PROCEEDINGS OF A SYMPO - IAEA Nuclear Data Services

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Evaluation of the ranges of fission products (IA E A -S M -1 7 0 /1 6 )......... 559 F. Rustichelli D iscu ssion .............................................................................................................. 573 A CCELERATO R AND SPACE SHIELDING (Section VII) Use o f nuclear data in designing sp a ce -scie n ce experim ents (IA E A -S M -170/42) .............................................................................................. 577 B .C . Clark, P. G. Kase, J.P. Martin and J. G. Morse D iscu ssion .............................................................................................................. 593 N uclear data fo r shielding and activation estim ates for TRIUMF (IA E A -S M -170/35) .......................................................................... 595 I. M. Thorson and W. J. Wiesehahn T ransport o f neutrons induced by 8 0 0 -MeV protons (IA E A -S M -17 0 /4 5) .............................................................................................. 607 R. G. Fluharty , P.A. Seeger, D. R. Harris, J.J. Koelling and O. L. Deutsch D iscu ssion .............................................................................................................. 617 Chairm en o f S ession s and S ecretariat o f the Sym posium ..................... 621
KEYNOTE ADDRESS OPENING <strong>OF</strong> THE <strong>SYMPO</strong>SIUM
Page 1: PROCEEDINGS OF A SYMPO ■ i INTERN
Page 6 and 7: The follow in g States are M em ber
Page 8 and 9: N U C L E A R D A T A IN S C IE N C
Page 10 and 11: A cce le ra to r and Space Shieldin
Page 12 and 13: C r o s s -s e ctio n uncertainty e
Page 17 and 18: CRITERIA OF CHOICE FOR COMPILATIONS
Page 19 and 20: SYMPOSIUM KEYNOTE 5 INTERNAL CRITER
Page 21 and 22: SYMPOSIUM KEYNOTE 7 are them selves
Page 23 and 24: SYMPOSIUM KEYNOTE 9 new techniques
Page 25: SYMPOSIUM KEYNOTE 1 1 [ 4 ] I n te
Page 28 and 29: C hairm an KOLSTAD (USA)
Page 30 and 31: 16 THOM and SCHNEIDER A frequently
Page 32 and 33: 18 TH OM and SCHNEIDER Three requir
Page 34 and 35: 2 0 TH OM and SCHNEIDER POTENTIAL A
Page 36 and 37: 2 2 THOM and SCHNEIDER 4 -ST flG E
Page 38 and 39: 24 THOM and SCHNEIDER the short wav
Page 40 and 41: 26 THOM and SCHNEIDER Three critica
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Page 44 and 45: 30 THOM and SCHNEIDER Small Light B
Page 46 and 47: 32 THOM and SCHNEIDER accuracy is a
Page 48 and 49: 34 THOM and SCHNEIDER The radial di
Page 50 and 51: 36 THOM and SCHNEIDER [4] RAGSDALE,
Page 52 and 53: 38 THOM and SCHNEIDER energy losses
Page 54 and 55: 40 WOLKENHAUER and LEONARD 1. Histo
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Page 58 and 59: 44 WOLKENHAUER and LEONARD • POWE
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50 WOLKENHAUER and LEONARD [13] SKE
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52 STUBBINS and WOLFE and f u n c t
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5 4 STUBBINS and WOLFE T A B L E I.
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56 STÜBBINS and WOLFE T A B L E II
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( TABLE III. 3-GROUP CROSS-SECTIONA
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TABLE IV. CRITICALITY REQUIREMENTS
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62 STUBBINS and WOLFE A. E f f e c
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64 STUBBINS and WOLFE T A B L E V .
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6 6 STUBBINS and WOLFE average time
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6 8 STUBBINS and WOLFE The economic
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I A E A - S M -1 7 0 /5 8 A STUDY O
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I A E A - S M -1 7 0 /5 8 73 T A B
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I A E A - S M -17 0 /5 8 75 T A B L
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I A E A - S M -1 7 0 /5 8 T A B L E
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I A E A - S M -1 7 0 /5 8 79 T A B
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I A E A - S M -1 7 0 /5 8 81 T A B
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10 г- T3 - i ï 10 S _l -г < 10 1
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О) I - o I A E A - S M -1 7 0 /5 8
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I A E A - S M -1 7 0 /5 8 8 7 The r
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SECTIONS EFFICACES DE CREATION DE D
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1 .1. Choc élastique I A E A -S M
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IAE A - S M - 1 7 0 /6 5 93 L'éner
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Section efficace de dommage Energie
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CONCLUSION IAE A - S M - 17 0 /6 5
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I A E A - S M -1 7 0 /6 5 107 TABLE
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IA E A -SM -1 7 0 /6 5 109 TABLEAU
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I A E A - S M -1 7 0 /6 5 111 TABLE
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I A E A - S M -1 7 0 /6 5 И З TAB
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IA E A -S M -n o/6 5 115 TABLEAU V
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I A E A - S M -1 7 0 /6 5 117 TABLE
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IA E A -S M -1 70/65 119 TABLEAU V
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I A E A - S M -1 7 0 /6 5 121 TABLE
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IAE A -SM -1 7 0 /6 5 123 TABLEAU I
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IAE A - S M - 1 7 0 /6 5 125 REFERE
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Section II REACTOR TECHNOLOGY
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IAEA- SM-170/91 ТОЧНОСТЬ Я
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IAEA SM-170/91 131 3) Для без
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IAEA SM -170/91 133 важност
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IAEA SM -170/ 91 135 ваемых
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ТАБЛИЦА II . (продолж
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П римечания к табли
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IAEA-S M -170/91 141 ZPR-III-48 и
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I A E A - S M -1 7 0 /6 9 ROLES RES
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I A E A - S M - 1 7 0 /69 145 L a q
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I A E A -S M - 1 7 0 /6 9 147 de la
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I A E A - S M -1 7 0 /6 9 149 FIG.
