.-1,

and

wherein a_Dy is accurately related to a_Py by a_Dy =(v/u) a_Py ; and

wherein the spatial phase of said spatially periodic x-ray intensity distribution projected when said object is absent onto slab-volume SV3 with period a_Py is carefully aligned with the phase of said detector-pixel array.

39. Apparatus of claim 32 wherein said structure within slab-volume SV3 is spatially-periodic in direction x with the spatial period a_3x ;

and

wherein said structure is oriented within the apparatus so that the periodicity-direction associated with spatial period a_3x lies in the direction x; and

wherein a is accurately related to a_Px by a_3x =v a_Px ; and

wherein the spatial phase of said spatially periodic x-ray intensity distribution projected when said object is absent onto slab-volume SV3 with period a_Px is carefully aligned with the phase of said spatially-periodic structure within slab-volume SV3; and

wherein a_3y is a distance measured in direction y.

40. Apparatus of claim 39 wherein said structure within slab-volume SV3 acts as a spatially-periodic mask;

and

wherein the spatial profile of the intensity distribution of x-rays projected onto slab-volume SV3 is masked by said structure within slab-volume SV3; and

wherein said x-ray image-detector measures said masked profile.

41. Apparatus of claim 40 wherein said structure within slab-volume SV3 is made from a material that absorbs x-rays and is configured so that its spatially-periodic structure acts as said spatially-periodic mask.

42. Apparatus of claim 39 wherein said structure within slab-volume SV3 is made from a fluor material that absorbs x-rays and that responds to said x-ray absorption by the emission of light;

and

wherein said x-ray image detector images the spatial profile of the distribution of light emission by said fluor material.

43. Apparatus of claim 39 wherein said structure within slab-volume SV3 is fabricated and configured to be additionally spatially-periodic within its associated useful y-direction width with period a_3y and with the additional additional periodicity-direction lying in the direction y.

44. Apparatus of claim 43 wherein said structure within slab-volume SV2 is fabricated and configured to be additionally spatially-periodic within its associated useful y-direction width with period a_2y and with the additional associated periodicity-direction lying in the direction y;

and

wherein, when said object is absent, and for x-rays with at least one specific energy value that lies within said energy-bandwidth, and throughout the associated useful x-direction width of said material structure within slab-volume SV3, then the two structures respectively within slab-volumes SV1 and SV2 acting together but not separately project onto slab-volume SV3 an x-ray intensity distribution that is substantially spatially-periodic in direction y with the spatial period a_Py ; and

wherein a_3y is accurately related to a_Py by a_3y =v a_Py ; and

wherein the spatial phase of said spatially periodic x-ray intensity distribution projected when said object is absent onto slab-volume SV3 with period a_Py is carefully aligned with the phase of said detector-pixel array.

45. Apparatus of claim 39 wherein said image that describes the internal structure of said object is divided into image-pixels;

and

wherein each image-pixel has an associated gray-scale for any produced image; and

wherein the quantity w is a positive integer; and

wherein a_Rx is accurately related to a_3x by a_Rx =w a_3x ; and

wherein a_Ry is accurately related to a_3y by a_Ry =w a_3y ; and

wherein each image-pixel is associated with an a_Rx -by-a_Ry area on a slab face of slab-volume SV3; and

wherein each image-pixel has dimensions scaled similarly in directions x and y, and has a width and height that are scaled similarly from the associated distances a_Rx and a_Ry ; and

wherein each image-pixel-associated a_Rx -by-a_Ry area on said slab face of slab-volume SV3 is subdivided into a multiplicity of labeled component areas that includes at least one associated b-labeled area and that includes at least one associated d-labeled area, and also may include other labeled component areas; and

wherein said specific names for said labels are inconsequential, as long as they are applied consistently to produce the same apparatus; and

wherein said other component areas may include one associated c-labeled area, and also may include additional associated b-labeled, c-labeled, and d-labeled areas; and

wherein the b-labels, c-labels, and d-labels within any two a_Rx -by-a_Ry areas on said slab face of slab-volume SV3 are configured to have the same geometric arrangement of said component area labels as each other when the centroids of the two a_Rx -by-a_Ry areas are spaced from each other in the direction x by a distance that is an integral multiple of a_3x ; and

wherein said x-ray image detector is segmented into detector-pixels; and

wherein said x-ray image detector measures simultaneously and independently the intensity of x-rays incident on each detector-pixel; and

