heft copenhagen magro - kuremedios francesco riva (cern) in collaboration with liu, pomarol,...
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![Page 1: HEFT Copenhagen magro - kuREMEDIOS Francesco Riva (CERN) In collaboration with Liu, Pomarol, Rattazzi 1603.03064, Azatov, Contino, Machado 1607.05236 8cm 1cm 8cm 35 km Precision=10-6](https://reader036.vdocuments.mx/reader036/viewer/2022070221/6135fde20ad5d2067647bb23/html5/thumbnails/1.jpg)
REMEDIOS
Francesco Riva (CERN)
In collaboration with Liu, Pomarol, Rattazzi 1603.03064,
Azatov, Contino, Machado 1607.05236
8cm1cm
8cm35 km
Precision=10-6
LHC AlpTransitL=27km L=35kmEbeam=362MJ Etrain=362MJ
Precision=??
- LHC precision tests (di/tri-boson): what is being searched for? -
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REMEDIOS
Francesco Riva (CERN)
In collaboration with Liu, Pomarol, Rattazzi 1603.03064,
Azatov, Contino, Machado 1607.05236
8cm1cm
8cm35 km
Precision=10-6
LHC AlpTransitL=27km L=35kmEbeam=362MJ Etrain=362MJ
Precision=??
- LHC precision tests (di/tri-boson): what is being searched for? -
![Page 3: HEFT Copenhagen magro - kuREMEDIOS Francesco Riva (CERN) In collaboration with Liu, Pomarol, Rattazzi 1603.03064, Azatov, Contino, Machado 1607.05236 8cm 1cm 8cm 35 km Precision=10-6](https://reader036.vdocuments.mx/reader036/viewer/2022070221/6135fde20ad5d2067647bb23/html5/thumbnails/3.jpg)
Two modes of exploration at LHC:A) Direct Searches:
![Page 4: HEFT Copenhagen magro - kuREMEDIOS Francesco Riva (CERN) In collaboration with Liu, Pomarol, Rattazzi 1603.03064, Azatov, Contino, Machado 1607.05236 8cm 1cm 8cm 35 km Precision=10-6](https://reader036.vdocuments.mx/reader036/viewer/2022070221/6135fde20ad5d2067647bb23/html5/thumbnails/4.jpg)
Two modes of exploration at LHC:A) Direct Searches:
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Two modes of exploration at LHC:A) Direct Searches:
B) Indirect Searches:
1) On SM resonance E=mZ, mh 2) Off SM resonance E>>mZ, mh
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Two modes of exploration at LHC:A) Direct Searches:
B) Indirect Searches:
1) On SM resonance E=mZ, mh 2) Off SM resonance E>>mZ, mh
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From LHCPlenty of Data in multiboson processes:
Why nobody cares??
��
?
?
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why nobody cares
Part 1
![Page 9: HEFT Copenhagen magro - kuREMEDIOS Francesco Riva (CERN) In collaboration with Liu, Pomarol, Rattazzi 1603.03064, Azatov, Contino, Machado 1607.05236 8cm 1cm 8cm 35 km Precision=10-6](https://reader036.vdocuments.mx/reader036/viewer/2022070221/6135fde20ad5d2067647bb23/html5/thumbnails/9.jpg)
These parameters EFT coefficients:$��
g⇤M2
✏abcWa ⌫µ W b
⌫⇢Wc ⇢µdim-6$
1 Smallness why nobody cares
hZ3 H†DµHD⇢B
⇢⌫ B̃
µ⌫$ dim-8fT,0 W 4µ⌫$
Involve the transverse polarizations of vectors
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These parameters EFT coefficients:$��
g⇤M2
✏abcWa ⌫µ W b
⌫⇢Wc ⇢µdim-6$
1
In popular models (e.g. SUSY, CH), VT elementary, these are tiny:
M g�� ⇠ g3
16⇡2
m2W
M2SILH: Giudice,Grojean,Pomarol,Rattazzi’2007
Smallness why nobody cares
hZ3 H†DµHD⇢B
⇢⌫ B̃
µ⌫$ dim-8fT,0 W 4µ⌫$
Involve the transverse polarizations of vectors
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2
For states have well defined helicity hE � mW
Amplitudes for 2➙2 with different htot don’t interfere
Azatov,Contino,Machado,FR’16
why nobody caresNon-Interference for BSM6 amplitudes
There is in fact one more obstruction to test transverse vectors:
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2
For states have well defined helicity hE � mW
Amplitudes for 2➙2 with different htot don’t interfere
Azatov,Contino,Machado,FR’16
why nobody caresNon-Interference for BSM6 amplitudes
There is in fact one more obstruction to test transverse vectors:
Any BSM dim-6 operator
tree level + at least one transverse vector No interference
Selection Rule:
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How? i) Helicity sums:n=m+m’-2 legs
Non-Interference for BSM6 amplitudes Azatov,Contino,Machado,FR’16
why nobody cares2
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How? i) Helicity sums:n=m+m’-2 legs
SM or BSM6 so that on-shell condition satisfied also for A3
p 2 Cp2 = 0
Non-Interference for BSM6 amplitudes Azatov,Contino,Machado,FR’16
why nobody cares2
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ii) Helicity of 3-point coupling dimension:$
Azatov,Contino,Machado,FR’16
How?
