A COMPUTER TOMOGRAPHIC METHOD AND A COMPUTER TOMOGRAPH

Abstract: In conventional backprojection, each pixel value is calculated separately. With N pixels N<3> additions are necessary. According to the invention, the summation is instead divided into partial sums which are then used to form new partial sums in a hierarchical way. A substantial computational reduction is obtained because a partial sum has approximately the same value for many neighbouring points, and that interpolations are feasible. Instead of N<3> additions, the number of additions can be reduced to the order of magnitude of N<2> log N.

Description: A computer tomographic method and a computer tomograph Introduction The present invention regards computer tomography and methods of evaluating tomography data. The method of the invention can be applied to all kinds of tomographic imagmg, whether registered by X-ray or radioactive absorption, by magnetic resonance (MR) or positron emission tomography (PET). In all those cases are obtained experimental values in the form of line mtegrals along multitudes of straight lmes The typical CT measurement consists of mounting an X-ray tube on a ro- tatable circular πng and a set of detectors m a row opposite the tube. The invention therefore regards a computer tomography method of the land recited in the preamble of claim 1 In computerized tomographic imagmg (CT) the mverse problem consists of determining a function from its line mtegrals We examine three different types of measured data sets, with diffeient scanmng geometries, namely two versions of parallel scanning (smogram. linogram) and fan-beam scanning (even cone-beam scanning) We will study the Filtered Backprojecnon Method (FBM) which is one of the most well-known and widely used methods The reason for the widh use of the filtered backpiojection algorithm is die high image quality. A. seπous problem m prior an evaluation of tomographic data in order to obtain an image is the heavy computational complexity for the back-projection operator, which is of the order N\ It is the general object of the invention to obtain an improved method of transforrmng tomographic data mto images, which is less complex and can give improvement either in computanonal speed or in an increased number of voxels/pixels in an image This object and other objects and advantages are obtained, according to the invention, by means of a computer tomography method of the kind recited, which is characterized by the steps recited in claim 1 Advantageous embodiments are recited in dependent claims In conventional backprojection each pixel value is calculated separately, which means that (9(N) operations are required for each pixel. Then the total number of operations will be of the order (3(N J ). Instead of directly doing the N 3 additions the basic idea behind the new algoπthm is to divide the summation into partial sums, which then are used to form new partial sums m a dyadic and hierarchial way, see Figure 1 The reason for this procedure is the benefit in computational reduction due to the fact that a partial sum has approximately the same value for many neighbouring points Thus each value of a partial sum is calculated once, but used several times when forming a new partial sum from two partial sums in a preceding level of the hierarchy Although in the present description, the invention is exemplified with forming hier- achial partial sums m a dyadic way, which is presently believed to be the best mode, it is also possible to sum more than two groups, namely, each time a number which is a prime number It is even not necessary to use the same prime number in each stage In a preferred embodiment, families of lines are combmed two and two, indicating that the total number of line families is a power of two. With a number of pixels/voxels of 512 x 512 an an equal number of families, i.e. angles of registration, this condition is fulfilled. However, without using the full advantages of the invention, it is possible m the partial sum calculation to combine three (or five, or any prime number) space distributions by making sums for those points where the lines for the largest angular difference mtersect, and adding interpolation values for the further distributions. It