wherein said x-ray image detector is segmented and positioned so that simultaneously and independently some of its various detector-pixels measure the intensities of x-rays incident only on associated b-labeled areas and some of its various detector-pixels measure the intensities of x-rays incident only on associated d-labeled areas; and

wherein each of said gray-scales is computed as a function of the measured intensity of x-rays incident on at least one associated b-labeled area and of the measured intensity of x-rays incident on at least one associated d-labeled area; and

wherein said gray-scale computation function also may depend on measured intensities of x-rays incident on additional associated b-labeled areas and also may depend on measured intensities incident on additional associated d-labeled areas; and

wherein said apparatus further includes means for performing said computation.

46. Apparatus of claim 45 wherein said gray-scale computation function includes a weighted linear combination of said measured intensities;

and

wherein at least one weight factor in said linear combination is negative.

47. Apparatus of claim 45 wherein the b-labels, c-labels, and d-labels within any two a_Rx -by-a_Ry areas on said slab face of slab-volume SV3 are configured to have the same geometric arrangement of said component area labels as each other when the centroids of the two a_Rx -by-a_Ry areas are spaced from each other in the direction y by a distance that is an integral multiple of a_3y.

48. Apparatus of claim 45 for producing at least two different images of the same object;

wherein said two different images display different physical properties of said object; and

wherein said x-ray image detector is segmented and positioned so that simultaneously and independently some of its various detector-pixels measure the intensities of x-rays incident only on b-labeled areas and some of its various detector-pixels measure the intensities of x-rays incident only on c-labeled areas and some of its various detector-pixels measure the intensities of x-rays incident only on d-labeled areas; and

wherein each gray-scale for each image-pixel for the first of said two different images is computed as a function of the measured intensity of x-rays incident on at least one associated b-labeled area, and of the measured intensity of x-rays incident on at least one associated c-labeled area, and of of the measured intensity of x-rays incident on at least one associated d-labeled area; and

wherein each gray-scale for each image-pixel for the second of said two different images is computed as a function of the measured intensity of x-rays incident on at least one associated b-labeled area, and of the measured intensity of x-rays incident on at least one associated c-labeled area, and of the measured intensity of x-rays incident on at least one associated d-labeled area; and

wherein the function used for the first of said two different images is different from the function used for the second of said two images.

49. Apparatus of claim 48 wherein a third image is produced, and

wherein said third image is colored, and

wherein one color component of said third image is scaled from the gray-scales of the first image, and

wherein a different color component of said third image is scaled from the gray-scales of the second image.

50. Apparatus of claim 39 for measuring the x-ray refractive-index-gradient structure of an object and for producing an image with edge-enhanced features;

wherein said refractive-index-gradient structure of said object induces a significant change to the intensity distribution of x-rays projected onto slab-volume SV3, relative to said distribution projected when said object is absent; and

wherein the distance a_3x has a sufficiently small value that the interaction of x-rays with said spatially-periodic structure within slab-volume SV3 provides, at least in part, means for detecting said significant change.

51. Apparatus of claim 39 further comprising means for adjusting the relative alignment of the spatially-periodic material structures within slab-volumes SV1, SV2, and SV3;

wherein said means for adjusting the relative alignment of the spatially-periodic material structures within slab-volumes SV1, SV2, and SV3 comprises

means for moving at least two of the three structures within slab-volumes SV1, SV2, and SV3,

a laser that emits light,

a telescope,

a mirror, and

an optical image detector;

wherein said telescope focuses said laser-emitted light; and

wherein the focusing of said telescope is adjustable; and

wherein said mirror transmits x-rays; and

wherein said mirror reflects at least some of said laser-emitted light; and

wherein said optical image detector detects and thereby measures the spatial profile of the intensity distribution of laser-emitted telescope-focused light that is incident upon it; and

wherein said x-ray image detector may serve as said optical image detector; and

wherein said mirror, said laser, and said telescope are positioned so that with appropriate focusing of said telescope said laser-emitted telescope-focused light propagates in the sequential order, first through said structure within slab-volume SV1, next through said structure within slab-volume SV2, next into slab-volume SV3, and then is detected; and

wherein said spatially-periodic structures within slab-volumes SV1, SV2, and SV3 are each made from a material that also interacts with said laser-emitted telescope-focused light; and

