JAICkl Conf SM cm 10cm 0 CJgJf L/D 1100A» ^35 fc ^ L to? C fct2.6], N R C (rotation-rotation^st) fffi ft tio.05" 2-2 N Slftff fc L, Pig

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1 JAKK1 Conf { j 土 札 合 J 去 市 ;1 ;IJJ υ}~ 刊!JC 6. fttm /7^J jt>/: 1 fi 1 y I f l /:' 'fl;r-7^t777 - K/7 7 i - CNRCT) C ttl* * C Tflt A 1 (0. 093cm"') A (2. 5cr ) * T O lotto. NRCTCR 1. & EfcH CC-CCD) if 7 7 A (N R) C 4ft: PCD(Plasma Coupled Devi ce) U - T -f ^ - v -t > t Tffl l> k N R C T ft X ^ 5 [7], T (NRCT) 8-2: )» , N R C T (0. l~l000 cm" 1 ) lillfflxct (0.1-lOcii- 1 ) NRCTT-li > <k 42-

2 JAICkl Conf SM cm 10cm 0 CJgJf L/D 1100A» ^35 fc ^ L to? C fct2.6], N R C (rotation-rotation^st) fffi ft tio.05" 2-2 N Slftff fc L, Pig.. 1cm" 1 A»<b2. 5c m 0: Base plale (Al) 1: Aluminium 2: Graphite (C) 3: Lead 4: Titanium 5: Copper (r. Iron 7. SUS..H4 <S: Acrvlic resin l )HD: Dry wood (high density) yi.d: Dry wood (low density) 10: ABS resin 11: Ciidmium +. Center of rotation I cm Fig.1 A sectional view of the object designed to test the linearity of the CT value of various materials. 43

3 JAICKI Ccuif 94 (KG (J()~ Inn, Life. ~ 2-3 ^ 6 L i F + ZnS (Ag) C C, CCD» 1 のミ? 2-4 C-CCD» *>^> 8 t, NR 510X492> fc., (3) ^ C4) fc, 2-5 IB 150μm~-こ 相 当 する 捕 捜 y 線 発 生 源 となる 第 1 44

4 JAKKI Q>nf 9~ fc U, 320 v- K f -f 180* 3. NRCT S64MB, * - # C J; 0 r ft -o &S *tie ^7LfcK:!&iBffea'fcfl!)iM y ^?A Csinogram), JS» 3, CTtt,, If- A^- K- >^*!lft*<n R r>ttfc -45

5 JAHRI J^EI~I Conf (a) Cb) Pig. 2 Tomograms reconstructed from (a) the 90 projection images at the slice number 230 and from (b) the 180 projection images at the slice number

6 JAKKI (\mf J 八 EI~I ~ (1) 7-'J*Sftffi, (2) (3) S> (2) tf C3) c*s»t if, -3fc u fcfc*, : Toshiba DSTP-9506)??tS/ l Sheppfc Logan 7 j* C3) Cfcrjfe^ x *J * Fig. 2 (a) fccfctf (b) ig. 2 Cb) ti <, 7-f- -< (artifact) '> > Fig.2 (a) &*>\ Fig.2 Cb) K*j^"C» ; y -j-a "?r>? h^ a»css«> > y v She P ptlogan7 r V 5. NRC N LTtt ttfc CHounsfield unit: SfcEHI number^ffi ^^^?*^ & AK Sitf u C ob j F B C T = 935X +93. CF«~ Co i C 1 ) -47 -

7 JAKRI Omf 9-1 9~ o Slice No2M Slice No.I2H Dry wood Acrylic resin 00 LU < 2000 u Q UJ IS) UJ Ph ±(l.05l (I.77II-H.IISV cm Wood w, 側 ~ (high density) Wood (low ~"n density), ily EFFECTIVE MACROSCOI'C CROSS SECTION, cm" 1 Fig.3 Reconstructed CT values vs. total macroscopic cross sections for various materials. Fig. 3-4 >->' Tef f Toax Train It,, 2500(2. 5cm- T= H2t)dt=ln[Io/I] = J [CTfifGdt: i C2), T C.3J S!fflftfrT..xt*» I tr ADC If* *>*v SI: L-T, ln(io).