is also possible to add line integrals for intermediate lines, for which no measurement was made, i.e by sernng intermediate (non-measured) line mtegrals to the mean value of the adjacent lmes, for which a measurement was made. Although the method is most easily understood for a case where all the line families belong to the same plane, which is the most common configuration in practice, and which is exemplified as xhe fan-type, the smogram and the linogram, it may also be adapted to the cone-beam case, where radianon from a source fills a cone, and detection is made in a two-dimensional array of detectors. Each detector men corresponds to a line through the field swept, and the contraption and the object are mutually rotated As shall be shown, a considerable saving in calculations may be obtained also this case In a special case, where each family of lmes consists of Lines which are mutually - parallel, it is possible, in a very favourable way, to obtain values for points which are equidistant in a rectangular screen pattern. This is obtained by making me two last line families, for which sums at intersections are calculated, be at mutually right angles Thereby , in principle, the last repeated second step is performed by two combined gro ps, symmetrized in relaπon to a direction at right angles to an angle belonging to a family of lmes which is at an extreme end of said enumerable order, thus obtaining a set of sum values which correspond to pixels in a cartesian system of screen pattern List of Figures 1 The sumπαac on process for N = 3 21 2 Division of the (.-: * , H-plane f ° r I'{ , ι. k'. f) 21 3 Division of che O-plane for I'(l. ι, k', l') 22 4 Division of che (k", l ")-plaae for I'{j, ι, k l") 23 5 Cone-beam geometry 24 6 Points of mcerseccion for the partial sum [(j. i. k. l. m) . . . 2 ..-> 2 The filtered backprojection algorithm for sinogram In the parallel scanning geometry a cross-section of the human body is scanned by a set of equally spaced parallel X-ray beams for a number of equally distributed directions. Thus the recorded detector values correspond to a discrete set of values from the Radon transform. The (n-dimensional) Radon transform of a function / on R n is defined by (Rf)(θ, s) = I f(X) dX, X θ=s which is the integral of / over the hyperplane whose normal is θ <E S n~ l , the unit sphere in R n , and with (signed) distance s € R l from the origin. The term sinogram is chosen since an attenuation function consisting of a (5-function, Dirac function, gives a Radon transform supported on a sinusoid in parameter space, i.e., (θ, s)-space. Before giving the inversion formula we will describe the backprojection. The (n-dimensional) backprojection operator R i maps a function g on S n~ i x R 1 into the set of functions on R n . The backprojection operator is defined by (Rtg) (X) = jf ^ g(θ, X ■ θ) dθ, X E R n . R i is the dual operator of R. Hence / (Rf)(θ, s) g(θ, s) dsdθ = I f(X) (R i g)(X) dX. The filtered backprojection algorithm is a numerical implementation of the inversion formula / = I (2T) 1 -" R u H n - l {Rf) in - y) . where H denotes the Hubert transform and (-) (n_1) denotes the (n-l)st derivative both with respect to the variable s. 3 Fast backprojection for sinogram In this section we will develope a method for backprojection. requiring only 0(N 2 \ogN) operations. This method can be used on the (n-dimensional) backprojection operator but in order to describe the main idea it suffices to study the case n — 2. Then (R i g)(X)= f g(Θ.X-θ)dθ, where X = 6 S l , or. with slightly different notation, (R i g)(x,y)= / g(υ,xcosυ + ysinυ) dυ. Strictly we should write g(θ(υ),xcosυ -f ysinv). We assume that g{θ,s) satisfies the condition g(—θ, —s) = g(θ, s) which implies that g(v -f- π, — s) = g(v, s). Then ( Rg) (x, y) = 2 / g(v, x cos v + y sin v) dv. Let g(υ, s) be sampled at the points g(v m , s n ) where N — 2 J , J positive integer. In order to compute the backprojection, we need to calculate the sums for A: 2 + - 2 < ^ j -, where A; and I are integers. Since ø is defined on a rectangular grid we might use linear interpolation for the variable s in the sum of formula 3.1. We choose instead the following procedure. First extend the definition of g by increasing