Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M....
Transcript of Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M....
![Page 1: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/1.jpg)
Exploring the SM EFT with diboson production
1810.05149 with C. Grojean and M. Riembau190x.xxxxx with G. Durieux and M. Riembau190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia
Marc Montull(postdoc at DESY)
Based on:
The 27th International Workshop on Weak Interactions and Neutrinos
![Page 2: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/2.jpg)
As we know, the LHC discovered the first scalar and elementary (?) particleconsistent with the SM Higgs boson
With this discovery, the SM is complete !!
Are we done ?
![Page 3: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/3.jpg)
DMNeutrinos Inflation
Baryon asymmetryGravity
No! There are still many things to be understood … for instance
![Page 4: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/4.jpg)
DMNeutrinos Inflation
Baryon asymmetryGravity
Even more, the LHC will keep running until 2037 !New discoveries
orNew constrains
No! There are still many things to be understood … for instance
![Page 5: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/5.jpg)
DMNeutrinos Inflation
Baryon asymmetryGravity
Even more the LHC will keep running until 2037 !
Hierarchy problem
Flavour structure
Strong CP problem
In any case clues on:
New discoveries or
New constrains
All the above +
No! There are still many things to be understood … for instance
![Page 6: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/6.jpg)
So far the LHC has not found any new physics yet…Hence, if there is NP around the EW scale it is either:
![Page 7: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/7.jpg)
- Light (but weakly coupled)- Limited by systematics
(large at LHC)
So far the LHC has not found any new physics yet…Hence, if there is NP around the EW scale it is either:
![Page 8: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/8.jpg)
- Heavy (effects suppressed) - Effects can be enhanced at high energy
What does this mean??
- Light (but weakly coupled)- Limited by systematics
(large at LHC)
So far the LHC has not found any new physics yet…Hence, if there is NP around the EW scale it is either:
![Page 9: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/9.jpg)
If new physics is heavy it can be studied with the SM EFT
![Page 10: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/10.jpg)
If new physics is heavy it can be studied with the SM EFT
The BSM cross section can be parametrized as
![Page 11: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/11.jpg)
If new physics is heavy it can be studied with the SM EFT
The BSM cross section can be parametrized as
If the BSM part grows faster with the CM Energy than the SM one
In this case the sensitivity to the BSM coefficients is increased with the CM Energy
![Page 12: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/12.jpg)
If new physics is heavy it can be studied with the SM EFT
(error in %)
The BSM cross section can be parametrized as
If the BSM part grows faster with the CM Energy than the SM one
In this case the sensitivity to the BSM coefficients is increased with the CM Energy
![Page 13: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/13.jpg)
If new physics is heavy it can be studied with the SM EFT
(error in %)
The BSM cross section can be parametrized as
If the BSM part grows faster with the CM Energy than the SM one
Bound becomes stronger at large E
In this case the sensitivity to the BSM coefficients is increased with the CM Energy
![Page 14: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/14.jpg)
Diboson production at the LHC is specially interesting
1) Sensitive to BSM physics addressing the hierarchy problem
for instance: Composite Higgs models, extra dimensions, Little Higgs
1) 2) 3) 4)
In particular, the processes modified by dimension 6 operators, which are:
Why are they interesting?
![Page 15: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/15.jpg)
2) The BSM contributions grow faster than the SM one
+ …
for example:
- In the SM each diagram grows with CM Energy but sum cancelsE 2
t-channel s-channel
Why are they interesting?
![Page 16: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/16.jpg)
+ …
- In the SM each diagram grows with CM Energy but sum cancels
- In the SMEFT vertices are modified, cancellation is spoiled(at dimension 6)
E 2
2) The BSM contributions grow faster than the SM one
t-channel s-channel
for example:
Why are they interesting?
Enhanced sensitivity!
![Page 17: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/17.jpg)
3) Diboson errors are small enough to set strong bounds thanks to E enhancement
1507.03268
Why are they interesting?
![Page 18: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/18.jpg)
Naively we expect a permille bound!!
3) Diboson errors are small enough to set strong bounds thanks to E enhancement
1507.03268
Since the BSM XS grows with E faster than the SM XS
Why are they interesting?
![Page 19: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/19.jpg)
Equivalent to study modifications to Zqq and aTGC
anomalous TGC
Schematically diboson production (WW, WZ):
Z couplings to quarks
![Page 20: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/20.jpg)
Equivalent to study modifications to Zqq and aTGC
anomalous TGC
Schematically diboson production (WW, WZ):
Z couplings to quarks
At dim=6:(Flavour Universality) 4 3 = 7 param+
![Page 21: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/21.jpg)
Schematically diboson production (WW, WZ):
Equivalent to study modifications to Zqq and aTGC
Z couplings to quarks
(LEP-1 @ Z-pole)
anomalous TGC(LEP-2)
![Page 22: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/22.jpg)
Equivalent to study modifications to Zqq and aTGC
SM
SM
SMaTGC
Z couplings to quarks
(LEP-1 @ Z-pole)
anomalous TGC(LEP-2)
Schematically diboson production (WW, WZ):
![Page 23: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/23.jpg)
Summary of our work on diboson:
1.1) Is it justified to neglect Zqq couplings @ LHC?