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I A E A -S M - 1 7 0 /6 9 T A B L E
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3 .5 . A u tr e s d em an d es I A
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CROSS-SECTION UNCERTAINTY EFFECTS O
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I A E A 'S M - 1 7 0 /7 T h e c o d
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1Л n» О О О 'í 16.375 REG. A
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I A E A -S M - 1 7 0 /7 161 T A B L
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EL USO DE PARAMETROS NEUTRONICOS DE
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IAE A - S M - 1 7 0 /2 165 En un r
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I A E A - S M -1 7 0 /2 1 6 7 E STI
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I A E A - S M -1 7 0 /2 169 T A B L
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I A E A - S M -1 7 0 /2 1 7 1 A d e
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I A E A - S M -1 7 0 /2 173 P a r t
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I A E A - S M -1 7 0 /1 8 ASSESSMEN
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I A E A -S M -1 7 0 /1 8 177 routin
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I A E A - S M -1 7 0 /1 8 179 TABLE
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I A E A - S M -1 7 0 /1 8 181 and
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I A E A - S M -1 7 0 /1 8 183 WIMS
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IAEA-SM-170/18 185 For the discrepa
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I A E A - S M -1 7 0 /1 8 187 exper
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IAEA -S M -1 7 0 /6 7 UTILISATION D
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1. 5. Nouvel intérêt des m esures
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IA E A -SM -17 0 / 67 193 P ar aill
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Section III SAFEGUARDS
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THE ROLE OF NUCLEAR DATA IN NUCLEAR
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IA E A -S M -1 70/7 8 199 I n s t e
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IA E A -S M -1 70/78 201 s t a t e
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IA E A -S M -1 70/78 203 s p e c t
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TABLE V . DECAY ENERGY Q, H A L F-L
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IA E A -S M -170/78 207 e . g . , o
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IA E A -S M -1 70/7 8 209 TA B L E
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IA E A -S M -1 70/7 8 211 T a b l e
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IAEA-SM “ 17 0 /7 8 213 (1) E v e
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IA E A -S M -1 70/78 l_ 36 / G O Z
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IA E A -SM -П О /5 4 THE ROLE OF
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IAEA-SM-170/54 The assay of a fuel
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IA E A -S M -1 7 0 /5 4 221 FIG. 3.
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IA E A -S M -17 0 /5 4 223 FIG. 6.
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LAEA-SM-17 0/5 4 225 w hich time th
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IAEA-SM-170/54 227 energies b elow
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IAEA-SM-17 0/54 229 coincidence rat
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IAEA-SM-17 0/54 231 [8] MENLOVE, H.
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234 EDER and LAM M ER In a "forward
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236 EDER and LAM M ER decay during
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238 EDER and LAM M ER The ra tio o
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240 EDER and LAM M ER Step 3: The n
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242 EDER and LAM M ER FIG . 2 100 1
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244 EDER and LAM M ER gamma ray mea
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246 EDER and LAM M ER T A B L E I.
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248 EDER and LAMMER TA B L E III. F
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250 EDER and LAM M ER T A B L E III
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252 EDER and LAMMER О . О 2 5 З
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254 EDER and LAMMER T A B L E V . E
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256 EDER and LAMMER T A B L E V (co
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258 EDER and LAMMER T A B L E V I.
