Comparison of the TDCR method and the CIEMAT/NIST method for ...
Comparison of the TDCR method and the CIEMAT/NIST method for ...
Comparison of the TDCR method and the CIEMAT/NIST method for ...
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ε<br />
electron spectrum S(E)<br />
1 PMT:<br />
2 PMTs:<br />
3 PMTs:<br />
ε<br />
ε<br />
ε<br />
1<br />
2<br />
=<br />
=<br />
E<br />
max<br />
E<br />
Free parameter model<br />
= −<br />
∫<br />
0<br />
max<br />
∫<br />
0<br />
E<br />
max<br />
T ∫<br />
0<br />
−EQ(<br />
E)/ M<br />
SE ( )(1 e ) dE<br />
S(<br />
E)(<br />
1−<br />
e<br />
S(<br />
E)(<br />
1−<br />
−EQ(<br />
E)<br />
/ 2M<br />
logical sum <strong>of</strong> double coincidences in a system with 3 PMTs:<br />
O. Nähle <strong>and</strong> K. Kossert <strong>Comparison</strong> <strong>of</strong> <strong>TDCR</strong> <strong>and</strong> CN <strong>for</strong> β emitters<br />
e<br />
−EQ(<br />
E)<br />
/ 3<br />
M<br />
)<br />
)<br />
2<br />
3<br />
dE<br />
dE<br />
D =<br />
Emax<br />
∫<br />
0<br />
−EQ( E)/3M2 −EQ(<br />
E)/3M3 SE ( )(3(1 −e) −2(1 −e)<br />
) dE