gSM) |hSM | = 1
BSM6) |hBSM | = 3⇠ 1
⇤2
Non-Interference for BSM6 amplitudes why nobody cares
2
From: Little group scaling + dimensional analysis(see e.g. Elvang,Huang’13)
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How? iii) SUSY* Ward Identities: |h(ASM4 )| < 2
Non-Interference for BSM6 amplitudes Azatov,Contino,Machado,FR’16
why nobody cares
(except ) + + + +
2
(aka Ultra Helicity Violation)
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How? iii) SUSY* Ward Identities: |h(ASM4 )| < 2
Non-Interference for BSM6 amplitudes Azatov,Contino,Machado,FR’16
why nobody cares
(except ) + + + +
2
(aka Ultra Helicity Violation)
*in the limit of either yu=0 or yd=yl=0:SM upliftable to SUSY+R-parity (with 1 Higgs doublet)
Grisaru,Pendleton,vanNieuwenhuizen’77
�SM
�SM
�SM
�SM
�SM
�Susy
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How? iii) SUSY* Ward Identities: |h(ASM4 )| < 2
Non-Interference for BSM6 amplitudes Azatov,Contino,Machado,FR’16
why nobody cares
➙
[Q, V ] ⇠ [Q, ] ⇠ V
0 = h0|[Q, +V +V +V +]|0i =X
i
h0| +...[Q, V +]...V +|0ie.g. / h0|V +V +V +V +|0i
+ + · · · = 0
SM :
(except ) + + + +
2
(aka Ultra Helicity Violation)
*in the limit of either yu=0 or yd=yl=0:SM upliftable to SUSY+R-parity (with 1 Higgs doublet)
Grisaru,Pendleton,vanNieuwenhuizen’77
�SM
�SM
�SM
�SM
�SM
�Susy
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How? iii) SUSY* Ward Identities: |h(ASM4 )| < 2
Non-Interference for BSM6 amplitudes Azatov,Contino,Machado,FR’16
why nobody cares
➙
[Q, V ] ⇠ [Q, ] ⇠ V
0 = h0|[Q, +V +V +V +]|0i =X
i
h0| +...[Q, V +]...V +|0ie.g. / h0|V +V +V +V +|0i
+ + · · · = 0
SM :
BSM : Operators with transverse V not supersymmetrizableElias-Miro,Espinosa,Pomarol’14
(except ) + + + +
2
(aka Ultra Helicity Violation)
*in the limit of either yu=0 or yd=yl=0:SM upliftable to SUSY+R-parity (with 1 Higgs doublet)
Grisaru,Pendleton,vanNieuwenhuizen’77
�SM
�SM
�SM
�SM
�SM
�Susy
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i) Helicity sumsii) Helicity of 3-point coupling dimension$
iii) SUSY* Ward Identities |h(ASM4 )| < 2
Non-Interference for BSM6 amplitudes Azatov,Contino,Machado,FR’16
why nobody cares
How?
2
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i) Helicity sumsii) Helicity of 3-point coupling dimension$
iii) SUSY* Ward Identities |h(ASM4 )| < 2
Non-Interference for BSM6 amplitudes Azatov,Contino,Machado,FR’16
why nobody cares
How?
BSM6
SM+SM
+SM
htot = 1� 1 = 0
htot = 1± 3 = 2, 4
2
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i) Helicity sumsii) Helicity of 3-point coupling dimension$
iii) SUSY* Ward Identities |h(ASM4 )| < 2
No Interference (dim-6, 4-point)
Non-Interference for BSM6 amplitudes Azatov,Contino,Machado,FR’16
why nobody cares
How?