the number of sampling points in the s-coordinate with a factor e, using linear interpolation, and introduce the notation for m = 0, ..., N - 1 and n = -≤f , ..., . Then, take 7 ' ] ) ~ Σ G(m, [e(fc cos u m + . sin u m )])., where [α] denotes α rounded to the nearest integer. Now, instead of directly doing the N 3 additions we will divide the summation into partial sums, which then are used to form new partial sums in a hierarchial way. The reason for this procedure is the benefit in computational reduction, due to the fact that a partial sum has the same value for many neighbouring points. First we define i-2->-l I(j.i,k,l)= ∑ G(m,[e(kcosυ m ÷lsi v m )]) m=(ι-l)-2^ for 0 < j < J, 1 < i < 2 J~j . Then we have the following simple relation I(j,i,k.l) = I(j-l,2i-l,kJ) + I(j-l,2i,k,l). In the following description we will show that the number of points (k,l) where the value of the partial sum I(j, i. k. I) has to be calculated is approximately twice as large as the number of points where the value of a partial sum I(j — l,i,k,l) has to be calculated. Hence, since the number of partial sums with different i- values at level j is N/2 3 , the total number of summation points for all partial sums at level j is approximately the same as for level j — I and since there are J = 2 log N j-levels we conclude that the total number of operations for all levels will be proportional to N 2 lo N. The variable i just stands for a rotation about the origin. Thus it will be convenient to make the following definition 2'-l I'(j,i,k .l') = ∑ G(m + (i- 1) ■ 2> .[e(k * cosυ m + T s v m ))). m=0 Then we have I(j,i,k,l) (3.2) = I * (j,i,kcosv(i-.i)2i + - ' sinι/( i _ i ), I Jcosu(j_ι.)2J — A ; sinι/(,_ι)2 ) and By definition we have We now see that / * (0. i. k{, t[) = I"(0. i, A-..], l 2 * ) if the points (k{. l\) and (JfcJ, l 2 *) are located in the same strip, see Figure 2. Now consider the next level, =l. We have r(l, ι. k', I') = C(2ι - 2, [ek'\) + G(2ι - 1. [e(k * cos υ x ÷ I' sin Vi )}), and we conclude that 7 * (1. i. k * . / * ) = 7 * (l, ι, k*_. I*) if (k{, / * ) and (Jfc.]. .J) are located in the same region, see Figure 3. Let e A ;- « cos vι ■ +- 1 r . sm vi = - ^ e According to Figure 3 it will be necessary to calculate 7 * (1, i. k* , I*) only for a and b integers. Therefore we mtroduce, general A; * and I * will not be integers. ϊ(l, ι, a, b) = I'(l. ι, k * , r) where a — ek" b = e(k' cos υ - / * sin Vι) Hence 1(1, i, a. b) = G(2ι - 2. a) + G(2ι - 1, b) Can we do a similar division of the (A; * , / * )-plane for I"(j, ι, k*, l") , > 1? Let * * = k _. • cosuoj.i + , 1 ;• sm • t^-i = - b e If two points (k{. l ) and (k 2 , I * ,) are in the same region, see Figure 4, we want r(j,i,kuι) = ι*(j,ι.ti.r 2 ). . \(k{ - k;) cos^ m + (l[ - .;) smt/ TO | < - (3.4) e for = 0, ..., 2 J - 1. In Figure 4 we see that all regions approximately satisfy condition (3.4) if u 2) _ι < , which corresponds to j < J — 1. In the same way as for j = l we introduce ϊ(j,ι,a,b) = r(j.i,k',n (3.5) where a = ek * b = e( ; * cosu 2 j_i -)- I'sinvj-i) By equations (3.3) and (3.5) we see that we have the following relation - l,2t-l,a,b l ) + ϊ(3-l,2ι,a l ,b) (3.6) where and By symmetry we have ϊ{j,i,b,a) « /( - l,2i - 1,6,0 + 7 - 1.2ϊ,δι,o) /(j, i, -α, -6) « /(j - 1, 2t - 1, -α, -0ι) + /(j/ - 1, 2ι, -oi, -6) and ϊ(j, i. a. a) z ϊ(j — l, 2i — l, a, aι) -r ϊ(j — 1.2? ' , a x . a) where which means that we only have to compute αi and b for 0 < a < \b\. The procedure suggested by this discussion of the partial sums leads to the following algorithm. We start by adding "extra" sample values by linear interpolation. Then we form partial sums of adjacent pairwise projections ( A projection m consists of all sample points G(m, n) where rn is fixed. ). The next step will be to form partial sums of four projections by adding two adjacent sums from the previous step. Thereafter we will subsequently form partial sums of 8, 16,32, ...projections. The iteration stops when full backprojection is obtained, that is, when the sum consists of all projections. A partial sum is only determined in points where two lines intersect whose angles are v 0 and v 2> -ι, with respect to the (A; * , / * )-plane, and whose perpendicular distances to the origin are ^ and ^ respectively, n t and π 2 integers. If e > 2 the process is stopped before we obtain /(J — 1, i, a, b). If the total number of points where the partial sums, at level j. are calculated is of the same order as the number of pixels, the process is stopped and the pixels are interpolated directly from the values of the partial sums at level j — 1. The pixel values are then calculated from equation (3.2). When e = 1 we calculate all the partial sums up to /(J — 1, i, α, b). Although the number of points where I(J — l, i, a, b) is calculated is of the same order as the number of pixels they do not coincide. This is caused by U j-i --, = f - f • Therefore we have to calculate the pixel values by equation (3.2) which is unnecessary if we instead do the following. We want to calculate .V/2 ∑ G(m, [k cos v m + I sin v m ]) (3.9) m=0 and ;V 53 G(m. [k cos v m + l smv m ])- (3.10) m=N/2 But now v N / — VQ = V N — v^/ 2 = so the points where we calculate the sums are in fact the pixels. One problem is that each sum, (3.9) and (3.10), consist of 2 ;_ i -I- 1 elements. However in order for the summation process to work, the number of elements in a sum has to be a power of two. Therefore we calculate ∑^Q 1 , ∑^ ' N μ + ∑mϊv/2 and ∑ΪLΛN/ +I - Then and Note that since the partial sums ∑ i 0 and ∑ ,= / 2 both contain the projection rn = N/2 and the projection m = 0 ~ m = N, we do the following. We assign the projections the values G(N/2, π) = 0 and G(0, π) = 0 in one of the partial sums. The total number of different values for ^ or - l = , k 2 + I 2 < ^, is If and i are fixed then the number of points where we calculate ϊ(j, i, a, b) is approximately the area of the circle, E -, divided by the area of one region ( ^rhomb), . c_. sin' V.n j _ , , i.e., e 221 4 - sin ϊΛv, -ι - Hence the total number of points a jt. i level l j ■ , i 1 = e 2 τ 2 V 2 "" -TI ' When j is small, ( =l, 2, 3.), the overlapping of the circle by rhombs is not so efficient but then -^ = ^, f , . Hence the total number of points for all levels is e"τr < -— A- log N ÷ N 2 (e - l) for e > 2 and 7T < Λ , ' -2 log N for e = 1. 4 The filtered backprojection algorithm for linogram In 1987 a new reconstruction algorithm was developed by Edholm [Edh87]. It is called the linogram method and is similar to the direct Fourier method but it is based on a different scanning geometry. In the parallel scanning geometry for sinogram, the projection lines. X-rays, are taken for a number of equally distributed directions which requires the detectors to rotate around the object. The linogram projections actually consist of two sets of projections. In the first linogram the detectors and the transmitters lie equally spaced on fixed lines parallel to the rr-axis and the projection angles are —45° < θ < 45°. Instead of equally distributed directions, Δ0=constant, we now get Δ tan f?=constant. In the second linogram the detectors and transmitters lie equally spaced on fixed lines parallel to the y-axis and 45° < θ < 135°,(Δcot(9=constant). Instead of the Radon transform it now will be natural to study the two linogram operators Ri and R 2 . and The term linogram is chosen since an attenuation function consisting of a (5-function gives a i? r and β 2 -transform supported on a line in parameter space, i.e.. (u, t/)-space. There exist dual operators, backprojection operators, R\ and R 2 iven by and f∞ -OO I (R l f)(u,υ)g(u.v)dudv= l f(x.y)(R[g](x,y)dxdy -OO J —OC ' _! _ R2f U ' V)9{U ' V) dUdV = S-oo i-oa (X ' V) (^) (X ' V) dXdy - The filtered backprojection algorithm for linogram is a numerical implementation of the inversion formula where H denotes the Hubert transform and ( ■ ) (1) denotes the derivative both with respect to the variable u. 5 Fast backprojection for linogram Here the procedure of summation for the backprojection is analogous to the one used for sinogram. It suffices to study the backprojection R and projection data from Ri since R 2 and R corresponds to a rotation about the origin of 90 c degrees. We want to determine (x, y) in the pixels (x, y) = (τ ) ) . N = 2 J where J is a positive integer and A:, I integers belonging to the disk k 2 + I 2 < ^. Then the function g(u. v) has to be sampled in the points g{u m , v n ), v n — n- n — — and u m = m-— , m integer, for all g(u m , υ n ) where the corresponding projection line intersect the unit circle. Therefore the number of parallel projection lines depends on the projection angle. For instance if n = 0 we have \m\ < y but if n = y we have \m\ < 2^-. We will divide the summation. into partial sums in the same way as we did for sinogram. In order for the summation process to work, the number of elements in a sum has to be a power of two. Therefore we start by splitting the summation in the following ay. + v n -i) t v n ) (5.11) N/2 -i Then we divide the sum ∑ into partial sums ( The procedure for ∑ is n=l n=-N/2 similar ). Define for 0 < j < J— 1.1 < i < 2 J~J~1 . The procedure suggested by this discussion of the partial sums is analogous to the method described in section 3 on page 8. A partial sum I(j, i. k, I) is only determined in points where two projection lines intersect, one projection line corresponds to and the other to υ t 2 , . If the projection line, which corresponds to (u a , U ( ,_ I) . 2 J+ I ). intersects the projection line, which corresponds to (uj,, v,. 21 ) , at the point ( ι,a,b j .ι, . b ) in the (A .)-plane we will use the notation ϊ(j, i. a, b) = I( , i, k Jtl<aιb , l 3ll , a ,b)- The projection line x = U m — υ n ■ y is the straight line through the points (m + n, —N/2) and (rn — n, N/2) in the (k, .)-plane. We have r jfc » j,ι,a,b , - — Ω u . 2 x ; V -l b U f '- 2 1 J ) -- J 1^ 1 ' 7 ,t,α,6 — 2J-1 Since we only are interested in points on the disc k 2 4- 1 2 < ^ N- 2 we get \b-a\ <2> -1. We obtain a similar relation for linogram as relation (3.6) for sinogram We have I(j, i, a, b) « ϊ(j - 1, % - 1. , 6 -- /(j - 1, 2z. α λ , 6) where and 2^- 1 2 J-1 — 1 2- 7-1 — 1 6ι = ~ — - a — ^- — 6 = a - 1 - - (6 — ) 2^ — 1 2^-1 2^ — 1 One major advantage of linogram compared to sinogram is that in the equations for αi and 6ι the terms which not are integers depend only on the difference b — α Then if we use linear interpolation the interpolation factors will be constant if b = b — a =constant Hence if we introduce the notation I(j,ι,a.b) = ϊ{j,ι,a,a-rb) we finallv obtain the simple and very effective summation algorithm « (1 - c)T(j - 12% - 1 a b - A) -*- cϊ(j - 12; - 1, , 6 - .4 - 1) + (1 - c)I(j -l.2ι,a- L -A b-A) + cl(j - 1, 2ι, α J - + 1, b - A - 1) where 6- 3 7 3 7 = A+c A integer and 0 < c < 1 Since c = 0 for b = 0, ±(2 J -1) and by using that we have the same interpolation factors for ±6, we only have to compute for 1 < b < 2 J -2 ( Let 1 < b < 2 3 -2 and b f j = A + c, A integer and 0 < c < 1 Then -b • ^ = - A - 1 + (1 - c) ) For sinogram, however, we had to compute a \ and b \ for all combinations of (a, b), a > b. Therefore the total number of times αi and 61 have to be computed, at level j, is approximately 2(2 J - 1)/V for sinogram. Hence although the number of summation points (a. b) is approximately the same for linogram and smogram the total computational complexity for a,ι and 61 . is O(N) for linogram but 0(N 2 ) for sinogram. Finally we calculate according to equation (5.11). Let 7ϊ(a, b) = ϊ(J - 1, 1. a, b) and I2(a, b) for the corresponding partial sum ∑ 9 (k + V-n - l). V- n ) , where a corresponds to the direction ι/_ι and b = a + b corresponds to the direction υ_,v/2- Then for 0 < I < N/2. The total computational complexity for the filtered fast backprojection algorithm for the linogram geometry is the same as for the sinogram geometry, i.e., N 2 log N. 6 Cone-beam and Fan-beam geometry The most common scanning geometries in medical tomography are the cone- beam geometry in the three-dimensional case, and the analogous fan-beam geometry in the two-dimensional case. In cone-beam scanning an X-ray source is rotating around the object along a circle while emitting cones of X-rays, which are recorded by a two-dimensional detector. In fan-beam scanning the cone-beams are screened off to a single plane and consequently recorded by a one-dimensional detector. Feldkamp, Davis and Kreiss [Fel84] have developed an approximate 3D-reconstruction algorithm for cone-beam projections. The computational complexity is of the order 0(N 4 ) for an image / of N x N x Nx pixels. By using the same technique as we did for the previous backprojection algorithms we will reduce the number of operations to C(Λ τ3 lo N). Next we will describe the cone-beam geometry. Let the position of the X-ray source be denoted by S(λ), where 0 < λ < 2π and r constant. Hence the X-ray source rotates around the object along a circle in the zy-plane. The detector plane is always perpendicular to the vector (λ), see Figure 5. Hence it will be practical to introduce the plane spanned by the normed vectors p(λ) and z, where p(λ) is the vector in the xy-p\a,ne which is perpendicular to S(λ), see Figure 5. Then the measured data can be represented by a discrete set of values from -7( ,p,g)= J f(x)dx. -.