wherein with appropriate focusing of said telescope said propagation of laser-emitted telescope-focused light through said spatially-periodic material structure within slab-volume SV1 generates by diffraction Fraunhofer diffraction orders; and

wherein laser-emitted telescope-focused light propagating in at least two of said Fraunhofer diffraction orders that are generated by diffraction of laser-emitted telescope-focused light by material within slab-volume SV1 is incident on said structure within slab-volume SV2; and

wherein the propagation of the laser-emitted telescope-focused light in each of said at least two Fraunhofer diffraction orders through said spatially-periodic material structure within slab-volume SV2 generates by diffraction more Fraunhofer diffraction orders; and

wherein laser-emitted telescope-focused light propagating in one of said Fraunhofer diffraction orders that is generated by diffraction of laser-emitted telescope-focused light by said structure within slab-volume SV2 is incident on a first incidence area on said structure within slab-volume SV3; and

wherein laser-emitted telescope-focused light propagating in a second one of said Fraunhofer diffraction orders that is generated by diffraction of laser-emitted telescope-focused light by said structure within slab-volume SV2 is incident on a second incidence area on said structure within slab-volume SV3; and

wherein said first and second incidence areas overlap; and

wherein by said overlap said laser-emitted telescope-focused light incident within said overlap-area forms a spatially-periodic optical interference pattern on said structure within slab-volume SV3; and

wherein said spatial periodicities of said optical interference pattern and of said spatially-periodic material structure within slab-volume SV3 together create a spatially-periodic moire pattern, if and when their two associated spatial periods are incommensurate; and

wherein said moire pattern is imaged by said optical image detector; and

wherein observations of said moire pattern can be used to guide said relative alignment adjustments.

52. Apparatus of claim 51 further comprised of means for adjusting said laser'"'"'s wavelength,

wherein a small adjustment of said laser'"'"'s wavelength improves said optical interference pattern'"'"'s fringe visibility.

53. Apparatus of claim 51 wherein said laser-emitted telescope-focused light propagating in a third one of said Fraunhofer diffraction orders that is generated by diffraction of laser-emitted telescope-focused light by said spatially-periodic material structure within slab-volume SV2 is incident on a third incidence area on said structure within slab-volume SV3;

and

wherein said first, second, and third incidence areas all overlap on a common three-way overlap-area; and

wherein by said overlap said laser-emitted telescope-focused light incident within said common three-way overlap-area forms said spatially-periodic optical interference pattern on slab-volume SV3.

54. Apparatus of claim 1 wherein said x-ray image detector is further comprised of

a plurality of small x-ray image detectors;

wherein said plurality of small x-ray image detectors can acquire simultaneously a plurality of small images; and

wherein said apparatus is further comprised of

means for combining said plurality of small images to form said image that describes the internal structure of said object.

55. Apparatus of claim 54 wherein said small x-ray image detectors are relatively positioned in a spatially-periodic geometrical pattern.

56. Apparatus of claim 55 wherein said spatially-periodic geometrical pattern includes gaps between said small x-ray image detectors.

57. Apparatus of claim 1 further comprised of

a multiple replication of apparatus component sets;

wherein said replication provides a plurality of x-ray image detectors; and

wherein said replication excludes replication of said object; and

wherein said replication excludes replication of said x-ray source; and

wherein said replication includes, as needed, said contents of slab-volumes SV1, SV2, and SV3; and

wherein said replication of an apparatus component is performed in such a manner that may result simply in the spatial extension of said apparatus component; and

wherein said x-ray source provides a common source of x-ray illumination for said replicated apparatus components; and

wherein each of said sets of replicated components acquires a small image that is descriptive of a portion of the internal structure of said object; and

wherein said sets of replicated components can acquire a plurality of small images simultaneously with each other; and

wherein said apparatus is further comprised of

means for combining said plurality of small images to form said image that describes the internal structure of said object.

58. Apparatus of claim 1 further comprising

means for acquiring and recording a plurality of small images,

means for combining said plurality of small images to form said image that describes the internal structure of said object,

means for acquiring at least one of said small images subsequently in time from another one of said small images, and

means for changing the relative positioning of the apparatus and the object between said temporally subsequent acquisitions of said small images.

