(DM) (SM) (mediator)...Martino Borsato - USC DM signals!3 SM DM SM DM Direct detection Detect...
Transcript of (DM) (SM) (mediator)...Martino Borsato - USC DM signals!3 SM DM SM DM Direct detection Detect...
Dark Matter at
the LHC
Martino Borsato†
†Universida de Santiago de Compostela
on behalf of ATLAS, CMS, LHCb
(SM)(mediator)
(DM)
Martino Borsato - USC
What to look for
๏ Experimental constraints:
• Relic density observed
• (Thermal) DM mass > keV
• Effectively EM neutral
• Cosmologically stable
• No or small self-interaction
!2
Planck, AA 594(2016)A13
e.g. Lovell et al. MNRAS 439(2014)300-317
Stable charged particle and direct detection
"Bullet cluster" AJ 648(2006)L109-L113
or more Slatyer and Wu. PRD95(2017)2,023010
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1000
2000
3000
4000
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6000
DTT
![µK
2]
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-60
-30
0
30
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∆D
TT
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-600
-300
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Planck 2015
Bullet cluster→ Compelling WIMP scenario
Martino Borsato - USC
DM signals
!3
SM
DM
SM
DM
Direct detection
Detect interactions of the DM wind
XENON, Panda, Lux, DarkSide, …
Collider search
• Mediator → DM
(holistic search)
• Mediator → SM
(peak search)
Indirect detection
Signals from DM annihilation
FERMI, PAMELA, AMS, HESS, IceCube, CTA, …
Mediator → DM
!4
Martino Borsato - USC
Mono-X searches at the LHC
๏ Exploit initial state radiation
• Missing energy + large-pT
‣ X = jet, photon, W, Z
๏ Main challenge: measure precisely SM backgrounds
• e.g. Z(νν)+X is irreducible
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SM DM
SM DM
X MET
χ
q
χ
q
q
Z′
χ χZ'
ν
q
χ
q
q
Z′
χ νZ
Martino Borsato - USC
Mono-jet backgrounds
๏ Vector+jet backgrounds
• 50-80% is Z(νν)+jet (irreducible)
๏ Estimate using control regions:
• Z()+jet, removing from event
• W(ν)+jet, removing from event
• γ+jet, removing γ from event
!6
Events
/ G
eV
2−10
1−10
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10
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610
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CMS
monojet
Data
inv.→H(125)
= 2.0 TeVmed
Axial-vector, m
)+jetsννZ(
)+jetsνW(l
WW/WZ/ZZ
Top quark
+jetsγ(ll), γZ/
QCD
Data
/ P
red.
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Tp
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Unc.
(Data
-Pre
d.)
2−
0
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μuon (2)
μuon (1)Jet
nsMET
Remove µµ
arXiv:1712.02345
Martino Borsato - USC
+je
tsγ
Z(ll)+
jets
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+jets MC γZ(ll)+jets /
(13 TeV)-1
35.9 fb
CMS
monojet
[GeV]T
Hadronic recoil p
400 600 800 1000 1200 1400
Data
/ P
red.
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Mono-jet backgrounds
๏ Ratio dσ(Z+jet)/dσ(W+jet)
and dσ(Z+jet)/dσ(γ+jet)
to simplify modelling
• Control-region to signal-region transfer factors from theory
๏ Progress in theory
• pT dependent NLO QCD+EW corrections of LO MC
• Including pT dependent correlations for corrections
• Ratios stable at few %
๏ Validation test on data
• Jet uncertainties cancel out
๏ Simultaneous fits of control
and signal regions
!7
LONLO QCDNNLO QCD
0.06
0.08
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pp →Z(`+`−)+ jet / pp →W(`ν)+ jet @ 13 TeV
Z(`
+`−)+
jet
/W(`
ν)+
jet
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0.95
1.0
1.05
pT,V [GeV]
R/
RN
LO
QC
D
3000
LONLO QCDNNLO QCD
0.01
0.02
0.03
0.04
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0.06
pp →Z(`+`−)+ jet / pp →γ+ jet @ 13 TeV
Z(`
+`−)+
jet
/γ+
jet
100 200 500 1000 30000.9
0.95
1.0
1.05
pT,V [GeV]
R/
RN
LO
QC
D
)+je
tsν
Z(ll)+
jets
/ W
(l
0
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0.22)+jets DataνZ(ll)+jets / W(l
)+jets MCνZ(ll)+jets / W(l
(13 TeV)-1
35.9 fb
CMS
monojet
[GeV]T
Hadronic recoil p
400 600 800 1000 1200 1400
Data
/ P
red.