8 JAMK1 c:<>nf!j~ flgfc&s. s l o /«5 I =exp(teff) C4) 10~:1, 12tT T.a«= 8. 3 t r K fft Table 1 Effective cross sections and lhickne~s maximum thickne&s of materials *«* <2> (cm" 1 ) tmax (Cm) Al Zn Pb Ti Cu Pe Ag Au I n Cd T7P> * >? i; A t ij X. 4- U y fc. t, D = 2 26

9 .I JAKKI '\I':I~I Conf 9~ ()(J~ tmax= 1' eff/<~> (5) Table 1 K /f< L fc 3-5 fitt, 0., L/D = 5cm 0 すなわち~ ' ^ -t 4. iglft «L/D 1024X ifflt 価 されており その 結 果 C 1'による 分 解 能 は Klasense の 式 口 3J を 用 いて ~o. れた これは CCD 素 子 上 で ~4.5 ピクセルに 相 当 する なお JRR-3Mの 熱 中 性 子 ラジオ グラフィ 施 設 は L/D=150~176 を 有 しており 5cm ゅの 被 写 体 で 最 大 の 幾 何 学 的 不 鮮 明 えば JRR3 の ~108n/cm2/s の 高 中 性 子 束 密 度 高 L/D [1] H. Kobayashi, et a 1..'"Neutron radiography using cooled CCD camera". NR-3 (1990) p [2] H. Kobayashi: "Studies of neutron transmittance measurements using cooled CCD camera". Proc. 1st Int. Topical Meeting on Neutron Radiography System Design and Characterization.(Pembroke.1990), Paper No.14. (to be publised). [3] E. McFarland, et al., "Multi-dimentional neutron-computed tomography using cooled CCD", IEEE Trans. Nuci. Sci., NS-38, (Apr.) 612 (1991). [1] I. Na, E. MacFarland and R. Lanza. "Quantitative evaluation of a neutron radiography and tomography system using cooled charge coupled devices designed for low fluence sources", NR-4(1992) Abst.p.90, (to be published). [5] H. Na, E. ~ MacFarland and R. Lanza, "A segmented array approach to large scale neutron radiography and tomography systems using cooled charge coupled devices" NR-4 (1992) Abst. p.108 (to be published). [6] H. Koabyashi: "Recent development of cooled CCD camera for NR imaging - Tomography", NR-4 (1992) Abst. p. 103 (to be published) cc

10 JAKKI Conf 94 9~ 002 [7]. Apr. 4-6,1989) E44. [8] D. ~ M. Tow, "Postirradiation examination using neutron tomography", NR-1 (1982) p [9] G.Matsumoto & S.Krata. "The neutron computer tomography", NR-1(1982) p.899. [10] Y. Murata et al.: "Two-dimensional neutron image excluding the effect of scattered neutron", NR-4 (1992) Abst. p.96 (to be published). [11] H. Kobayashi et al. : "Macroscopic cross section measurements and defect detection in materials using neutron radiography technique", J. Nucl. Sci. Technol. 29. (11), 1045 (1992). [12] L. A. Shepp and B. F. Logan: "The Fourier reconstruction of a head section" IEEE Trans. Nucl. Sci.. NS-21. (June). 21 (1974). [13] H. A. Klasens: "Measurement and calculation of unsharpness combination in X-ray photography", Philips Res. Rep., 1. 4 (Aug. 1946). NR-1: "Neutron Radiography", eds. J. P. Barton and P. v.d. Hardt, (D. Reidel Publ., Dordrecht. 1982), Proceedings of the 1st World Conference on Neutron Radiography, (San Diego. Dec ). NR-2: "Neutron Radiography", eds. J. P. Barton et al., (D. Reidel Publ., Dordrecht. 1987). Proceedings of the 2nd World Conference on Neutron Radiography, (Paris, June 16-20, 1986). NR-3: "Neutron Radiography (3)", eds. S. Fujine et al., (Kluwer Publ. Dordrecht, 1990), Proceedings of the 3rd World Conference on Neutron Radiography, (Osaka. May ). NR-4: "Neutron Radiography (4)". (in press). Proceedings of the 4th World Conference on Neutron Radiography, (San Fransisco, May 10-16, 1992). 51 -

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