59. Apparatus of claim 58 wherein said means for changing said relative positioning of said apparatus and the object is selected from

means for rotationally repositioning said apparatus relative to said object,

means for translationally repositioning said apparatus relative to said object, and

means for rotationally and translationally repositioning said apparatus relative to said object.

9. Apparatus of 8 wherein said source emits x-rays dominantly from a spatially small but finite-size spatial region S, and

wherein W_S is the approximate x-direction width of said finite-size spatial region S within which said dominant emission of x-rays occurs, and

wherein the distance a_1x is substantially smaller than the distance W_S.

60. Apparatus for producing an image that describes the internal structure of an object, comprising

a source of x-rays,

an x-ray image detector;

improved by its further comprising

three very-thin slab-shaped volumes, SV1, SV2, and SV3, each with substantially-planar slab faces oriented relative to each other to be substantially-mutually-parallel, and each containing an associated very-thin material structure that interacts with x-rays, and

means for limiting the energy-bandwidth of detected x-rays;

wherein said three contained structures are positioned between said source and said detector so that x-rays from said source propagate in the sequential, order first through said structure within slab-volume SV1, next through said structure within slab-volume SV2, next through said object, next into slab-volume SV3, and then are detected; and

wherein, when said object is absent, and for x-rays with at least one specific energy value that lies within said energy-bandwidth, and throughout the associated useful x-direction width of said material structure within slab-volume SV3, then the two structures respectively within slab-volumes SV1 and SV2 acting together but not separately project onto slab-volume SV3 an x-ray intensity distribution that is substantially spatially-periodic and has a substantial spatial intensity variation; and

wherein, when said object is absent, and for said x-rays with said specific energy value that lies within said energy-bandwidth, then each of the two structures respectively within slab-volumes SV1 and SV2, acting alone with the other absent, projects onto slab-volume SV3 an x-ray intensity distribution that is different from said spatial distribution projected by said two structures acting together; and

wherein any associated residual spatial periodicity of either of said two distributions projected by said two structures acting alone has a diminished spatial intensity variation relative to said spatial distribution projected by said two structures acting together, and/or has a dominant spatial period that is different from that projected by said two structures acting together.

61. Method for producing an image that describes the internal structure of an object, comprising

providing a source of x-rays, and

providing an x-ray image detector;

wherein said method is improved by its further comprising

providing three very-thin slab-shaped volumes, SV1, SV2, and SV3, each with substantially-planar slab faces oriented relative to each other to be substantially-mutually-parallel, and with each slab-volume containing an associated very-thin material structure that interacts with x-rays; and

positioning said three contained structures between said source and said detector; and

propagating x-rays from said source in the sequential order, first through said structure within slab-volume SV1, next through said structure within slab-volume SV2, next through said object, next into slab-volume SV3, and then detecting the x-rays; and

limiting the energy-bandwidth of the energy spectrum of x-rays that are detected; and

configuring and further positioning the two spatially-periodic structures respectively within slab-volumes SV1 and SV2

so that when said object is absent, and for x-rays with at least one specific energy value that lies within said energy-bandwidth, and throughout the associated useful x-direction width of said material structure within slab-volume SV3, then the two structures respectively within slab-volumes SV1 and SV2 acting together but not separately project onto slab-volume SV3 an x-ray intensity distribution that is substantially spatially-periodic, and

so that when said object is absent, and for said x-rays with said specific energy value that lies within said energy-bandwidth, then each of the two structures respectively within slab-volumes SV1 and SV2, acting alone with the other absent, projects onto slab-volume SV3 an x-ray intensity distribution that is different from said spatial distribution projected by said two structures acting together, and

so that any associated residual spatial periodicity of either of said two distributions projected by said two structures acting alone has a diminished spatial intensity variation relative to said spatial distribution projected by said two structures acting together, and/or has a dominant spatial period that is different from that projected by said two structures acting together.

62. Method of claim 61 wherein said object includes portion of a human body, and

wherein said image is used to diagnose a disorder of said human body.

63. Method of claim 61 further comprising

fabricating the material structure within slab-volume SV2 to be spatially-periodic and with an appropriate structure, spatial period, and from an appropriate material;

and

adjusting the positional spacing between slab-volume SV1 and SV2; and

adjusting the positional spacing between slab-volume SV2 and SV3;

so that

if, hypothetically, with said object absent, said structure within slab-volume SV1 were to be removed and were to be replaced by an infinitesimally-small source of x-rays located at some point within slab-volume SV1, with said x-rays emitted by said infinitesimally-small source having an energy that lies within said energy-bandwidth,

then the structure within slab-volume SV2 would project x-rays from said infinitesimally-small source to form a spatially-periodic x-ray intensity pattern on slab-volume SV3, with said pattern having a significant spatially-periodic spatial intensity variation.

