The impact of a 4th generation on mixing and CP violation in the charm system
We study mixing in the presence of a fourth generation of quarks. In particular, we calculate the size of the allowed CP violation which is found at the observable level well beyond anything possible with CKM dynamics. We calculate the semileptonic asymmetry a SL ( D ) and the mixing induced CP asym...
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Published in: | The journal of high energy physics Vol. 2010; no. 7 |
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Main Authors: | , , , , , |
Format: | Journal Article |
Language: | English |
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01-07-2010
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Abstract | We study
mixing in the presence of a fourth generation of quarks. In particular, we calculate the size of the allowed CP violation which is found at the observable level well beyond anything possible with CKM dynamics. We calculate the semileptonic asymmetry
a
SL
(
D
) and the mixing induced CP asymmetry η
f
S
f
(
D
) which are correlated with each other. We also investigate the correlation of η
f
S
f
(
D
) with a number of prominent observables in other mesonic systems like ε′/ε, Br(
K
L
→ π
0
), Br(
K
+
→ π
+
), Br(
B
s
→ μ
+
μ
-
), Br(
B
d
→ μ
+
μ
-
) and finally
S
ψϕ
(
B
s
) in the Bs system. We identify a clear pattern of flavour and CP violation predicted by the SM4 model: While simultaneous large 4G effects in the
K
and
D
systems are possible, accompanying large NP effects in the
B
d
system are disfavoured. However this behaviour is not as pronounced as found for the LHT and RSc models. In contrast to this, sizeable CP violating effects in the
B
s
system are possible unless extreme effects in η
f
S
f
(
D
) are found, and Br(
B
s
→ μ
+
μ
-
) can be strongly enhanced regardless of the situation in the
D
system. We find that, on the other hand,
S
ψϕ
(
B
s
) > 0.2 combined with the measured ε′/ε significantly diminishes 4G effects within the
D
system. |
---|---|
AbstractList | We study
mixing in the presence of a fourth generation of quarks. In particular, we calculate the size of the allowed CP violation which is found at the observable level well beyond anything possible with CKM dynamics. We calculate the semileptonic asymmetry
a
SL
(
D
) and the mixing induced CP asymmetry η
f
S
f
(
D
) which are correlated with each other. We also investigate the correlation of η
f
S
f
(
D
) with a number of prominent observables in other mesonic systems like ε′/ε, Br(
K
L
→ π
0
), Br(
K
+
→ π
+
), Br(
B
s
→ μ
+
μ
-
), Br(
B
d
→ μ
+
μ
-
) and finally
S
ψϕ
(
B
s
) in the Bs system. We identify a clear pattern of flavour and CP violation predicted by the SM4 model: While simultaneous large 4G effects in the
K
and
D
systems are possible, accompanying large NP effects in the
B
d
system are disfavoured. However this behaviour is not as pronounced as found for the LHT and RSc models. In contrast to this, sizeable CP violating effects in the
B
s
system are possible unless extreme effects in η
f
S
f
(
D
) are found, and Br(
B
s
→ μ
+
μ
-
) can be strongly enhanced regardless of the situation in the
D
system. We find that, on the other hand,
S
ψϕ
(
B
s
) > 0.2 combined with the measured ε′/ε significantly diminishes 4G effects within the
D
system. We study mixing in the presence of a fourth generation of quarks. In particular, we calculate the size of the allowed CP violation which is found at the observable level well beyond anything possible with CKM dynamics. We calculate the semileptonic asymmetry aSL(D) and the mixing induced CP asymmetry ηfSf (D) which are correlated with each other. We also investigate the correlation of ηfSf (D) with a number of prominent observables in other mesonic systems like ε′/ε, Br(KL → π0), Br(K+ → π+), Br(Bs → μ+μ-), Br(Bd → μ+μ-) and finally Sψϕ(Bs) in the Bs system. We identify a clear pattern of flavour and CP violation predicted by the SM4 model: While simultaneous large 4G effects in the K and D systems are possible, accompanying large NP effects in the Bd system are disfavoured. However this behaviour is not as pronounced as found for the LHT and RSc models. In contrast to this, sizeable CP violating effects in the Bs system are possible unless extreme effects in ηfSf (D) are found, and Br(Bs → μ+μ-) can be strongly enhanced regardless of the situation in the D system. We find that, on the other hand, Sψϕ(Bs) > 0.2 combined with the measured ε′/ε significantly diminishes 4G effects within the D system. |