1.2) Can the LHC improve the bounds on the Zqq w.r.t LEP?
1) 1810.05149 with C. Grojean and M. Riembau
2) 190x.xxxxx with G. Durieux and M. Riembau
2.1) Improving the sensitivity and range with VBF
(ongoing)
3) 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia
3.1) Detailed study of the Wh channel
(ongoing)
![Page 24: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/24.jpg)
Summary of our work on diboson:
1.1) Is it justified to neglect Zqq couplings @ LHC?
1.2) Can the LHC improve the bounds on the Zqq w.r.t LEP?
1) 1810.05149 with C. Grojean and M. Riembau
2) 190x.xxxxx with G. Durieux and M. Riembau
2.1) Improving the sensitivity and range with VBF
(ongoing)
3) 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia
3.1) Detailed study of the Wh channel
(ongoing)
![Page 25: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/25.jpg)
1.1) Is it justified to neglect Zqq couplings @ LHC?
![Page 26: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/26.jpg)
1.1) Is it justified to neglect Zqq couplings @ LHC?
Zqq=0
Fit to anomalouts Triple Gauge Couplings
Combine current leptonic data for WW, WZ from CMS & ATLAS
dg1z
dka
(LHC only)
![Page 27: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/27.jpg)
1.1) Is it justified to neglect Zqq couplings @ LHC?
Zqq=0
+Global fit w/ LEP
Zqq 0
Fit to anomalouts Triple Gauge Couplings
Combine current leptonic data for WW, WZ from CMS & ATLAS
dg1z
dka
(LHC only)
(LHC + LEP-1)
![Page 28: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/28.jpg)
LHC NOW
- Difference between considering Zqq non-zero or zero is of order 20%(+ global fit w/ LEP)
![Page 29: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/29.jpg)
- Difference > 100% @ HL-LHC: Not Justified to Neglect Zqq!
LHC
HL-LHC
NOW
3 ab-1Zqq=0MFVZqq+ LEPZqq 0
![Page 30: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/30.jpg)
At high energies WW, WZ only test 5 directions
but depend on 7 parameters: 4 Zqq couplings and 3 aTGC
LHC bounds
![Page 31: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/31.jpg)
At high energies WW, WZ only test 5 directions
but depend on 7 parameters: 4 Zqq couplings and 3 aTGC
LHC bounds
Zqq=0
![Page 32: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/32.jpg)
At high energies WW, WZ only test 5 directions
but depend on 7 parameters: 4 Zqq couplings and 3 aTGC
LHC bounds
Zqq=0
LEP 1 bounds
+ LEPZqq 0
![Page 33: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/33.jpg)
1.2) Can the LHC improve the bounds on the Zqq w.r.t LEP?
![Page 34: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/34.jpg)
1.2) Can the LHC improve the bounds on the Zqq w.r.t LEP?
ZdR
Combine current leptonic data for WW, WZ from CMS & ATLAS
Z to down type q
Fit to Zqq vertex corrections
ZdL
![Page 35: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/35.jpg)
1.2) Can the LHC improve the bounds on the Zqq w.r.t LEP?
= 0LHC 4 param
LHC 7 param
LHC 5 param
ZdR
Combine current leptonic data for WW, WZ from CMS & ATLAS
Z to down type q
Fit to Zqq vertex corrections
ZdL
![Page 36: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/36.jpg)
- Current data is competitive with LEP setting bounds to Zqq down type q!
1.2) Can the LHC improve the bounds on the Zqq w.r.t LEP?
LEP - MFV
LEP - Flavour Universal
= 0LHC 4 param
LHC 7 param
LHC 5 param
ZdR
Combine current leptonic data for WW, WZ from CMS & ATLAS
Z to down type q
Fit to Zqq vertex corrections
![Page 37: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/37.jpg)
LHC NOWZ to down type q Z to up type q
- For the up type corrections, the LHC is still not competitive with LEP
![Page 38: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/38.jpg)
- WV @ HL-LHC may improve the bounds on all the Zqq vertices w.r.t LEP!
LHC
HL-LHC
NOW
3 ab-1
Z to down type q Z to up type q
Z to up type qZ to down type q
![Page 39: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/39.jpg)
Interpreting the bounds
EFT OKEFT not-OK
weak
strong
LEP
LHC
LHC & LEP
In our case this means that we can only constrain theories where
Our LHC bounds on the BSM parameters are only valid for large BSM masses
![Page 40: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/40.jpg)
In our case this means that we can only constrain theories where
Our LHC bounds on the BSM parameters are only valid for large BSM massesInterpreting the bounds
EFT OKEFT not-OK
weak
strong
LEP
LHC
LHC & LEP
We would like to:
1) Increase the Sensitivity (constrain weakly coupled theories)2) Lower the cutoff (increase range of the bounds)
Increase the Sensitivity
Lower the cutoff
![Page 41: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/41.jpg)
2.1) Improving the sensitivity and range with VBF?