64. Method of claim 63 further comprising

forming said spatially-periodic x-ray intensity pattern on slab-volume SV3 with x-rays from said infinitesimally-small source by

using wave interference of the electromagnetic waves associated with said x-rays, and by

using the fractional-Talbot-effect to provide said wave interference;

wherein the Talbot effect is included as special case of the fractional Talbot effect; and

wherein the formation of spatially-periodic geometric shadows is included as a further special case of the Talbot effect.

65. Method of claim 64 further comprising

controlling the average energy and the energy-bandwidth of x-rays that are detected,

providing an appropriately chosen structure, spatial period, and appropriate material for the structure within slab-volume SV2,

providing an appropriately chosen positional spacing between slab-volume SV1 and SV2, and

providing an appropriately chosen positional spacing between slab-volume SV2 and SV3,

so that aspects of the fractional Talbot effect obtain for the energy-bandwidth limited spectrum of x-rays that are detected.

66. Method of claim 64 further comprising

controlling the average energy and energy-bandwidth of x-rays that are detected,

providing the spectrum of said controlled energy-bandwidth-limited x-rays with a multiplicity of energy component values,

providing an appropriately chosen structure, spatial period, and appropriate material for the structure within slab-volume SV2,

providing an appropriately chosen positional spacing between slab-volume SV1 and SV2, and

providing an appropriately chosen positional spacing between slab-volume SV2 and SV3,

so that aspects of the fractional Talbot effect obtain for low energy x-rays within the energy-bandwidth limited spectrum of x-rays that are detected, and

so that different aspects of the fractional Talbot effect obtain for high energy x-rays within the energy-bandwidth limited spectrum of x-rays that are detected.

67. Method of claim 61 further comprising

fabricating each of the two structures respectively within slab-volumes SV1 and SV2 so that its structure is spatially periodic in at least one periodicity-direction, and

adjusting the orientations of said two structures and associated slab-volumes SV1 and SV2 so that said at least one associated periodicity-direction for slab-volume SV1 and said at least one associated periodicity-direction for slab-volume SV2 are both substantially-parallel to said substantially mutually-parallel slab-faces of said slab-volumes and are substantially-parallel to each other.

68. Method of claim 67 further comprising

fabricating the spatially-periodic material structure within slab-volume SV1 from a material that absorbs x-rays and further configuring said spatially-periodic material structure within slab-volume SV1 with a spatially-periodic distribution of x-ray transmitting portions and x-ray absorbing portions,

so that the spatially-periodic material structure within slab-volume SV1 and said source of x-rays together act as a spatially-periodic source of x-rays, and

further configuring the relationships between the structure and spatial period of the structure within slab-volume SV1, and the structure and spatial period of the structure within slab-volume SV2, the energy-bandwidth-limited x-ray spectrum, and the positional spacing between slab-volume SV1 and SV2, and the positional spacing between slab-volume SV2 and SV3,

so that, when said object is absent, then x-rays emitted by said source and with some energy component within said energy-bandwidth-limited x-ray spectrum source and transmitted by a large multiplicity of x-ray transmitting portions of the spatially-periodic structure within slab-volume SV1 propagate through said structure within slab-volume SV2 to thereby project onto slab-volume SV3 an associated large multiplicity of spatially-periodic x-ray intensity patterns, that each have a spatial period and a spatial phase such that the large multiplicity of intensity patterns reinforce each other in phase, and

so as to maintain by said in-phase reinforcement a substantial intensity spatial variation projected onto slab-volume SV3, and

so as to form by said in-phase reinforcement a high-intensity spatially-periodic x-ray intensity pattern on slab-volume SV3.