ArticleNumber | 94 |
Author | Buras, Andrzej J. Duling, Björn Recksiegel, Stefan Feldmann, Thorsten Promberger, Christoph Heidsieck, Tillmann |
Author_xml | – sequence: 1 givenname: Andrzej J. surname: Buras fullname: Buras, Andrzej J. organization: Physik Department, Technische Universität München, TUM Institute for Advanced Study, Technische Universität München – sequence: 2 givenname: Björn surname: Duling fullname: Duling, Björn organization: Physik Department, Technische Universität München – sequence: 3 givenname: Thorsten surname: Feldmann fullname: Feldmann, Thorsten organization: Physik Department, Technische Universität München – sequence: 4 givenname: Tillmann surname: Heidsieck fullname: Heidsieck, Tillmann email: theid@ph.tum.de organization: Physik Department, Technische Universität München – sequence: 5 givenname: Christoph surname: Promberger fullname: Promberger, Christoph organization: Physik Department, Technische Universität München – sequence: 6 givenname: Stefan surname: Recksiegel fullname: Recksiegel, Stefan organization: Physik Department, Technische Universität München |
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CitedBy_id | crossref_primary_10_1016_j_nuclphysb_2011_11_023 crossref_primary_10_1016_j_physletb_2012_06_075 crossref_primary_10_1140_epjc_s10052_012_1867_7 crossref_primary_10_1140_epjc_s10052_022_10299_9 crossref_primary_10_1103_PhysRevD_86_115008 crossref_primary_10_1007_JHEP06_2012_007 crossref_primary_10_1103_PhysRevD_83_114510 crossref_primary_10_1007_JHEP07_2021_099 crossref_primary_10_1002_prop_201100062 crossref_primary_10_1103_PhysRevD_85_114035 crossref_primary_10_1155_2013_672972 crossref_primary_10_1103_PhysRevD_85_095025 crossref_primary_10_1103_PhysRevD_82_055015 crossref_primary_10_1016_j_nuclphysb_2011_02_018 crossref_primary_10_1016_j_physletb_2011_07_024 crossref_primary_10_1103_PhysRevD_82_035018 crossref_primary_10_1103_PhysRevD_82_095006 crossref_primary_10_1007_JHEP11_2010_121 crossref_primary_10_1007_JHEP09_2010_104 crossref_primary_10_1155_2013_910275 crossref_primary_10_1103_PhysRevD_83_035017 crossref_primary_10_1103_PhysRevD_92_013002 crossref_primary_10_1103_PhysRevD_84_053009 |
Cites_doi | 10.1016/0550-3213(94)90044-2 10.1088/1126-6708/2009/03/001 10.1088/1126-6708/2009/03/108 10.1140/epjc/s10052-006-0137-y 10.1088/1126-6708/2009/07/097 10.1103/PhysRevLett.97.101801 10.1103/PhysRevLett.102.211802 10.1007/JHEP03(2010)009 10.1016/0550-3213(90)90373-L 10.1140/epjc/s10052-009-1173-1 10.1016/j.nuclphysb.2009.12.019 10.1103/PhysRevLett.103.071602 10.1186/1754-0410-3-4 10.1088/1126-6708/2007/01/066 10.1016/S0370-1573(99)00095-2 10.1134/S1063778810040095 10.1007/JHEP03(2010)023 10.1016/j.physletb.2008.07.018 10.1016/j.physletb.2010.04.012 10.1140/epjc/s2003-01154-0 10.1016/j.physletb.2008.08.058 10.1016/j.physletb.2009.12.048 10.1016/0370-2693(88)90994-X |
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Keywords | Rare Decays Beyond Standard Model CP violation |
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mixing in the presence of a fourth generation of quarks. In particular, we calculate the size of the allowed CP violation which is found at the... We study mixing in the presence of a fourth generation of quarks. In particular, we calculate the size of the allowed CP violation which is found at the... |
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SubjectTerms | Asymmetry Classical and Quantum Gravitation CP violation Elementary Particles Flavor (particle physics) High energy physics Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum Physics Relativity Theory String Theory |
Title | The impact of a 4th generation on mixing and CP violation in the charm system |
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