- Source: Michel parameters
The Michel parameters, usually denoted by
ρ
,
η
,
ξ
{\displaystyle \rho ,\eta ,\xi }
and
δ
{\displaystyle \delta }
, are four parameters used in describing the phase space distribution of leptonic decays of charged leptons,
l
i
−
→
l
j
−
ν
i
ν
j
¯
{\displaystyle l_{i}^{-}\rightarrow l_{j}^{-}\nu _{i}{\bar {\nu _{j}}}}
. They are named after the physicist Louis Michel. Sometimes instead of
δ
{\displaystyle \delta }
, the product
ξ
δ
{\displaystyle \xi \delta }
is quoted. Within the Standard Model of electroweak interactions, these parameters are expected to be
ρ
=
3
4
,
η
=
0
,
ξ
=
1
,
ξ
δ
=
3
4
.
{\displaystyle \rho ={3 \over 4},\quad \eta =0,\quad \xi =1,\quad \xi \delta ={3 \over 4}.}
Precise measurements of energy and angular distributions of the daughter leptons in decays of polarized muons and tau leptons are so far in good agreement with these predictions of the Standard Model.
Muon decay
Consider the decay of the positive muon:
μ
+
→
e
+
+
ν
e
+
ν
¯
μ
.
{\displaystyle \mu ^{+}\to e^{+}+\nu _{e}+{\bar {\nu }}_{\mu }.}
In the muon rest frame, energy and angular distributions of the positrons emitted in the decay of a polarised muon expressed in terms of Michel parameters are the following, neglecting electron and neutrino masses and the radiative corrections:
d
2
Γ
x
2
d
x
d
cos
θ
∼
(
3
−
3
x
)
+
2
3
ρ
(
4
x
−
3
)
+
P
μ
ξ
cos
θ
[
(
1
−
x
)
+
2
3
δ
(
4
x
−
3
)
]
,
{\displaystyle {\frac {d^{2}\Gamma }{x^{2}dxd\cos \theta }}\sim (3-3x)+{\frac {2}{3}}\rho (4x-3)+P_{\mu }\xi \cos \theta [(1-x)+{\frac {2}{3}}\delta (4x-3)],}
where
P
μ
{\displaystyle P_{\mu }}
is muon polarisation,
x
=
E
e
/
E
e
m
a
x
{\displaystyle x=E_{e}/E_{e}^{max}}
, and
θ
{\displaystyle \theta }
is the angle between muon spin direction and positron momentum direction. For the decay of the negative muon, the sign of the term containing
cos
θ
{\displaystyle \cos \theta }
should be inverted.
For the decay of the positive muon, the expected decay distribution for the Standard Model values of Michel parameters is
d
2
Γ
d
x
d
cos
θ
∼
x
2
[
(
3
−
2
x
)
−
P
μ
cos
θ
(
1
−
2
x
)
]
.
{\displaystyle {\frac {d^{2}\Gamma }{dxd\cos \theta }}\sim x^{2}[(3-2x)-P_{\mu }\cos \theta (1-2x)].}
Integration of this expression over electron energy gives the angular distribution of the daughter positrons:
d
Γ
d
cos
θ
∼
1
+
1
3
P
μ
cos
θ
.
{\displaystyle {\frac {d\Gamma }{d\cos \theta }}\sim 1+{\frac {1}{3}}P_{\mu }\cos \theta .}
The positron energy distribution integrated over the polar angle is
d
Γ
d
x
∼
(
3
x
2
−
2
x
3
)
.
{\displaystyle {\frac {d\Gamma }{dx}}\sim (3x^{2}-2x^{3}).}
References
Lecture on Lepton Universality by Michel Davier at the 1997 SLAC Summer Institute.
Electroweak Couplings, Lepton Universality, and the Origin of Mass: An Experimental Perspective, article by John Swain, from the Proceedings of the Third Latin American Symposium on High Energy Physics.
Kata Kunci Pencarian:
- Mont Saint-Michel
- Smarck Michel
- Michel Aoun
- Michel Marcel Navratil
- Hartmut Michel
- Michel Rocard
- Michel Preud'homme
- Michel Suleiman
- Michel Aflaq
- Pascastrukturalisme
- Michel parameters
- Michel
- Muon
- Louis Michel (physicist)
- Michel Foucault
- Michel Aflaq
- Michel de Montaigne
- Sony Michel
- Michael Bublé
- Emmanuel Macron