69. Method of claim 61 further comprising

fabricating each of the structures respectively within slab-volume SV1 and SV2

so that its structure is spatially periodic in at least two mutually-non-parallel periodicity-directions;

and

adjusting the orientations of said two contained fabricated spatially-periodic material structures and associated slab-volumes

so that said associated first periodicity-directions of the structures respectively within slab-volume SV1 and SV2 are both substantially parallel to said substantially mutually-parallel to slab-faces of said slab-volumes and are substantially parallel to each other, and

so that said associated second periodicity-directions of the structures respectively within slab-volume SV1 and SV2 are both substantially parallel to said substantially mutually-parallel to slab-faces of said slab-volumes and are substantially parallel to each other.

70. Method of claim 61 further comprising

fabricating the structures respectively within slab-volumes SV1 and SV2, each from a material that absorbs x-rays, each with a spatially-periodic arrangement of x-ray transmitting portions and x-ray absorbing portions, and each with an appropriate spatial period,

adjusting the positional spacing between slab-volume SV1 and SV2, and

adjusting the positional spacing between slab-volume SV2 and SV3,

so that the structure within slab-volume SV2 and said infinitesimally-small source of x-rays within slab-volume SV1 together project said spatially-periodic x-ray intensity pattern onto slab-volume SV3 as a spatially-periodic geometric x-ray shadow of said spatially-periodic material structure within slab-volume SV2.

71. Method of claim 61 further comprising

fabricating the structure within slab-volume SV2, from a material that absorbs x-rays, and with a spatially-periodic arrangement of x-ray transmitting portions and x-ray absorbing portions.

72. Method of claim 61 further comprising

fabricating the structure within a slab-volume with a spatially-periodic spatial-thickness-profile that has the approximate form of a periodic step-function.

73. Method of claim 61 further comprising

fabricating a structure within a slab-volume from a material that refracts x-rays, and

fabricating said structure within said slab-volume to be spatially-periodic in at least one periodicity-direction,

so that it then acts as an x-ray phase grating.

74. Method of claim 73 further comprising

fabricating said structure within said slab-volume from a material and with a typical thickness

so as to diminish the absorption of x-rays by said said structure.

75. Method of claim 61 further comprising

fabricating the spatially-periodic material structure within slab-volume SV1 from a material that absorbs x-rays, and

configuring said spatially-periodic material structure within slab-volume SV1 with a spatially-periodic distribution of x-ray transmitting portions and x-ray absorbing portions,

so that the spatially-periodic material structure within slab-volume SV1 and said source of x-rays together act as a spatially-periodic source of x-rays.

76. Method of claim 61 further comprising

providing the spectrum of said energy-bandwidth-limited x-rays with a multiplicity of energy component values,

projecting a first x-ray intensity pattern onto slab-volume SV3 when said object is present using low energy x-rays within said energy-bandwidth limited spectrum, and

projecting a second x-ray intensity pattern onto slab-volume SV3 when said object is present using high energy x-rays within said energy-bandwidth limited spectrum,

so that said first and second patterns are different from each other, and

detecting the difference between said first and second patterns.

77. Method of claim 76 further comprising

creating an image from said difference, and

using said difference to provide information concerning the spatial distribution and material composition of said object.

78. Method of claim 76 further comprising

configuring said energy-bandwidth-limited x-ray spectrum so that at least one of its low energy components has an energy below the energy of an x-ray absorption edge of some chemical element;

configuring said energy-bandwidth-limited x-ray spectrum so that at least one of its high energy components has an energy above the energy of an x-ray absorption edge of some chemical element; and

obtaining said image for an object,

wherein said chemical element is anisotropically distributed within said object.

79. Method of claim 61 further comprising

configuring the x-ray energy bandwidth and the average x-ray energy, the parameters, periodicities, materials, structures, and structural configurations for the contents of slab-volumes SV1, SV2, and SV3, the spacing between slab-volumes SV1 and SV2, and the spacing between slab-volumes SV2 and SV3,

so that, when said object is absent, then a substantially-spatially-periodic x-ray intensity distribution is projected onto slab-volume SV3 by the structures within slab-volumes SV1 and SV2 for x-rays with said energy-bandwidth-limited spectrum.

80. Method of claim 61 for measuring the x-ray refractive-index-gradient structure of an object and for producing an image with edge-enhanced features, further comprising

diminishing the spatial period of said substantially spatially-periodic x-ray intensity distribution projected onto slab-volume SV3 when said object is absent for x-rays with said at least one specific energy,

using the presence of said object and further using said refractive-index-gradient structure of said object to induce significant changes to an intensity distribution of x-rays projected onto slab-volume SV3,

detecting said changes, and

forming an image from the spatial distribution of said changes.

