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Unified Theories with U(2) Flavor Symmetry
High Energy Physics - Phenomenology · Submitted 23 Oct 1996
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim A fit to the fermion mass data leads to a prediction for the angles of the CKM unitarity triangle, which will allow a significant test of these unified U(2) theories.
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The abstract, sentence by sentence
A general operator expansion is presented for quark and lepton mass matrices in unified theories based on a U(2) flavor symmetry, with breaking parameter of order $V_{cb} \approx m_s/m_b \approx \sqrt{m_c/m_t}$. While solving the supersymmetric flavor-changing problem, a general form for the Yukawa couplings follows, leading to 9 relations among the fermion masses and mixings, 5 of which are precise. The combination of grand unified and U(2) symmetries provides a symmetry understanding for the anomalously small values of $m_u/m_c$ and $m_c/m_t$. A fit to the fermion mass data leads to a prediction for the angles of the CKM unitarity triangle, which will allow a significant test of these unified U(2) theories. A particular SO(10) model provides a simple realization of the general operator expansion. The lighter generation masses and the non-trivial structure of the CKM matrix are generated from the exchange of a single U(2) doublet of heavy vector generations. This model suggests that CP is spontaneously broken at the unification scale --- in which case there is a further reduction in the number of free parameters.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A general operator expansion is presented for quark and lepton mass matrices in unified theories based on a U(2) flavor symmetry, with breaking parameter of order $V_{cb} \approx m_s/m_b \approx \sqrt{m_c/m_t}$. | contribution 0.96 | 0.86 | 0.13 | asserted 1.00 |
| s1 | While solving the supersymmetric flavor-changing problem, a general form for the Yukawa couplings follows, leading to 9 relations among the fermion masses and mixings, 5 of which are precise. | result 0.88 | 0.85 | 0.30 | asserted 1.00 |
| s2 | The combination of grand unified and U(2) symmetries provides a symmetry understanding for the anomalously small values of $m_u/m_c$ and $m_c/m_t$. | interpretation 0.88 | 0.69 | 0.16 | asserted 1.00 |
| s3 | A fit to the fermion mass data leads to a prediction for the angles of the CKM unitarity triangle, which will allow a significant test of these unified U(2) theories. | result 0.83 | 0.87 | 0.30 | asserted 0.82 |
| s4 | A particular SO(10) model provides a simple realization of the general operator expansion. | contribution 0.51 | 0.70 | 0.05 | asserted 0.99 |
| s5 | The lighter generation masses and the non-trivial structure of the CKM matrix are generated from the exchange of a single U(2) doublet of heavy vector generations. | method 0.44 | 0.59 | 0.14 | asserted 0.99 |
| s6 | This model suggests that CP is spontaneously broken at the unification scale --- in which case there is a further reduction in the number of free parameters. | interpretation 0.92 | 0.55 | 0.13 | hedged possibility 1.00 |
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The paper
Original abstract
A general operator expansion is presented for quark and lepton mass matrices in unified theories based on a U(2) flavor symmetry, with breaking parameter of order $V_{cb} \approx m_s/m_b \approx \sqrt{m_c/m_t}$. While solving the supersymmetric flavor-changing problem, a general form for the Yukawa couplings follows, leading to 9 relations among the fermion masses and mixings, 5 of which are precise. The combination of grand unified and U(2) symmetries provides a symmetry understanding for the anomalously small values of $m_u/m_c$ and $m_c/m_t$. A fit to the fermion mass data leads to a prediction for the angles of the CKM unitarity triangle, which will allow a significant test of these unified U(2) theories. A particular SO(10) model provides a simple realization of the general operator expansion. The lighter generation masses and the non-trivial structure of the CKM matrix are generated from the exchange of a single U(2) doublet of heavy vector generations. This model suggests that CP is spontaneously broken at the unification scale --- in which case there is a further reduction in the number of free parameters.
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References
How the literature uses it
35 arXiv papers cite this in 46 sentences
Papers citing it · 25 sentences without a confident label
Compares with it 1 paper
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Let us contrast this with existing implementations of $U(2)$ breaking [ref] , which generate the flavor structure of the light families.
Hierarchies from Higher Flavor Spin · Introduction · 0.91
Cites it as background 18 papers
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To achieve this goal, we consider four basic hypotheses about the flavour structure of the soft-breaking terms: the Minimal Flavour Violation (MFV) hypothesis [ref] , a chiral $U(2)$ flavour symmetry [ref] , a $U(1)$ symmetry a la Froggatt-Nielsen [ref] , and finally the framework of disoriented $A$ terms [ref] .
Exploring the flavour structure of the high-scale MSSM · Introduction · 0.83
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Representative examples with $n_2=1$ and $n_3=0$ include $U(2)_all$ [ref] , $U(2)_ψ_L=q+ℓ$ [ref] , $U(2)_q+e^(c)$ and $U(2)_10 ×Z_2$ [ref] , as well as constructions such as $MFP=SU(2)_q ×U(1)_X$ [ref] and $SU(2)_all ×U(1)_F$ [ref] .
Hierarchies from Higher Flavor Spin · Introduction · 0.88
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In contrast to abelian models, where there is a lot of freedom in fixing the charges of the SM fermions under the flavour symmetry, non-abelian models [ref] are quite predictive for fermion mass matrices once the pattern of symmetry breaking is specified.
Anatomy and Phenomenology of FCNC and CPV Effects in SUSY Theories · Non-abelian Flavour Models · 0.93
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