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Improved π0, η, η′ transition form factors in resonance chiral theory and their $$ {a}_{\mu}^{\textrm{HLbL}} $$ contribution
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Abstract
Working with Resonance Chiral Theory, within the two resonance multiplets saturation scheme, we satisfy leading (and some subleading) chiral and asymptotic QCD constraints and accurately fit simultaneously the π
0
, η, η′ transition form factors, for single and double virtuality. In the latter case, we supplement the few available measurements with lattice data to ensure a faithful description. Mainly due to the new results for the doubly virtual case, we improve over existing descriptions for the η and η′. Our evaluation of the corresponding pole contributions to the hadronic light-by-light piece of the muon g − 2 read:
$$ {a}_{\mu}^{\pi^0-\textrm{pole}}=\left(61.9\pm {0.6}_{-1.5}^{+2.4}\right)\times {10}^{-11} $$
a
μ
π
0
−
pole
=
61.9
±
0.6
−
1.5
+
2.4
×
10
−
11
,
$$ {a}_{\mu}^{\eta -\textrm{pole}}=\left(15.2\pm {0.5}_{-0.8}^{+1.1}\right)\times {10}^{-11} $$
a
μ
η
−
pole
=
15.2
±
0.5
−
0.8
+
1.1
×
10
−
11
and
$$ {a}_{\mu}^{\eta^{\prime }-\textrm{pole}}=\left(14.2\pm {0.7}_{-0.9}^{+1.4}\right)\times {10}^{-11} $$
a
μ
η
′
−
pole
=
14.2
±
0.7
−
0.9
+
1.4
×
10
−
11
, for a total of
$$ {a}_{\mu}^{\pi^0+\eta +{\eta}^{\prime }-\textrm{pole}}=\left(91.3\pm {1.0}_{-1.9}^{+3.0}\right)\times {10}^{-11} $$
a
μ
π
0
+
η
+
η
′
−
pole
=
91.3
±
1.0
−
1.9
+
3.0
×
10
−
11
, where the first and second errors are the statistical and systematic uncertainties, respectively.
Springer Science and Business Media LLC
Title: Improved π0, η, η′ transition form factors in resonance chiral theory and their $$ {a}_{\mu}^{\textrm{HLbL}} $$ contribution
Description:
Abstract
Working with Resonance Chiral Theory, within the two resonance multiplets saturation scheme, we satisfy leading (and some subleading) chiral and asymptotic QCD constraints and accurately fit simultaneously the π
0
, η, η′ transition form factors, for single and double virtuality.
In the latter case, we supplement the few available measurements with lattice data to ensure a faithful description.
Mainly due to the new results for the doubly virtual case, we improve over existing descriptions for the η and η′.
Our evaluation of the corresponding pole contributions to the hadronic light-by-light piece of the muon g − 2 read:
$$ {a}_{\mu}^{\pi^0-\textrm{pole}}=\left(61.
9\pm {0.
6}_{-1.
5}^{+2.
4}\right)\times {10}^{-11} $$
a
μ
π
0
−
pole
=
61.
9
±
0.
6
−
1.
5
+
2.
4
×
10
−
11
,
$$ {a}_{\mu}^{\eta -\textrm{pole}}=\left(15.
2\pm {0.
5}_{-0.
8}^{+1.
1}\right)\times {10}^{-11} $$
a
μ
η
−
pole
=
15.
2
±
0.
5
−
0.
8
+
1.
1
×
10
−
11
and
$$ {a}_{\mu}^{\eta^{\prime }-\textrm{pole}}=\left(14.
2\pm {0.
7}_{-0.
9}^{+1.
4}\right)\times {10}^{-11} $$
a
μ
η
′
−
pole
=
14.
2
±
0.
7
−
0.
9
+
1.
4
×
10
−
11
, for a total of
$$ {a}_{\mu}^{\pi^0+\eta +{\eta}^{\prime }-\textrm{pole}}=\left(91.
3\pm {1.
0}_{-1.
9}^{+3.
0}\right)\times {10}^{-11} $$
a
μ
π
0
+
η
+
η
′
−
pole
=
91.
3
±
1.
0
−
1.
9
+
3.
0
×
10
−
11
, where the first and second errors are the statistical and systematic uncertainties, respectively.
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