81. Method of claim 61 further comprising

detecting x-rays by

using at least part of said structure within slab-volume SV3 as at least one component of said x-ray image detector.

82. Method of claim 61 further comprising

spatially masking image detection by said x-ray image detector by

using said structure within slab-volume SV3 as a spatially-periodic mask.

83. Method of claim 82 further comprising

configuring the spatially-periodic mask pattern of said structure within slab-volume SV3 by

using a tiling algorithm.

84. Method of claim 61 further comprising

fabricating the material structure within slab-volume SV3 to be spatially-periodic with an appropriate spatial period and with an appropriate spatial structure, and

accurately relatively positioning said structures within slab-volumes SV1, SV2, and SV3,

so that the spatial phase and period of said structure within slab-volume SV3 are accurately harmonically related to the spatial phase and period of said spatially-periodic x-ray intensity distribution projected by said two structures respectively within slab-volumes SV1 and SV2 acting together when said object is absent and with said at least one specific x-ray energy value that lies within said energy-bandwidth.

85. Method of claim 84 further comprising

spatially masking said spatially-periodic x-ray intensity distribution projected by said two structures respectively within slab-volumes SV1 and SV2 acting together when said object is absent and with said at least one specific x-ray energy value that lies within said energy-bandwidth, by

using said structure within slab-volume SV3 as a spatially-periodic mask, and

segmenting said x-ray image detector into a spatially-periodic array of detector-pixels,

accurately positioning said spatially-periodic array of detector-pixels relative to said spatially-periodic masking structure within slab-volume SV3, and

providing an accurate harmonic relationship between the spatial periods of said spatially-periodic array of detector-pixels and of a spatially-periodic x-ray intensity distribution that hypothetically would be projected onto said detector in the absence of said structure within slab-volume SV3 and in the absence of said object by x-rays from said x-ray source and by said structures respectively within slab-volumes SV1 and SV2 all acting together.

86. Method of claim 84 for obtaining accurate relative positions and orientations for said structures that are contained within said slab-volumes, further comprising

providing a source of light;

providing an optical image detector;

wherein said x-ray image detector may serve as said optical image detector; and

fabricating the structures within slab-volumes SV1 and SV2 from a material such said structures within slab-volumes SV1 and SV2 transmit and diffract light;

propagating light in sequence through slab-volume SV1, through slab-volume SV2, and onto slab-volume SV3;

diffracting said light by said structures in slab-volumes SV1 and SV2;

forming a spatially-periodic optical-interference-pattern in said light on slab-volume SV3,

wherein said optical-interference-pattern has a spatial period and periodicity-direction that are directly related to said spatial period and periodicity-direction of said spatially-periodic x-ray intensity distribution projected by said two structures respectively within slab-volumes SV1 and SV2 acting together when said object is absent and with said at least one specific x-ray energy value that lies within said energy-bandwidth; and

forming a moire pattern between said optical-interference-pattern and said spatially-periodic structure within slab-volume SV3;

detecting said moire pattern;

changing said moire pattern by

adjusting the relative positions and orientations of said structures; and

detecting said changes;

adjusting the relative positions and orientations of said structures by

using said detected changes as a guide; and

guiding said adjustments to obtain accurate relative positions and orientations for said structures.

87. Method of claim 86 further comprising

adjusting the wavelength of said light, and

controlling the spectrum of said light, thereby improving said optical-interference-pattern'"'"'s fringe visibility.

88. Method of claim 86 further comprising

focusing said light prior to propagating it through slab-volume SV1,

providing by said diffraction and by said focusing a multiplicity of optical foci near slab-volume SV3, and

adjusting the relative spacings between slab-volumes SV1, SV2 and SV3 so that said foci coincide.

89. Method of claim 86 further comprising

adjusting said relative positions and orientations of said structures by

iterating various adjustment steps;

wherein said various adjustment steps include at least two of the following steps;

focusing said light prior to propagating it through slab-volume SV1 so that its optical focus lies near slab-volume SV1 and then adjusting the position of said structure within slab-volume SV2 as a step,

focusing said light prior to propagating it through slab-volume SV1 so that its optical focus lies near slab-volume SV1 and then adjusting the orientation of said structure within slab-volume SV2 as a step,

focusing said light prior to propagating it through slab-volume SV1 so that its optical focus lies near slab-volume SV2 and then adjusting the position of said structure within slab-volume SV1 as a step,

focusing said light prior to propagating it through slab-volume SV1 so that its optical focus lies near slab-volume SV2 and then adjusting the orientation of said structure within slab-volume SV1 as a step, and

adjusting the wavelength of said light as a step.