BSM6
SM+SM
+SM
htot = 1� 1 = 0
htot = 1± 3 = 2, 4
2
![Page 23: HEFT Copenhagen magro - kuREMEDIOS Francesco Riva (CERN) In collaboration with Liu, Pomarol, Rattazzi 1603.03064, Azatov, Contino, Machado 1607.05236 8cm 1cm 8cm 35 km Precision=10-6](https://reader036.vdocuments.mx/reader036/viewer/2022070221/6135fde20ad5d2067647bb23/html5/thumbnails/23.jpg)
i) Helicity sumsii) Helicity of 3-point coupling dimension$
iii) SUSY* Ward Identities |h(ASM4 )| < 2
No Interference (dim-6, 4-point)
Non-Interference for BSM6 amplitudes Azatov,Contino,Machado,FR’16
why nobody cares
How?
BSM6
SM+SM
+SM
htot = 1� 1 = 0
htot = 1± 3 = 2, 4
2
interference vanishes
� /X
|Amp|2 ' SM2(1 + ciE2
M2+ c2i
E4
M4)
Small effects, are even smaller!
![Page 24: HEFT Copenhagen magro - kuREMEDIOS Francesco Riva (CERN) In collaboration with Liu, Pomarol, Rattazzi 1603.03064, Azatov, Contino, Machado 1607.05236 8cm 1cm 8cm 35 km Precision=10-6](https://reader036.vdocuments.mx/reader036/viewer/2022070221/6135fde20ad5d2067647bb23/html5/thumbnails/24.jpg)
Present constraints:
LEP2:�� 2 [�0.059, 0.017]95%C.L. (LEP EW: 1302.3415)
E = 130� 209GeV
) M & 30 GeV
LHC:
why nobody cares
�� 2 [�0.019,+0.019]…E & 1TeV
…so small that is doesn’t even make sense as an EFT.
Non-Interference+Smallness
�� ⇠ g2
16⇡2
m2W
M2
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why nobody cares?Because there is no structured scenario
where these searches are self-consistent (need strong coupling)
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why caring (Remedios)
Part 2
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Strongly Coupled BSM?
quantum effects generally propagate new couplings to the whole SM
⇣ ⌘! !
How can SM be light and weakly coupled at E<mw and strongly coupled at E>>mw?
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Strongly Coupled BSM?
quantum effects generally propagate new couplings to the whole SM
⇣ ⌘! !
How can SM be light and weakly coupled at E<mw and strongly coupled at E>>mw?
Need shielding: Approximate Symmetries broken in SM
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Strongly Coupled BSM?
quantum effects generally propagate new couplings to the whole SM
⇣ ⌘! !
How can SM be light and weakly coupled at E<mw and strongly coupled at E>>mw?
Need shielding: Approximate Symmetries broken in SM
∼E2
mW ME
gSM2
g*2g2(E)
A ' g2SM
✓1 +
g2⇤g2SM
E2
M2
◆⌘ g2(E)
Symm
etry
Symm
etry Higher-dim
operators (dim-6, sim-8…)
SM Lagrangian (dim-4)
IrrelevantMarginal
g* stronggSM weak
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Strongly Coupled BSM and Approximate Symmetries
Scalars: Composite HiggsHiggs is a Pseudo Goldstone boson from new strong sector (symm=SO(5)/SO(4))
Georgi,Kaplan’84; Agashe,Contino,Nomura,Pomarol’04; Giudice,Grojean,Pomarol,Rattazzi’07;…
H ! H + c g⇤@µH ✏HShift Symm:+n.l. +n.l. symmetry
H
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Strongly Coupled BSM and Approximate Symmetries
Scalars: Composite HiggsHiggs is a Pseudo Goldstone boson from new strong sector (symm=SO(5)/SO(4))
Georgi,Kaplan’84; Agashe,Contino,Nomura,Pomarol’04; Giudice,Grojean,Pomarol,Rattazzi’07;…
H ! H + c g⇤@µH ✏HShift Symm:+n.l. +n.l.
g2⇤M2
(@µ|H|2)2 �|H|4large small
symmetryH
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Strongly Coupled BSM and Approximate Symmetries
Scalars: Composite HiggsHiggs is a Pseudo Goldstone boson from new strong sector (symm=SO(5)/SO(4))
Georgi,Kaplan’84; Agashe,Contino,Nomura,Pomarol’04; Giudice,Grojean,Pomarol,Rattazzi’07;…
H ! H + c g⇤@µH ✏HShift Symm:+n.l. +n.l.
g2⇤M2
(@µ|H|2)2 �|H|4large small
symmetryH
A ⇠ �
✓1 +
g2⇤�
E2
M2
◆Large effects VLVL➙VLVL at high-E:
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Strongly Coupled BSM and Approximate Symmetries
Scalars: Composite Higgs
Vectors: ?