Many work done on diboson to improve the bounds, e.g.
Falkowski et al. (1609.06312 )Azatov et. al (1707.08060)Panico et al. (1708.07823 )Franceschini et al. (1712.01310 )
Bellazzini et al. (1806.09640 )Azatov et. al (1901.04821)Banerjee et. al (1905.02728 )+ …
(ongoing work with G. Durieux and M. Riembau)
![Page 42: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/42.jpg)
Why study VBF?
1) Analytic simplification is possible via Equivalent EW bosons
The process factorises into a: - soft scale (radiated W)- hard scale (2->2 scattering)
Rattazzi et al. 1202.1904
![Page 43: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/43.jpg)
Why study VBF?
1) Analytic simplification is possible via Equivalent EW bosons
The process factorises into a:
2) VBF is sensitive to the same operators as diboson
- soft scale (radiated W)- hard scale (2->2 scattering)
Diboson has the same diagrams as the 2->2 channel rotated 90 degrees
Rattazzi et al. 1202.1904
![Page 44: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/44.jpg)
Why study VBF?
1) Analytic simplification is possible via Equivalent EW bosons
The process factorises into a:
2) VBF is sensitive to the same operators as diboson
- soft scale (radiated W)- hard scale (2->2 scattering)
3) It is possible to completely reconstruct final stateImplement cuts on CM Energy + cuts to increase sensitivity (angular distr)
Diboson has the same diagrams as the 2->2 channel rotated 90 degrees
Rattazzi et al. 1202.1904
![Page 45: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/45.jpg)
First naive attempt: Separating of soft vs hard processes
We can define a jet imbalance variable given by:
BSM
SM EW
QCD
which we checked has a good discriminating power between signal and bkg
![Page 46: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/46.jpg)
Comparing to other works with cuts that increase sensitivity
1712.01310 (WZ with run1 data)
CMS VBF analysis adding CM E cuts only
Wilson coefficient in the Warsaw basis
![Page 47: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/47.jpg)
1712.01310 (WZ with run1 data)
VBF analysis without any extra cuts
VBF using jet imbalance and CM E cuts
CMS VBF analysis adding CM E cuts only
- Simple analysis already very powerful
- Possibility to further improve it with angular distributions, BDT
Wilson coefficient in the Warsaw basis
Increased sensitivity and range to lower scales
Comparing to other works with cuts that increase sensitivity
![Page 48: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/48.jpg)
Conclusions1) CMS and ATLAS aTGC fits will need to include Zqq corrections soon
2) Diboson @ LHC can improve the LEP bounds on the Zqq corrections
- At least under the MFV or FU assumptions
- Need of further study with other channels and more sensitive cuts
3) New possibilities to test diboson operators with VBF
- Would be interesting if CMS and ATLAS would try to do it
- Results hopefully coming soon
![Page 49: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/49.jpg)
Thanks
![Page 50: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/50.jpg)
We studied WW, WZ channels using the same cuts as CMS/ATLAS Possible to improve bounds with other cuts/channels
aTGC @ HL-LHC
WW + WZ(our work)
WZ (new cuts) (Francheschini et al.)
Zh (Banerjee et al.)
WW(our work) WZ
(our work)
- Wh hasn’t been studied in detail yet.- Preliminary results seem competitive (ongoing work)
![Page 51: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/51.jpg)
Cross check with CMS and ATLAS is OK, e.g.
Used MadGraph5_aMC@NLO to get BSM cross section and fit
- Leading order
- No Pythia (we checked didn’t affect much)
- No correlation between bins
We did a simple analysis
Fuks et al- BSMC package
![Page 52: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/52.jpg)
Interpreting the bounds
so they are of the same order as dim 8
In these fits, the quadratic pieces are non-negligible
Need of power counting to ensure:
1) dimension 8 are negligible
2) physical mass larger than Energy events
EFT OKEFT not-OK
weak
strong
LEP
LHC
LHC & LEP
![Page 53: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/53.jpg)
At dimension six 59 operators (Flavour Universality)
![Page 54: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/54.jpg)
![Page 55: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/55.jpg)
1) Drell-Yan
2) Diboson production
Farina et al 1609.08157
Improving LEP bounds on Universal Parameters W, Y
Butter et al 1604.03105
Sensitivity enhancement already used to expand previous LEP bounds
Improving LEP-2 bounds on anomalous Triple Gauge Couplings
Azatov et al 1707.08060
![Page 56: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/56.jpg)
Bounds on Zff anomalous couplins (from LEP)
Flavour Universality MFV
Bounds on aTGCFalkowski et al. 1503.07872
Butter, et al.1604.03105
![Page 57: Exploring the SM EFT with diboson production · 2019. 6. 5. · 190x.xxxxx with G. Durieux and M. Riembau 190x.xxxxx with F. Bishara, P. Englert, C. Grojean, G. Panico, A. Rossia](https://reader033.fdocuments.in/reader033/viewer/2022060810/608ed71d55b0716a33445916/html5/thumbnails/57.jpg)
1) Data used
We chose the most significant leptonic channels