ENTRY M0383 20231129 M127M0383 0 1 SUBENT M0383001 20231129 M127M0383 1 1 BIB 14 53 M0383 1 2 TITLE Measurement of differential cross sections of deuteron M0383 1 3 photodisintegration in the photon energy range 250 - M0383 1 4 500 MeV. M0383 1 5 AUTHOR (V.B.Ganenko,V.A.Gushchin,Ju.V.Zhebrovskij, M0383 1 6 L.Ja.Kolesnikov,A.L.Rubashkin,P.V.Sorokin) M0383 1 7 REFERENCE (J,SNP,55,1280,1992) M0383 1 8 English translation of YF,55,(9),2311,1992. M0383 1 9 (J,YF,55,2311,1992) M0383 1 10 INSTITUTE (4UKRKFT) M0383 1 11 FACILITY (LINAC,4UKRKFT) LU-2 linear accelerator of the Kharkov M0383 1 12 Physicotechnical Institute. M0383 1 13 INC-SOURCE (BRST,KINDT) M0383 1 14 DETECTOR (MAGSP) 4-channel scintillation telescope placed in M0383 1 15 the focal plane of magnetic-spectrometer SP-02. M0383 1 16 METHOD (EXTB) M0383 1 17 PART-DET (P) M0383 1 18 SAMPLE The liquid-deuterium low-temperature target. M0383 1 19 ANALYSIS The direct registration of protons. M0383 1 20 The differential cross sections of the reaction M0383 1 21 gd -> pn were calculated using the relation (2) of M0383 1 22 the article: dSIG/dOMEGA = (A/NP)(C/J) where M0383 1 23 N is the Avogadro number, A and p are atomic weight M0383 1 24 and density of the target, C is the yield of the M0383 1 25 reaction, and J is the integral over the angular and M0383 1 26 energy acceptance of the experimental arrangement M0383 1 27 and the effective volume of the target formed by the M0383 1 28 intersection of the incident photons with the M0383 1 29 deuterium target. The integral was calculated by the M0383 1 30 Monte Carlo method. M0383 1 31 ERR-ANALYS (DATA-ERR) The mean-root-square errors are given. M0383 1 32 (ERR-SYS) The systematic ones were estimated to be M0383 1 33 about 4.4 % as determined by the following factors: M0383 1 34 the photon-beam monitoring (1.5%), the number of M0383 1 35 atoms in the deuterium target (1%), and the geometry M0383 1 36 of the experiment (the size of the beam on the M0383 1 37 target, the size of the entrance collimator of the M0383 1 38 spectrometer, the coplanarity of the reaction plane M0383 1 39 with the the horizontal plane of the spectrometer, M0383 1 40 etc.) in the calculation of the integral (4%). M0383 1 41 COMMENT The deuteron photodisintegration cross sections have M0383 1 42 been measured at c.m.s. angles of 90, 105, 120, and M0383 1 43 135 degree and in the energy range 250 - 500 MeV. The M0383 1 44 experimental data are compared with theoretical M0383 1 45 calculations which take into account the excitation M0383 1 46 of the dibarion resonances. M0383 1 47 HISTORY (19960226C) M0383 1 48 (19960313U) M0383 1 49 (20061025A) REFERENCE and DATES corrected at MSU CDFE, M0383 1 50 lowercase. M0383 1 51 (20231129A) Corrected by V. Varlamov: lowercase, M0383 1 52 TITLE, REFERENCE, INSTITUTE, FACILITY, DETECTOR, M0383 1 53 INC-SOURCE, METHOD, ANALYSIS, ERR-ANALYS, SAMPLE, M0383 1 54 REACTION, STATUS, COMMON, SUBENTS 002-005 merged. M0383 1 55 ENDBIB 53 0 M0383 1 56 COMMON 1 3 M0383 1 57 ERR-SYS M0383 1 58 