Higgs is a Pseudo Goldstone boson from new strong sector (symm=SO(5)/SO(4))Georgi,Kaplan’84; Agashe,Contino,Nomura,Pomarol’04; Giudice,Grojean,Pomarol,Rattazzi’07;…
H ! H + c g⇤@µH ✏HShift Symm:+n.l. +n.l.
g2⇤M2
(@µ|H|2)2 �|H|4large small
symmetryH
A ⇠ �
✓1 +
g2⇤�
E2
M2
◆Large effects VLVL➙VLVL at high-E:
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Problem: Gauge bosons: weak SM coupling ( )@µ + igAµ
Naively, contrary to scalars, gauge bosons couple universally
Liu,Pomarol,Rattazzi,FR’16
Strong transverse vectors at high-E
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Problem: Gauge bosons: weak SM coupling ( )@µ + igAµ
Naively, contrary to scalars, gauge bosons couple universally
Liu,Pomarol,Rattazzi,FR’16
Strong transverse vectors at high-E
However:
Strong higher-d interactions
g = 0Aµ composite, g*
No light charged d.o.f (but large dipoles possible)
(Euler-Heisenberg)
L =M4
g2⇤L
@µM
, g⇤F̂µ⌫
M2,�
!
�
L =M4
g2⇤L
@µM
, g⇤F̂µ⌫
M2,�
!
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Problem: Gauge bosons: weak SM coupling ( )@µ + igAµ
Naively, contrary to scalars, gauge bosons couple universally
Liu,Pomarol,Rattazzi,FR’16
Strong transverse vectors at high-E
However:
Strong higher-d interactions
g = 0Aµ composite, g*
No light charged d.o.f (but large dipoles possible)
(Euler-Heisenberg)
L =M4
g2⇤L
@µM
, g⇤F̂µ⌫
M2,�
!
�
L =M4
g2⇤L
@µM
, g⇤F̂µ⌫
M2,�
!
g 6= 0
Light d.o.f. with charge
Weak marginal interactions
g
g⇤
L =M4
g2⇤L
✓@µ + igAµ
M, g⇤
Fµ⌫
M2,�
◆
q =g
g⇤
L =M4
g2⇤L
@µM
, g⇤F̂µ⌫
M2,�
!
⌧ 1
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Strong transverse vectors at high-E
g ! 0Inonu-Wigner Contraction (’53)
#generators invariant (Like Poincaré->Galilei)
Non-abelian SU(2)localU(1)3
local
⇥ SU(2)global
Liu,Pomarol,Rattazzi,FR’16
What symmetry is broken by g and not by g*? none…
Monopole interactions (covariant derivative)
Multipole interactions (field strengths)
g⇤Faµ⌫ @µ + igAa
µTa
Symmetry deformation: a new selection rule to build EFTs (different from spurions)
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Strong transverse vectors: Implications1
M2(D⇢W
a,⌫µ )2 M & 2TeV
Barbieri,Pomarol,Rattazzi,Strumia’04
W,Y ' m2W
M2. 10�3 ➙
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Strong transverse vectors: Implications1
M2(D⇢W
a,⌫µ )2 M & 2TeV
Barbieri,Pomarol,Rattazzi,Strumia’04
W,Y ' m2W
M2. 10�3 ➙
�� ⇡ g⇤m2
W
M2g⇤M2
✏abcWa ⌫µ W b
⌫⇢Wc ⇢µ M &
rg⇤4⇡
2.2 TeV
g2⇤M4
W 4µ⌫
fT,0 ⇡ g2⇤M4 M &
rg⇤4⇡
1.1 TeV
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Strong transverse vectors: Implications
��
W,Y���� ���� ���� ����
�
�
�
�
�
��
��
� [���]
�*
�����
�=����fT,0 ⇡ g2⇤
M4
So far the only models that motivate these searches consistently
Remedios (Remedios the Beauty was not a creature of this world- Gabriel Garcia Marquez )
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⇠ g2SM
Strong transverse vectors: ImplicationsWT scattering
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⇠ g2SM
⇠ gg⇤E2
M2g⇤M2
✏abcWa ⌫µ W b
⌫⇢Wc ⇢µ
Strong vectors:D6
Strong transverse vectors: ImplicationsWT scattering
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⇠ g2SM
⇠ gg⇤E2
M2g⇤M2
✏abcWa ⌫µ W b
