DARPE: Search Results
Entry No. D1007

N.Jarmie1,R.E.Brown1,R.A.Hardekopf1
Los Alamos National Laboratory, NM1
Physical Review, Part C, Nuclear Physics29(1984)2031


FUSION-ENERGY REACTION 2H(T,ALPHA)N FROM E(T)=12.5 TO 117 KEV

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DataFilePhysical quantitiesReaction(s)Energies
1 *THTL DSIGMA/DOMEGA
DSIGMA/DOMEGA: dsigma/dOmega #1; THTL: Scattering angle theta in lab. system #4
2H(P,P)2H; 10.04 MEV
2 *INC-ENGY-LAB XSECTN INC-ENGY-LAB9) ENGY10) ENGY11) ENGY12)
ENGY: Energy; INC-ENGY-LAB: Incident energy in lab. system #3; XSECTN: Cross section #1
2H(T,ALPHA)N; between 117 and 12.5 KEV
3 *INC-ENGY-LAB XSECTN INC-ENGY-LAB9) ENGY10) ENGY11) ENGY12)
ENGY: Energy; INC-ENGY-LAB: Incident energy in lab. system #3; XSECTN: Cross section #1
2H(T,ALPHA)N; between 117 and 12.5 KEV
4 *INC-ENGY-LAB DATA6)
INC-ENGY-LAB: Incident energy in lab. system #3
2H(T,ALPHA)N; between 117 and 12.5 KEV

6) ASTROPHYSICAL S FUNCTION; FOR REACTIONS HAVING A D+T INCIDENTCHANNEL, S IS GIVEN BY S=SIGMA*E*EXP(1.08727E**(-1/2)).
9) THE NOMINAL TRITON BOMBARDING ENERGY, E(T)
10) THE TRITON ENERGY AT THE CENTER OF THE GAS TARGET.
11) THE TRITON ENERGY AS IT ENTERS THE BEAM CALORIMETER
12) THE DEUTERON BOMBARDING ENERGY THAT IS EQUIVALENT TO E(T)
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