90. Method of claim 61 for removing x-ray-scatter-induced unsharpness from said image, further comprising

segmenting said x-ray image detector into a spatially-periodic array of detector-pixels with an appropriate spatial period and with an appropriate spatial structure;

accurately relatively positioning said structures within slab-volumes SV1 and SV2 and said array of detector-pixels

so that the spatial phase and period of said array of detector-pixels are accurately harmonically related to and are phase matched to the spatial phase and period of said spatially-periodic x-ray intensity distribution projected by said two structures respectively within slab-volumes SV1 and SV2 acting together when said object is absent and with said at least one specific x-ray energy value that lies within said energy-bandwidth;

selecting from said array as a spatially-periodic-set a first set of detector-pixels that are illuminated by x-rays in x-ray BRIGHT areas of said projected distribution;

selecting from said array as a spatially-periodic-set a second set of detector-pixels that are illuminated by x-rays in x-ray DARK areas of said projected distribution;

measuring x-ray intensities using said detector-pixel array with said object present;

subtracting intensities measured with said object present by said second set of detector-pixels from intensities measured with said object present by said first set of detector-pixels; and

forming an image from said subtracted intensities.

91. Method of claim 90 wherein detector-pixels are selected from said array as spatially-periodic-sets, further comprising

configuring said spatially-periodic-sets of detector-pixels via a tiling algorithm, and

configuring said spatially-periodic-sets of detector-pixels so that different sets are disjoint, and

configuring said spatially-periodic-sets of detector-pixels so that different sets of detector-pixels are spatially interlaced with each other, and

configuring said spatially-periodic-sets of detector-pixels so that each set provides sparse spatially-periodic array of detector pixels.

92. Method of claim 90 for producing at least two different images of the same object,

wherein said two different images display different physical properties of said object, further comprising

selecting from said array as a spatially-periodic-set a third set of detector-pixels,

using a first algorithm to provide a first image from x-ray intensities measured when said object is present by said first, second and third sets of detector pixels, and

using a second algorithm to provide a second image from x-ray intensities measured when said object is present by said first, second and third sets of detector pixels,

wherein said first algorithm is different from said second algorithm.

93. Method of claim 61 further comprising

acquiring and recording data for a plurality of partial images,

wherein each of said partial images describes a portion of the internal structure of said object;

and

synthesizing said partial images;

thereby

forming an image that describes the internal structure of said object.

94. Method of claim 93 further comprising

configuring said x-ray image detector as of a plurality of partial-image detectors, and

acquiring said data for said plurality of partial images by

detecting x-rays with said plurality of partial-image detectors.

95. Method of claim 93 further comprising

acquiring said data for said plurality of partial images as a sequence of temporally-spaced data-acquisition steps;

and

using the same x-ray image detector sequentially more than once during said temporal sequence of steps.

96. Method of claim 95 further comprising

repositioning said structures that lie within slab-volumes SV1, SV2, and SV3, and said x-ray image detector relative to said object while

maintaining the relative positioning of said structures that lie within slab-volumes SV1, SV2, and SV3, and said x-ray image detector, and

performing said relative repositioning between data-acquisition steps as a step in said temporal sequence.

97. Method of claim 96 wherein said relative repositioning is comprised of

rotating said structures that lie within slab-volumes SV1, SV2, and SV3, and said x-ray image detector, relative to said object.

98. Method of claim 96 wherein said relative repositioning is comprised of

translating linearly said structures that lie within slab-volumes SV1, SV2, and SV3, and said x-ray image detector, relative to said object.

99. Method of claim 96 wherein said relative repositioning is comprised of

simultaneously translating linearly and rotating said structures that lie within slab-volumes SV1, SV2, and SV3, and said x-ray image detector, relative to said object, thereby

providing helical trajectories for the motions of said structures and detector.

100. Method of claim 93 for producing an image that describes the three-dimensional internal structure of an object, wherein said synthesizing is comprised of

performing a tomographic transformation of acquired image data.