(A.p.f) where L(\.p,q) is the straight line through the points S(X) and D(p,q) == pp(X) + qz. Now the approximate inversion formula can be written as [Fel84] 1 /(£) = A(λ, x) 2 G{X, A(λ, x)x ■ p(X), A(X, x)z) dλ, (6.12) 4τr 2 Jo w here A(X,x) r 2 -x-5(λ) and {l, F.I) ii,F- l .i) G{λ,p.q) = \σ\ , \S(X)-D(p,q)\ 9( P,Q) [X. σ, q) (λ,P,<?), i.e., we multiply the projection dataρ(λ,p, q) with a weight function .^. ^, — ΓT and then perform a rampfiltering in the variable p. The final backprojection in (6.12) is computationally the most heavy part of the inversion algorithm. The major difference between this backprojection and all the previous is the weight function A(X,x). Now let g(X,p.q) be sampled at the points g(X a ,Pb, Qc) where, r > 1 and N = 2 J . with J integer, and we want to estimate f(x) in the points Xk.i.m = (%k, yι, Zm) — ( , j, η^j , k,l and m integers, for k 2 + I 2 ÷ τn 2 < ^- . Thus ι 2ιV-l ~ -r— r - ∑ A(X a , Xk. m) 2 G(X a , (λ α , XkΛ,m)Xk.l,m ■ P(λ β ), A(X a , Xk,l,m)Zm), 4ττ^ α -^o w here A{X a ,Xk,ι,m) = = A(a,k,l) and X k ,ι ,m -p(λ β ) = Xfcsinλ α - yι cos λ α = (x-p){a,k,l). If we now divide the sum into partial sums in the same way as we did in section 3 we get 53 A(a. k, l G(X a , A(a, k, l)(x ■ p)(a, k, l),A(a, k. l)z m ). α=(t-l)-2J Now if the interval is small, i.e. j small, we can make the approximation A(a.k,l) vA(a JιX .k.l) (6.13) where a. jιX = % • 2 J — (2 j + l)/2. the average angle. Thus t-2->-l -4(α jιt , k, I) 2 5Z G ( λ <" A (H k > (* ■ P)( Q ; k, I), A(a jιtl k. l)z m ). a={x-ιyv Define i-2-»-l I(j,i,k,l,m)= G(λ α ,( -p)(α,A ; , ,- )- α=(t-l)-2> Then as before J( , t, A;, Z, m) = I(j - 1, 2t - 1, A, , ) + /( - 1, 2i, k, I, m). A partial sum is only determined in points where two projection lines, projected on the xy-pl&ne. intersect one projection line coming from S X ( ,_ιy 2] ) and the other from -?(λ,. 2J _, ), see Figure 6. Now since .4(λ, x) obviously can't be approximated by a constant for all λ, except x = 0, the iteration process is stopped after a few steps, at level JO > and the pixels are interpolated directly from the values of the partial sums at level j Q . We have ~ k, 1)1, A(a n , t , k. l)m). At a first glance the method seems to be far less efficient for this backprojection than for the previous ones. But if we consider that the level j — I reduces the number of summations by half and j = 2 to approximately a fourth of the original number, and so on, we see that it is almost as efficient as the other. The accuracy of the approximation (6.13) depends strongly on the distance between the point (k, I) and the origin, i.e., But since the inversion formula (6.12) is correct only for points in the plane z = 0 and the artifacts in the other planes z = m increase with the absolute value of rn the region of interest usually is k + I 2 -r- m 2 « r. For (k, l) fixed point the accuracy of (6.13) depends on the angle difference -I — λ ( ,_ 1) 2 j not on the number of elements. 2 ] , in the partial sum. 2 ] - 1 1 -I — λ(j_ι).2r = TΓ — — — Hence if N — 2 J corresponds to that the iteration process is stopped at level jo then 2N corresponds to that the iteration process is stopped at level j 0 -f- 1 in order to have the same accuracy for the approximation (6.13). Then if the region of interest consists of n 3 pixels the number of operations for the back- projection will be of the order 0(n 2 N log N). In the two-dimensional case, fan-beam scanning, the procedure is identical, m = 0. Hence if the region of interest is of size n 2 the computational complexity will be 0(nN log N). References [Edh87j P.R. Edholm. G.T. Herman. Linograms in image reconstruction from projections IEEE Transactions on medical imaging, Vol. MI- 6. pp.301-307. 