⌫⇢Wc ⇢µ
Strong vectors:D6
Strong transverse vectors: ImplicationsWT scattering
⇠ g2⇤E4
M4
(NDA: 4-point vertex≈ coupling2)
g2⇤M4
W 4µ⌫D8
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⇠ g2SM
⇠ gg⇤E2
M2g⇤M2
✏abcWa ⌫µ W b
⌫⇢Wc ⇢µ
Strong vectors:D6
Strong transverse vectors: ImplicationsWT scattering
. 1
. 1
g⇤g
E2
M2
g⇤g
E2
M2
�ABSM
ASM. 1 dimension-6 analysis ok
⇠ g2⇤E4
M4
(NDA: 4-point vertex≈ coupling2)
g2⇤M4
W 4µ⌫D8
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⇠ g2SM
⇠ gg⇤E2
M2g⇤M2
✏abcWa ⌫µ W b
⌫⇢Wc ⇢µ
Strong vectors:D6
Strong transverse vectors: ImplicationsWT scattering
⇠ g2⇤E4
M4
(NDA: 4-point vertex≈ coupling2)
g2⇤M4
W 4µ⌫
. 1
. 1
g⇤g
E2
M2
g⇤g
E2
M2
�ABSM
ASM. 1 dimension-6 analysis ok
D8
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⇠ g2SM
⇠ gg⇤E2
M2g⇤M2
✏abcWa ⌫µ W b
⌫⇢Wc ⇢µ
Strong vectors:D6
Strong transverse vectors: ImplicationsWT scattering
⇠ g2⇤E4
M4
(NDA: 4-point vertex≈ coupling2)
g2⇤M4
W 4µ⌫
. 1
. 1
g⇤g
E2
M2
g⇤g
E2
M2
�ABSM
ASM. 1 dimension-6 analysis ok
D8
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⇠ g2SM
⇠ gg⇤E2
M2g⇤M2
✏abcWa ⌫µ W b
⌫⇢Wc ⇢µ
Strong vectors:D6
Strong transverse vectors: ImplicationsWT scattering
⇠ g2⇤E4
M4
(NDA: 4-point vertex≈ coupling2)
g2⇤M4
W 4µ⌫D8
g⇤g
E2
M2
g⇤g
E2
M2
�ABSM
ASM& 1 dim-6 not ok! dim-8 dominate!
(EFT E/M expansion still valid: dimension-10 small)
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Strong transverse vectors: ImplicationsWT scattering
��� �����
���� ����+�����
���� ����
��� ��
� �� �
���
�π� ���
� π
�
� *
���� → ����
(EFT E/M expansion still valid: dimension-10 small)
Non-interference: even at low-E D8>D6
dim-8 always large for WW scattering
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Dimension-8
g2⇤M4
(W aµ⌫)
4Remedios Model: gg⇤M2
W a ⌫µ W b
⌫⇢WbµW a⇢W bµW a⇢
g ⌧ g⇤Dim-8 Dim-6
Approximate (Non-linear) symmetries go beyond shielding the SM…
(dimension-10 smaller by E2/M2)
Liu,Pomarol,Rattazzi,FR’16
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Dimension-8
g2⇤M4
(W aµ⌫)
4Remedios Model: gg⇤M2
W a ⌫µ W b
⌫⇢WbµW a⇢W bµW a⇢
g ⌧ g⇤Dim-8 Dim-6
H 2 ISO(4)/SO(4)Composite Higgs: (flat coset)
g2⇤M4
(DµH†D⌫H)2 ✏c
g2⇤M2
(H†DµH)2
Proportional to coset curvature
Approximate (Non-linear) symmetries go beyond shielding the SM…
(dimension-10 smaller by E2/M2)
Liu,Pomarol,Rattazzi,FR’16
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Dimension-8
g2⇤M4
(W aµ⌫)
4Remedios Model: gg⇤M2
W a ⌫µ W b
⌫⇢WbµW a⇢W bµW a⇢
g ⌧ g⇤Dim-8 Dim-6
H 2 ISO(4)/SO(4)Composite Higgs: (flat coset)
g2⇤M4
(DµH†D⌫H)2 ✏c
g2⇤M2
(H†DµH)2
Proportional to coset curvature
Fermions as Pseudo-GoldstinosBardeen, Visnjic’82; Bellazzini,FR’soon
� = ⇠ +i
2F 2@µ ( ̄�̄
µ⇠ � ⇠̄�̄µ )
g2⇤M4
(@µ ̄�µ )2 ✏SUSY
g2⇤M2
( ̄�µ )2
Approximate (Non-linear) symmetries go beyond shielding the SM…
(dimension-10 smaller by E2/M2)
Liu,Pomarol,Rattazzi,FR’16
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HEFT 993, 15456,…
HEFT2013-2016
HEFT2017HEFT2018
(from Brian)
fear not…
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HEFT 993, 15456,…
HEFT2013-2016
HEFT2017HEFT2018
(from Brian)
fear not…
Can there be symmetries that protect dimension-10 in 2➙2 processes?
