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Spontaneous Flavor ViolationSamuel Homiller — [email protected]
Samuel HomillerC. N. Yang Institute for Theoretical Physics
& Brookhaven Natl. Lab
Spontaneous Flavor Violation and the 2HDM
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Based on arXiv:1811.00017 and 190X.XXXX
In collaboration with D. Egaña-Ugrinovic and Patrick Meade
Phenomenology Symposium, May 7, 2019University of Pittsburgh
Samuel Homiller — [email protected] Spontaneous Flavor Violation
• The LHC has a broad, active program searching for new physics (NP) at the TeV scale
• Great time to examine our assumptions about how NP couples to the Standard Model
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The Search for New Physics
Luca Silvestrini, UTFit
• Flavor violation bounds are already probing ~ 100s TeV scale. How do we reconcile this disparity?
Samuel Homiller — [email protected] Spontaneous Flavor Violation �3
Avoiding Flavor Bounds Requires Assumptions
λd†2,ij Qi dj Hc
2, ξij (d†i iσμ dj) Z′�μ
For flavored new physics, simplest assumption is Minimal Flavor Violation
In a 2HDM MFV implies: λu2,ij ∝ yu
SM, λd2,ij ∝ yd
SM
This implicitly assumes NP couples mainly to third generation quarks!
Yu = diag(ySMu , ySM
c , ySMt )
Yd = diag(ySMd , ySM
s , ySMb )
FCNCs in SM suppressed by Yukawa & CKM factors
yuSM = (VT Yu)ij, yd
SM = Yd
yuSM =
10−5 10−3 10−2
10−6 10−3 10−2
10−8 10−4 1
Samuel Homiller — [email protected] Spontaneous Flavor Violation �4
Alignment Suppresses FCNCs
ℒ ⊃ − VTijY
u Qi H uj + Yd Qi Hc dj
+Kd Qi Hc2 dj
This is clear when we look in a particular basis:
Couplings to new physics can be arbitrarily large, without introducing FCNCs
But demanding alignment without a UV completion is very ad hoc
d
s
H2
12 12
d
s
∝ κ212 = 0
Kd = diag(κd, κs, κb)
Yu = diag(ySMu , ySM
c , ySMt )
Yd = diag(ySMd , ySM
s , ySMb )
Samuel Homiller — [email protected] Spontaneous Flavor Violation �5
Spontaneous Flavor Violation
Samuel Homiller — [email protected] Spontaneous Flavor Violation �6
A UV Completion for Flavor Alignment
Flavor Violation “in the up sector”
Idea: All quark family number & CP breaking via renormalization of either right-handed up- or down-type quarks
L � �VTij Y
uQi H uj + Y
dQi H
cdj +K
dQi H
c2 dj
Couplings to the other sector remain aligned⟹
L � iZuij u
†i �
µDµuj + id†i �µDµdi + iQ†
i �µDµQi+
Samuel Homiller — [email protected] Spontaneous Flavor Violation �7
A UV Completion for Flavor Alignment
Note: Two distinct theories: up- or down-type SFV
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.
.
.
.
.
�n
u†
u
⟹ iZuij u†
i σμDμuj
L � iZuij u
†i �
µDµuj + id†i �µDµdi + iQ†
i �µDµQi+
Mixing with Spontaneously Broken Flavor Vacuum
Samuel Homiller — [email protected] Spontaneous Flavor Violation �8
Flavor Bounds in an SFV 2HDM
Order ~ 0.1 couplings to first and second generation quarks are allowed for a large range of masses!
Charged Higgs Contributions to FCNCs arise at loop-level
Samuel Homiller — [email protected] Spontaneous Flavor Violation
Heavy Higgs Produced in Tree-Level Quark Fusion, Decays to Dijets
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Limits from Dijet Searches
Much of the parameter space is more efficiently probed with colliders — even for O(100 GeV) new Higgses!
Samuel Homiller — [email protected] Spontaneous Flavor Violation �10
Mixing Leads to Enhancement of SM Yukawas
-102
-102
-30
-30
-10
-1010
10
30
30
102
102
-0.4 -0.2 0.0 0.2 0.4
-0.4
-0.2
0.0
0.2
0.4
-10
-10
-5
-5
-2
-22
2
5
5
10
10
-0.4 -0.2 0.0 0.2 0.4
-0.4
-0.2
0.0
0.2
0.4
Realistic targets for quark-flavor taggers!
Up-Type SFV Down-Type SFV
Samuel Homiller — [email protected] Spontaneous Flavor Violation
• Spontaneous Flavor Violation ensures flavor alignment — allows for large couplings to light quarks
• In the 2HDM, this leads to strong production and enhanced Yukawas
• SFV can be applied to any BSM model!
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Conclusions
SMEFT,MSSM,Z-primes,Leptoquarks,Vector-like quarks,Axions,Colored Scalars,…
• Flavor assumptions have drastic implications for new physics searches and collider phenomenology
Samuel Homiller — [email protected] Spontaneous Flavor Violation �12
Backup
Samuel Homiller — [email protected] Spontaneous Flavor Violation �13
Backup: Details of the UV Completion
UA
uj
SjA
ui
S⇤iA
ℒ ⊃ MAB UA UB + ξ SiA ui UA
U(3)U U(3)U U(3)u U(1)B Z2
U 3 1/3 �1U 3 �1/3 �1S 3 3 �1
Introduce mixing between up-quark and heavy VLQs in a flavor breaking vacuum
Integrating out heavy quarks leads to wave-function renormalization of the SM up-quarks
No additional spurions/fields transforming under U(3)u
�⇥⌘uij Qi H uj � ⌘
dij Qi H
cdj + h.c.
⇤+ LBSM
The source of all flavor-breaking! CKM matrix arises from returning to
canonical basisZuij = �ij +
⇠⇤⇠
M⇤AMA
S⇤iASjA
Samuel Homiller — [email protected] Spontaneous Flavor Violation �14
Backup: Additional Flavor Bounds
Samuel Homiller — [email protected] Spontaneous Flavor Violation �15
Backup: Additional Flavor Bounds
Samuel Homiller — [email protected] Spontaneous Flavor Violation �16
Backup: Additional Collider Bounds
Samuel Homiller — [email protected] Spontaneous Flavor Violation �17
Backup: Additional Collider Bounds