1987. [Fel84] L.A. Feldkamp. L.C. Davis, J.W. Kress, Practical cone beam algorithms Journal of optical soc. Am., Vcl. A6. pp.612-619, 1984. [Νat86] F. Natterer, The mathematics of computerized tomography John Wiley & Sons Ltd, Chichester, 1986. [Radl7] J. Radon. Uber die bestimmung von funktionen durch ihre integral- werte langs gewisser manmgfaltigkeiten Ber. Verh. Sachs. Akad. 69, p.262. 1917. Instead of using the approximation (6.13) we can even perform the multiplication of the weight function in an iterative way. In order to describe the main idea it suffices to study the two-dimensional case.2 = 0. the extension to the case z φ 0 is obvious. We introduce the notations x = R-, y ) L{X.p) = L(X,p,Q) and i 2-»-l I(j,i,x)= ∑ A(X a ,x) 2 G(X a .A(X a ,x)x-p{X a )). α=(»-l)-2J Let x(j,ι,pι,p 2 ) denote the point of intersection between the lines 7-(λ (l _ 1) . 2 j,2pι/ ' ) and L(X l . 2} _ i ,2p 2 /N). Then we will use the notation We obtain a similar relation as (3.6) Hj,i,Pi,P2) ~Ki ~ l,2i- - 1.2i,d 2 ,p 2 ), where d \ and d are calculated in a similar way as equations (3.7) and (3.8) for aj and b x . In general d x and d will not be integers. In order to obtain the correct value of the weight function we will apply the following procedure. We will only consider the partial sum I{j — l,2ι — l, ι.d ) the procedure for ϊ(j — 1,2., d , p ) is analogous. We start by only consider the term which corresponds to a = (i — 1) • 2° -- 2 }~1 — 1, i.e., A(X i ,x l ) 2 G(X i ,2d 1 /N) « A(Xi, Xi) 2 ( c t G(Xά, 2^3/N) -r c 2 G(X ά , 2([d 1 ] + 1)/N)) +c 2 A , Xa~ ' A(X a -, x 3 ) 2 C(λ 5 , 2{[d x ] + 1)/N), ^ ■ \ Λ ά^Xi) " where £-, = x(j — 1, 2£ — l,pι,dι), x 2 = x(j - l,2i- l,pι, [c-ι]) ; x 3 = x(j - 1, 2i - l,pι, [dι] + 1), d x = [r,] -f c 2 , 0 < c 2 < 1 and c x + c 2 = 1. Therefore we will use the following approximation ϊ(j -l,2ι- l.p^i;) « Cl ^ ^ /(j - 1,2* - l, Pl) ft]) +c 2 ^TTT ^ ^ - 1- 2z - l )Pll [d x ] + 1), Λ^Λύ- 3J where ά = (i — 1) • 2 J - 2 ]~1 — 1. In order for the approximation to be accurate for all terms in the partial sum ϊ(j — l,2ι — l,p x .d ) all weight functions which belong to the partial sum have to satisfy the condition A(Λ αl ,x(j - l,2i-l.p x ,d γ )) 2 _ A(X a2 .x(j-1.2ι-l,p x ,d x )) 2 A(X aX ,x(j- 1.2ι-l.p x ,d) - ~ A(X a2 ,x( - l,2ι-l.p d)) ' iov(ι-l)-2 ] <ol,o2< {ι-l)-2 i ÷2 J - l -l<md[d x ] <d< [d x ]÷l. The error obtains its maximum when l = (1 — 1) ■ 2 J and α2 = (1 — 1) ■ 2 J ÷ 2 J~l — 1. It suffices to consider the case A(0,x( - 1, pχ.d x )) 2 _ A(X.x(j - 1, l.pi.di)) 2 A(0,x(j-l,l, Pl ,d))* ~ ^(λ^U- i .p ! ,-.)) 2 ' for i = 1 and λ = 2 3~l - 1. The points x( - 1. l.pi.di) and xl - 1, l,pι,fi) are located on the fine (0, 2p x /N) which can be written Let x(j - 1, l,pι,dι) = x{t x ) and £(ji - 1, l,p x ,d) = x(f). Then (0,x(r ) = ^ and A(0,x(£)) = 7 e have ^ t l + (^)(l-cosA)-^sinΛ _ t = A(0,x( )) ~ t x i + (!=£_.) (i _ cosλ) - 2*. sin λ ~ *ι (0, (*)) ' The number of points of intersection increase with λ. In fact we have l*ι - *l κ / - Hence 1 1--tt for some constant c. At the first steps of the iteration the error will be extremely small oc 1/N 2 and then increase to o 1/N at the final step. Now we return to the three-dimensional case, z ψ 0. We introduce the notations i-2>-l I(j, i, x, z) = Z i4 ( λ "- ^) 2 G{X a , A(Xa, x) ■ p(λ α ), A(X a , x)z) α=(t-l)-2-' and ϊ(J, P P2,z) = I(j,i,x(j,i,pι,P2),z). We have the relation HJ,I,P P 2 ,Z) ~ ϊ(j - l,2z- l,p x ,d x ,z) + ϊ(j - l,2i,d 2 ,p ,z), We will use the same approximation as before the only difference is that we have to adjust the value of the variable z. ϊ(j-l,2i-l,p x ,[d x ],z ) where ά = (i - 1) • V + 2 3~l - 1, A = (i - 1) • 2 ] + (2 j ~ l - l)/2 the average angle and z ■ A(X,x x ) = ri ■ i4(λ,x 2 ) = 2 2 • A(λ,x 3 ). In general z x and z 2 are not integers but since the weight function and the points of intersection 2 and x 3 are independent of z we can perform an interpolation of the variable z in the usual way. The accuracy of the approximation in the .r-direction depends on the previous condition, i.e., A(X,ϊι) _ .4(A B ,Jι) and A(X,xι) _ A(X a ,x ) A(X,x 2 ) ~ (λ α , 2 ) n A(X,x 3 ) ~ A(X a ,x 3 ) for (i - 1) ■ 2 j < a < (i - 1) • 2 j + 2 "1 - 1.