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HEFT 993, 15456,…
HEFT2013-2016
HEFT2017HEFT2018
(from Brian)
fear not…
Can there be symmetries that protect dimension-10 in 2➙2 processes?
Adams,Arkani-hamed,Dubovsky,Nicolis,Rattazzi’06; Bellazzini’16;…
NO! Positivity constraints from analyticity,unitarity,crossing symm.:
L = @µ⇡@µ⇡ +
c8M4
(@µ⇡@µ⇡)2 +
c10M6
(@µ⇡@⌫@µ⇡)2
c8 > 0
A symmetry that protects dim-10 can never be considered exact
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ConclusionsLHC/LEP: many €€resources€€ to test transverse vectors
Not BSM motivated (non-interference, smallness in ordinary models)
Henning,Lu,Melia,Murayama’15; Lehman,Martin’15
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ConclusionsLHC/LEP: many €€resources€€ to test transverse vectors
Not BSM motivated (non-interference, smallness in ordinary models)
Remedios: structurally robust scenario for strong coupling- large multipoles/small monopoles- deformed symmetry
Henning,Lu,Melia,Murayama’15; Lehman,Martin’15
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ConclusionsLHC/LEP: many €€resources€€ to test transverse vectors
Not BSM motivated (non-interference, smallness in ordinary models)
Remedios: structurally robust scenario for strong coupling- large multipoles/small monopoles- deformed symmetry
Approximate symmetries can lead to dim-8 domination in 2➙2 processes
Motivation for some QGC searches
Motivation for dim-8 operator classification
New patterns for deviations from the SMHenning,Lu,Melia,Murayama’15; Lehman,Martin’15
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ConclusionsLHC/LEP: many €€resources€€ to test transverse vectors
Not BSM motivated (non-interference, smallness in ordinary models)
Remedios: structurally robust scenario for strong coupling- large multipoles/small monopoles- deformed symmetry
So far the hierarchy problem has shaped our picture of TeV-physics.
Here “Data-driven”: what can we learn from well-measured quantities?
Approximate symmetries can lead to dim-8 domination in 2➙2 processes
Motivation for some QGC searches
Motivation for dim-8 operator classification
New patterns for deviations from the SMHenning,Lu,Melia,Murayama’15; Lehman,Martin’15
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Conclusions
Precision Tests at LHC
EFT (M
otivat
ion/st
ructur
e)
BSM Perspective
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Through Partial Compositeness?
Either free or irrelevant
dim[O] � 2
No CFT or Warped Extra-D model exists
Ferrara,Gatto,Grillo’74,Mack’79
Relevant if dim[O] < 2
Unitarity
dim[J ] = 3Marginal
Strong transverse vectors: UV?
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Through Partial Compositeness?
Either free or irrelevant
dim[O] � 2
No CFT or Warped Extra-D model exists
Ferrara,Gatto,Grillo’74,Mack’79
Relevant if dim[O] < 2
Unitarity
dim[J ] = 3Marginal
Strong transverse vectors: UV?
dd
Strong transverse vectors=Remedios
(Remedios the Beauty was not a creature of this world- Gabriel Garcia Marquez )
No warped UV model
Remedy to motivate (some) LHC searches
…