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260 EDER and LAMMER I n a f o r w a
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262 EDER and LAMMER 5 . 1 . 3 . D e
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264 EDER and LAMMER 5.3. Examples o
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266 EDER and LAMMER REFERENCES r d
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268 EDER and LAMMER c a r r i e d o
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270 BERENYI claims for radioactive
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T A B L E I. H A L F -L IF E O F R
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T A B L E II. Y IELD O F G A M M A
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T A B L E lib . CONTIN U ATIO N Rad
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T A B L E lid . CO N TIN U ATIO N R
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280 BERÉNYI future: it would be ve
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282 BERÉNYI [29] ARDISON, G. et MA
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Section IV LIFE SCIENCES
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LE ROLE DES DONNEES NUCLEAIRES DANS
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IA E A -S M -1 70/97 289 FIG. 1. S
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C IB L E Hg PARTICU LES iA E A -S M
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IA E A -S M -1 7 0/9 7 293 ou syst
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IAEA -SM -1 7 0 /9 7 295 Le princip
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IA E A -S M -1 70/97 nous examinero
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IA E A -S M -1 70/97 299 T A B L E
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IA E A -S M -1 70/9 7 301 capture
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lA E A -S M -1 7 0 /9 7 303 T A B L
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IA E A -S M -17 0 /9 7 305 FIG. 10.
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c o m p o s itio n du co r p s h u
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IA E A -S M -17 0 /9 7 309 (3) BÈR
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IA E A -S M -1 7 0/9 7 311 D I S C
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314 DENNIS However, these aspects a
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316 DENNIS D O S E ( K r a d s ) FI
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318 DENNIS F IG .6. An illustration
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TABLE I. SUMMARY OF I. C. R . P. RE
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322 DENNIS F IG .9. Specific energy
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324 DENNIS Similar details are requ
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326 DENNIS C l J LAURIE, J., ORR, J
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IAEA -SM-170/64 PROBLEMES POSES PAR
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IAEA-SM-170/64 331 liè r e s , dan
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IAEA-SM- П О /64 333 Le rendem en
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NUCLEAR DATA AND NEUTRON ACTIVATION
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IAEA-SM-170/3 T A B L E lia . A C T
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IAEA-SM-170/3 339 At th is stage mo
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T A B L E V b . IS O T O P IC SEN S
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IAEA-SM-ИО/З 343 TABLE VI. ELEM
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IAEA-SM-ПО/З 345 The follow ing
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IAEA-SM- ПО/З 347 TABLE IX . DET
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IAEA-SM-170/3 349 [10] SEELMANN-EGG
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352 COHEN L es radioélém en ts de
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354 COHEN TABLEAU II. CONSTANTES NU
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356 COHEN On peut pen ser que les t
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I A£ A-SM-170/92 APPLICATION OF NU
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IAE A-SM-170/92 361 The p roblem s
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4. 20N e(p ,tf)18F 5. 160 (a , 2n)1
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T A B L E I. (continu ed) 13. Oak R
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T A B L E II. SP E C IF IC A T IO N
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IAEA-SM-170/92 369 Neutrons produce
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8.3. A c c e le r a t o r p ro d u
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IAEA-SM-170/92 373 R.В.R. PERSSON:
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Chairman K.H. LIESER (Federal Repub
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378 GÓRSKI Unfortunately, the labe
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380 GÓRSKI several billions of yea
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NUCLEAR DATA REQUIRED FOR THE INTER
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IAEA-SM -170/28 385 dissipated by t
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100 10 IAEA-SM -17 0/28 387 1 5 10
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IAE A -S M -17 0/28 389 m ay not be
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Chairman G. В. YANKOV (USSR)
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394 CROUCH it was thought proper to
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396 CROUCH its uncertainty; the cha
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398 CROUCH It should also be mentio
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400 CROUCH Table I I Ac Pile Neutro
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402 CROUCH Table III (cont) Th then
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404 CROUCH Table IV Pa Pile neutron
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406 CROUCH Table V I 'Th Pile neutr
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408 CROUCH Table V (cont) 'Th Pile
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410 CROUCH 77 Ge As 347 347 Table V
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412 CROUCH Table VII (cont) 233 U T
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414 CROUCH Table VII (cont) U Therm
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420 CROUCH Table VIII (cont) U Ther
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422 CROUCH Table VIII (cont) U Ther
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424 CROUCH Table VIII (cont) 235 U
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426 CROUCH 1 2 Table VIII (cont) 23
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428 CROUCH T a b l e V I I I ( c o
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1 83 89 91 97 99 103 105 106 109 11
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432 CROUCH Table X 239 Pu Thennal n
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434 CROUCH Table X (cont) 239 Pu Th
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436 CROUCH T a b le X ( c o n t ) P
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438 C R O U C H T a b le X ( c o n
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440 C R O U C H Table XI Pu Thermal
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442 CROUCH T a b l e X I ( c o n t
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4 4 4 CRO U CH T a b l e X I ( c o