Claims: Claims 1. A computer tomography method for obtaining a mapping of a variable in an object, said variable being measured in the form of line integral values over a multi- tude of lines, crossing said object, the multitude of measured lines being subdivided into families of lines, which families are enumerable in an order determined by successive relative angular shifts between patterns of lines in successive families, characterized in that a) in a first step, groups are combined out of said families, each group consisting of a first prime number of families of lines having adjacent positions in said order, said lines of said highest and lowest order of families forming a multitude of intersection points between lines belonging to one family and lines belonging to another family, and calculating for each of said intersection points of the sum of the line integral values for the two respective said lines intersecting at that point, and further adding values interpolated to said points from eventual intermediate families, said first step resulting, for each said group of families, in a plurality of points in a plane, for which pomts individual sum values are stored, said sums forming space distributions, one for each said group, b) in a successive step combining a further prime number of previously combined groups, wit their calculated space distributions, representative of adjacent positions in said order into further groups representative of a number of families which is said farther prime number times that of an immediately preceding step, having successive positions in said order, and calculating for points of intersection between those lines belonging to the families of the lowest and highest order within the number of families comprised in each combined group, of sums of values representative of the two respective space distributions, and summing thereto values for the aforesaid points of intersection taken for distributions belonging to eventual intermediate groups, either for points coinciding with those having calculated individual sums using such sums, or, for points not so coinciding, adding values interpolated from adjacent points in a respective space distribution, forming in said successive step higher order space distributions, to a number which is reduced by the factor of said further number compared to that of the starting point of said successive step, c) and repeating said second step until obtention of a final space distribution. 2. A computer tomography method of claim 1, characterized in that said interpolations are performed by linear interpolation of values belonging to points of intersection regarding a line participating in a respective intersection point, for which an interpolated value is desired. 3. A computer tomography method of claim 1, characterized in that said interpolations are performed taking into account neighbour distribution points in the plane, belonging to more than one line. 4. A computer tomography method of claim 1, characterized in that said first prime number is 2. 5. A computer tomography method of claim 4. characterized in that each said further prime number is 2. 6. A computer tomography method of claim 5, wherein each family of lines consists of lines which are mutually parallel, characterized in that the last repeated second step is performed by two combined groups, symmetrized in relation to a direction at right angles to an angle belonging to a family of lines which is at an extreme end of said enumerable order, thus obtaining a set of sum values which correspond to pixels in a cartesian system of screen pattern. 7. A computer tomograph having a plurality of detectors for sensing intensities along a multitude of lines, some of which are intersecting each other, said lines intersecting an object to be tomographed, said plurality of detectors being connected to a calculator for calculating pixel values for the intersected object, characterized in that the said calculator is provided with means for calculating partial sums according to a preceding claim.

Inventors: NILSSON STEFAN, NILSSON, STEFAN
Applicants: NILSSON STEFAN, NILSSON, STEFAN
Application year: 1997
Main classification: A61B6
IPC codes: G06T11