0.5
1
1.5
arXiv:1712.02345 arXiv:1712.02345
Lindert et al arXiv:1705.04664 Lindert et al arXiv:1705.04664
Martino Borsato - USC
Mono-jet results
๏ Results on simplified DM models
• Vector, axial-vector, scalar, pseudo-
scalar mediator (s-channel)
• 4 parameters: mDM, mmed, gSM, gDM
๏ Reach for gDM=1, mmed = 3 mDM:
• Up to ~1.6-1.8 TeV for mmed (vector)
• Below gSM ~ 0.1 for low mmed < 1TeV
!8
[GeV]VZm
0 1000 2000
[G
eV
]χ
m
0
500
1000exp
σ 2 ±Expected limit
)exp
σ 1 ±Expected limit (
)PDF, scale
theoryσ 1 ±Observed limit (
Relic Density (MadDM)
ATLAS-1
= 13 TeV, 36.1 fbs
Vector Mediator
Dirac Fermion DM
= 1.0χ
= 0.25, gq
g
95% CL limits
χ
= 2
mVZm
SM DM
SM DMmed
arXiv:1712.02345
arXiv:1711.03301
Martino Borsato - USC
Mono-X results
๏ Searched in mono-jet, but also
mono-γ and mono-V
๏ No excess in ATLAS+CMS
(36/fb from 2015+2016)
• Best sensitivity to date
• In the era of precision searches
๏ 40/fb on tape from 2017 and
2018 run happening now
๏ Challenging analysis in future
high-luminosity upgrade
!9
Signature ATLAS CMS
Mono-jet 36/fb 1711.03301 36/fb 1712.02345
Mono-γ 36/fb 1704.03848 13/fb 1706.03794
Mono-V(had) 3.2/fb 1608.02372 36/fb 1712.02345
Mono-Z(lep) 36/fb 1708.09624 36/fb 1711.00431
Mono-H(γγ,ττb,b)36.1/fb 1706.03948,
1707.0130236/fb EXO-16-055
[GeV] medMediator mass M0 500 1000 1500 2000 2500
[G
eV
] D
MD
ark
matter
mass m
0
100
200
300
400
500
600
700
800
900
1000
LHCP 2017 PreliminaryCMS
Axial-vector mediator
Dirac DM = 1.0
DMg
= 0.25q
g
= 0l
gExclusion at 95% CL
Observed
Expected
[EXO-16-048]
)-1 (35.9 fbDM + j/V(qq)
[EXO-16-039]
)-1 (12.9 fbγDM +
[EXO-16-052]
)-1 (35.9 fbDM + Z(ll)
DM = 2 x m
MedM
0.12≥ 2 hcΩ
LHCP 2017 PreliminaryCMS
Axial-vector mediator
Dirac DM = 1.0
DMg
= 0.25q
g
= 0l
g
Martino Borsato - USC
SUSY searches
๏ SUSY provides a candidate for DM
• χ0 down to 100 GeV still allowed
• Many different searches constraining DM candidate
• Interplay with direct searches investigated with global fits
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pMSSM11 EPJC78(2018)3-256
E.Bagnaschi, K.Sakurai, MB, et al
100 101 102 103
mχ0
1[GeV]
10−50
10−48
10−46
10−44
10−42
10−40
10−38
σSI
p[c
m2]
PANDAX-II
XENO
N1T
LUX
XENONnT
XENON1T
LZ
CRESST-II
CDMSlite
CDEX-1
pMSSM11 w/ LHC13 : best fit, 1σ, 2σ, 3σpMSSM11 w/o LHC13 : best fit, 1σ, 2σ, 3σ
µ > 0, Ωχ0
1
= ΩCDM
mAMSB EPJC77(2017)4-268
E.Bagnaschi, MB, K.Sakurai, et al
Martino Borsato - USC
DM from Higgs decays
๏ Powerful search channel if mDM < mH/2
• H(125) only scalar we know, a portal to DM?