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1 83 84 89 90 91 92 93 95 97 99 103
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1 89 95 97 99 103 106 109 111 112 1
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450 C R O U C H T a b l e XVI ( c o
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452 c r o u c h Table XVI (cont) Re
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454 CROUCH T a b l e X V I ( c o n
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456 C R O U C H T a b l e X V I ( c
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458 C R O U C H m y m e m o r y goe
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460 W ALKER o b t a i n y i e l d s
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462 W ALKER a v e r a g e i s o n l
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464 W ALKER TABLE II. RELATIV E ELE
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Fission Product А Л a ± Да - b
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468 W ALKER p e r i o d . T h e t h
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470 W ALKER T A B L E IV. M A J O R
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472 W ALKER d e t e c t o r t o s o
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474 W ALKER T A B L E V . N U C L I
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476 W ALKER [1 1 ] H a w k i n g s
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478 DEVILLERS e t a l. sont sn effe
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480 DEVILLERS e t a l. . 2 3 8 U' :
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482 DEVILLERS e t a l. Les modes de
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DEVILLERS e t a l. Une table de pro
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suivantes : DEVILLERS e t a l. Les
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488 DEVILLERS e t a l. G ESTION P E
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T A B L E A U III. E N E R G I E L
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492 DEVILLERS e t a l. F I G .3 . D
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494 DEVILLERS e t a l. T A B L E A
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4 9 6 DEVILLERS e t a l. F i l e 1
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4 9 8 DEVILLERS e t a l. F i l e 1
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500 DEVILLERS et al. F i l e 1 MT =
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502 DEVILLERS et al. (2) (3 ) (4 )
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DISCUSSION OF FISSION-PRODUCT YIELD
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IAEA-SM-170/13 507 In their evaluat
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T A B L E I (continu ed) IAEA-SM-17
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IAEA-SM-170/13 511 also measured, t
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IAEA-SM-170/13 513 contribute to th
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LAEA-SM-170/13 515 The accuracy of
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IAEA-SM-170/13 517 The samples used
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LAEA-SM-170/13 519 An example o f t
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IAEA-SM-170/13 521 In the discussio
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IAEA-SM-170/13 523 data have been c
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T A B L E II (con tin u ed) fissio
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IAEA-SM-170/13 527 Apart from the f
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IAEA-SM-170/13 529 mass peak only w
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T A B L E IV (continu ed) Mass No.
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T A B L E IV (continued) Mass No. 1
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T A B L E V (continued) Mass Ko. Th
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T A B L E V (continued) Mass No. Th
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T A B L E VI (continued) Mass No. t
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T A B L E VI (continu ed) Mass No.
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IAEA-SM-170/13 543 and Scadden [9 2
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T A B L E VII (continued) Mass No.
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IAEA-SM-170/13 547 in a forthcoming
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IAEA-SM-170/13 549 [48] WAHL, A. C
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IAEA-SM-170/13 551 D I S C U S S I
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554 GRUPPELAAR 2. PRESENT SITUATION
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556 GRUPPELAAR FIG. 1. Calculated c
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558 GRUPPELAAR R E F E R E N C E S
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560 RUSTICHELLI H ow ever, by using
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562 RUSTICHELLI The en ergies of th
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T A B L E I. A B SO L U T E RANGES
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T A B L E II (continu ed) Phosphoru
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T A B L E II (continu ed) Ces i urn
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TABLE II (continued) Americî um Am
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572 RUSTICH ELLI The ra tio in air
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Section VII ACCELERATOR AND SPACE S
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I A E A - S M -17 0 /4 2 USE OF NUC
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I A E A - S M -17 0 /4 2 579 a n d
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I A E A - S M -17 0 /4 2 581 is onl
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I A E A - S M -17 0 /4 2 583 m a g
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IA E A -S M - П 0 /4 2 585 to assa
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I A E A - S M -17 0 /4 2 587 dead l
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I A E A - S M -1 7 0 /4 2 589 phosp
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I A E A - S M -17 0 /4 2 591 T A B
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I A E A - S M -17 0 /4 2 593 [22] V
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I A E A - S M -17 0 /3 5 NUCLEAR DA
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I A E A - S M -1 7 0 /3 5 597 t r o
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I A E A - S M - n O /3 5 599 o u t
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I A E A - S M -17 0 /3 5 601 r e a
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I A E A - S M -17 0 /3 5 603 F IG .
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I A E A - S M - n O /3 5 605 s y s
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TRANSPORT OF NEUTRONS INDUCED BY 8
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MAIN BEAM UNE IAEA-SM-17 0 /4 5 609
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I A E A - S M -17 0 /4 5 611 F I G
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(a) A cy lin d rica l geometry was
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I A E A - S M -17 0 /4 5 F IG . 7 .
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I A E A - S M -17 0 /4 5 REFERENCES
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I A E A - S M -17 0 /4 5 619 is o f
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H O W T O O RD ER IAEA PUBLICATIONS
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