PER-CENT M0383 1 59 4.4 M0383 1 60 ENDCOMMON 3 0 M0383 1 61 ENDSUBENT 60 0 M0383 199999 SUBENT M0383002 20231129 M127M0383 2 1 BIB 3 5 M0383 2 2 REACTION (1-H-2(G,N)1-H-1,,DA) M0383 2 3 STATUS (TABLE) The data from table 1 M0383 2 4 of Journ.Sov.Nucl.Phys.55,1280,1992. M0383 2 5 HISTORY (20231129A) Corrected by V. Varlamov: REACTION, M0383 2 6 STATUS, NOCOMMON, DATA substituted. M0383 2 7 ENDBIB 5 0 M0383 2 8 NOCOMMON 0 0 M0383 2 9 DATA 4 79 M0383 2 10 ANG-CM EN DATA DATA-ERR M0383 2 11 ADEG MEV MU-B/SR MU-B/SR M0383 2 12 90. 270. 5.88 .08 M0383 2 13 90. 298. 5.76 .09 M0383 2 14 90. 309. 4.83 .07 M0383 2 15 90. 318. 4.59 .08 M0383 2 16 90. 325. 4.41 .08 M0383 2 17 90. 347. 4.02 .06 M0383 2 18 90. 360. 3.19 .05 M0383 2 19 90. 370. 2.81 .05 M0383 2 20 90. 378. 2.60 .06 M0383 2 21 90. 399. 1.93 .04 M0383 2 22 90. 416. 1.49 .04 M0383 2 23 90. 428. 1.36 .03 M0383 2 24 90. 436. 1.24 .04 M0383 2 25 90. 449. 1.12 .04 M0383 2 26 90. 463. .89 .03 M0383 2 27 90. 475. .86 .03 M0383 2 28 90. 485. .87 .03 M0383 2 29 90. 499. .80 .03 M0383 2 30 90. 510. .67 .02 M0383 2 31 90. 522. .68 .03 M0383 2 32 90. 532. .71 .03 M0383 2 33 90. 540. .75 .03 M0383 2 34 90. 551. .58 .03 M0383 2 35 105. 272. 4.82 .10 M0383 2 36 105. 299. 5.51 .16 M0383 2 37 105. 310. 4.50 .12 M0383 2 38 105. 319. 4.20 .13 M0383 2 39 105. 326. 4.11 .14 M0383 2 40 105. 348. 3.22 .13 M0383 2 41 105. 361. 2.46 .11 M0383 2 42 105. 372. 1.99 .10 M0383 2 43 105. 381. 1.80 .10 M0383 2 44 105. 401. 1.72 .05 M0383 2 45 105. 419. 1.35 .04 M0383 2 46 105. 431. 1.12 .04 M0383 2 47 105. 439. 1.09 .04 M0383 2 48 105. 449. .96 .06 M0383 2 49 105. 472. .81 .06 M0383 2 50 105. 486. .77 .06 M0383 2 51 105. 495. .75 .06 M0383 2 52 120. 231. 4.42 .06 M0383 2 53 120. 272. 4.60 .07 M0383 2 54 120. 305. 4.53 .15 M0383 2 55 120. 316. 3.75 .12 M0383 2 56 120. 327. 3.44 .13 M0383 2 57 120. 336. 3.28 .13 M0383 2 58 120. 348. 2.80 .07 M0383 2 59 120. 362. 2.01 .06 M0383 2 60 120. 375. 1.74 .07 M0383 2 61 120. 384. 1.50 .07 M0383 2 62 120. 402. 1.41 .04 M0383 2 63 120. 422. 1.19 .03 M0383 2 64 120. 435. .97 .03 M0383 2 65 120. 446. .84 .02 M0383 2 66 120. 469. .69 .04 M0383 2 67 120. 484. .60 .03 M0383 2 68 120. 494. .57 .03 M0383 2 69 120. 506. .48 .03 M0383 2 70 120. 523. .51 .05 M0383 2 71 120. 536. .57 .05 M0383 2 72 135. 192. 3.78 .05 M0383 2 73 135. 232. 4.33 .06 M0383 2 74 135. 273. 4.18 .07 M0383 2 75 135. 296. 3.90 .15 M0383 2 76 135. 310. 3.51 .12 M0383 2 77 135. 322. 3.04 .13 M0383 2 78 135. 330. 2.69 .13 M0383 2 79 135. 345. 2.35 .07 M0383 2 80 135. 363. 1.77 .06 M0383 2 81 135. 375. 1.33 .07 M0383 2 82 135. 386. 1.18 .07 M0383 2 83 135. 394. 1.13 .04 M0383 2 84 135. 415. .98 .03 M0383 2 85 135. 431. .74 .03 M0383 2 86 135. 444. .68 .02 M0383 2 87 135. 472. .62 .04 M0383 2 88 135. 486. .57 .03 M0383 2 89 135. 503. .52 .03 M0383 2 90 135. 518. .56 .03 M0383 2 91 ENDDATA 81 0 M0383 2 92 ENDSUBENT 91 0 M0383 299999 NOSUBENT M0383003 20231129 M127M0383 3 1 NOSUBENT M0383004 20231129 M127M0383 4 1 NOSUBENT M0383005 20231129 M127M0383 5 1 ENDENTRY 5 0 M038399999999