ENTRY             K+70          0                                   K+70 0    1
SUBENT         K+70  1          0                                   K+70 1    1
BIB                 13         27                                   K+70 1    2
INSTITUTE  (CCP) INSTITUTE NOT SPECIFIED IN THE ORIGINAL PAPER.     K+70 1    3
REFERENCE  (J,JET/L,12,3,149,1970)                                  K+70 1    4
AUTHORS    (K.V.KARADZHEV,V.I.MAN'KO,A.N.NERSESYAN,F.E.CHUKREEV)    K+70 1    5
TITLE      INVESTIGATION OF A POSSIBLE VIOLATION OF THE             K+70 1    6
           INDEPENDENCE OF THE DECAY OF A COMPOUND NUCLEUS          K+70 1    7
           OF THE SPIN OF THE INPUT CHANNEL                         K+70 1    8
FACILITY   FACILITY NOT SPECIFIED IN THE ORIGINAL PAPER.            K+70 1    9
INC-PART   (P) PROTONS.                                             K+70 1   10
TARGET     THIN LAYER OF P3ZN2 SPUTTERED ON TANTALUM SUBSTRATE.     K+70 1   11
METHOD     MEASURED EXCITATION FUNCTION FOR 31P(P,GAMMA)32          K+70 1   12
           REACTION IN THE VICINITY OF THE EP = 2114 KEV            K+70 1   13
           RESONANCE. USED A NAI SCINTILLATION DETECTOR TO          K+70 1   14
           MEASURE GAMMA RAYS SINCE CROSS SECTION WAS TOO LOW       K+70 1   15
           TO USE A GERMANIUM DETECTOR. IT WAS NECESSARY TO         K+70 1   16
           PLACE THIS DETECTOR VERY CLOSE TO THE TARGET IN POOR     K+70 1   17
           GEOMETRY. TOTAL ANGULAR DISTRIBUTION NOT MEASURED.       K+70 1   18
           ONLY THE RATIO OF GAMMA-RAY YIELD AT 0 AND 90            K+70 1   19
           DEGREES WAS DETERMINED. NO OTHER DETAILS ARE GIVEN       K+70 1   20
           IN THE ORIGINAL PAPER.                                   K+70 1   21
DETECTOR   (SCINT) 9-CM DIA, X 10-CM LONG NAI SCINTILLATION         K+70 1   22
           DETECTOR.                                                K+70 1   23
MONITOR    MONITOR NOT SPECIFIED IN THE ORIGINAL PAPER.             K+70 1   24
CORRECTION CORRECTIONS FOR GEOMETRIC EFFECTS WERE APPLIED.          K+70 1   25
ERR-ANALYS ERROR IN RESULT IS GIVEN. ERROR ANALYSIS METHOD          K+70 1   26
           NOT DISCUSSED IN THE ORIGINAL PAPER.                     K+70 1   27
COMMENT    THIS IS A VERY BRIEF COMMUNICATION THAT PROVIDES FEW     K+70 1   28
           DETAILS CONCERNING THE WORK.                             K+70 1   29
ENDBIB              27                                              K+70 1   30
ENDSUBENT            1                                              K+70 199999
SUBENT         K+70  2          0                                   K+70 2    1
BIB                  2          8                                   K+70 2    2
REACTION   31P(P,GAMMA)32S                                          K+70 2    3
COMMENTS   RATIO OF GAMMA-RAY YIELD AT 0 AND 90 DEGREES RELATIVE    K+70 2    4
           TO INCIDENT PROTON BEAM WAS MEASURED WITH A NAI          K+70 2    5
           SCINTILLATION DETECTOR PLACED CLOSE TO THE TARGET IN     K+70 2    6
           POOR GEOMETRY. DATA OBTAINED FROM TEXT OF ORIGINAL       K+70 2    7
           PAPER. EP = INCIDENT PROTON ENERGY. RATIO = RATIO        K+70 2    8
           OF GAMMA-RAY YIELD AT 90 DEGREES TO THAT OBTAINED        K+70 2    9
           AT 0 DEGREE. RATIO-ERR = ERROR IN RATIO.                 K+70 2   10
ENDBIB               8                                              K+70 2   11
DATA                 3          1                                   K+70 2   12
EP         RATIO      RATIO-ERR                                     K+70 2   13
KEV        NO-DIM     NO-DIM                                        K+70 2   14
 2114.      5.54       0.5                                          K+70 2   15
ENDDATA              3                                              K+70 2   16
ENDSUBENT            2                                              K+70 299999
ENDENTRY             2                                              K+709999999