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Muon Decay
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The decay of the muon has been studied at PSI with several precision
measurements: The longitudinal polarization
P_{\mathrm{L}}(E)
P
L
(
E
)
with the muon decay parameters
\xi'
ξ
′
,
\xi''
ξ
″
,
the Time-Reversal Invariance (TRI) conserving transverse polarization
P_{\mathrm{T_{1}}}(E)
P
T
1
(
E
)
with the muon decay parameters
\eta
η
,
\eta''
η
″
,
the TRI violating transverse polarization
P_{\mathrm{T_{2}}}(E)
P
T
2
(
E
)
,
with
\alpha'/A
α
′
/
A
,
\beta'/A
β
′
/
A
and the muon decay asymmetry with
P_{\mu}\xi
P
μ
ξ
.
The detailed theoretical analysis of all measurements of normal and
inverse muon decay has led for the first time to a lower limit
|g^{V}_{LL}| > 0.960
|
g
L
L
V
|
>
0.960
(“
V-A
V
−
A
”)
and upper limits for nine other possible complex couplings, especially
the scalar coupling
|g^{S}_{LL}| < 0.550
|
g
L
L
S
|
<
0.550
which had not been excluded before.
Title: Muon Decay
Description:
The decay of the muon has been studied at PSI with several precision
measurements: The longitudinal polarization
P_{\mathrm{L}}(E)
P
L
(
E
)
with the muon decay parameters
\xi'
ξ
′
,
\xi''
ξ
″
,
the Time-Reversal Invariance (TRI) conserving transverse polarization
P_{\mathrm{T_{1}}}(E)
P
T
1
(
E
)
with the muon decay parameters
\eta
η
,
\eta''
η
″
,
the TRI violating transverse polarization
P_{\mathrm{T_{2}}}(E)
P
T
2
(
E
)
,
with
\alpha'/A
α
′
/
A
,
\beta'/A
β
′
/
A
and the muon decay asymmetry with
P_{\mu}\xi
P
μ
ξ
.
The detailed theoretical analysis of all measurements of normal and
inverse muon decay has led for the first time to a lower limit
|g^{V}_{LL}| > 0.
960
|
g
L
L
V
|
>
0.
960
(“
V-A
V
−
A
”)
and upper limits for nine other possible complex couplings, especially
the scalar coupling
|g^{S}_{LL}| < 0.
550
|
g
L
L
S
|
<
0.
550
which had not been excluded before.
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