๏ Gluon fusion and VH
• Tag with ISR jet or a boson V(hh) or Z()
• Same final state as monoX searches
๏ Vector-boson fusion (VBF)
• Tag using forward jets (large ∆η)
• Low backgrounds (S/B ~ 0.5)
• Most sensitive signature
‣ 13TeV result from CMS BR < 28%(21% exp)
• Z(νν), W(ν) bkgs from control regions
• Shape fit to maximise sensitivity
‣ 8TeV result from ATLAS BR < 28%(31% exp)
• Still competitive, update soon!
!11Combined VBF-tag Z(ll)H-tag V(qq')H-tag ggH-tag
SM
σ inv.)
/→
x B
(H
σ95%
CL u
pper
limit o
n
0
0.2
0.4
0.6
0.8
1
1.2
1.4
Observed
Median expected
68% expected
95% expected
(13 TeV)-1
35.9 fb
CMS Preliminary
Combined limit: 0.24 (0.18)
H(125)
χ
χ
H(125) χ
χ
W/Z∗
H
χ
χ
W/ZggF
VBF
VH
CMS PAS-HIG-17-023ATLAS 1508.07869
CMS PAS-HIG-17-023
Mediator → SM
!12
Martino Borsato - USC
0 500 1000 1500 2000 2500
0.0
0.5
1.0
1.5
2.0
2.5
MZ'B(GeV)
gB
UA2
CDF Run I
CDF 1.1 fb!1
CMS
0.13 fb!1
ATLAS 1 fb!1
CMS
4 fb!1
CMS 5 fb!1
CMS 20 fb!1
ATLAS
13 fb!1
L ∝gB
6Z 0
Bµqγµq
arXiv:1306.2629
Mediator searches
๏ New mediator can decay back to SM
๏ If mmed accessible at LHC could be
key to establish characteristics of
DM interaction
๏ Low sensitivity for light mmed due
to trigger pT thresholds
‣ Recently progress on this front:
1. Boosted dijets (ISR jet tag)
2. Data scouting (trigger-level jets)
!13
SM DM
SM DMmed
SM SM
SM SMmed
Martino Borsato - USCZ' mass (GeV)
50 100 200 300 1000
q'
couplin
g, g
0.02
0.03
0.04
0.1
0.2
0.3
0.4
1CMS
(13 TeV)-135.9 fb
95% CL upper limits
UA2 [13]
CDF Run 1 [18]
CDF Run 2 [19]
[24]-1ATLAS 8 TeV, 20.3 fb
[34]-1CMS 8 TeV, 18.8 fb
[35]-1CMS 13 TeV, 12.9 fb
Z Width (indirect) [71]
ObservedExpected 1 std. deviation±
2 std. deviation±
Mediator searches
Boosted dijets
๏ Require an ISR jet or γ to satisfy trigger threshold
๏ Boosted collimated dijet reconstructed as large-R jet
• Use jet substructure to separate
from single-jet background
๏ Example: CMS JHEP 01(2018)097
• Narrow ISR jet pT > 500 GeV
• Probing m(Z’) down to 50 GeV
• Background from single-jet control regions
(substructure variable uncorrelated from mass)
๏ Example: ATLAS arXiv:1801.08769
• Extending down to m(Z’) = 100 GeV
!14
Events
/ 5
GeV
0
5000
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20000
25000Data 3)×W(qq)+jets (
Total SM pred. 3)×Z(qq)+jets (
Multijet pred. 3)×(qq)+jets (tt/t
=135 GeVZ'
=0.17, mq'
Z'(qq), g
(13 TeV)-1
35.9 fb
CMS
: 500-600 GeVT
p
(GeV)SDm50 100 150
Data
/Pre
dic
tion
0.9
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JHEP 01(2018)097
JHEP 01(2018)097
Martino Borsato - USC
Mediator searches
Data scouting
๏ Reduce trigger rates at “low" mass
• Online jet reconstruction
• Compact event format
๏ Example: ATLAS arXiv:1804.03496
• Construct jets in HLT from Calorimeter
• Only jets pi and quality to disk (0.5%)
• ET > 100 GeV (29/fb), ET > 75 GeV (3.6/fb)
• Searching down to m(Z’) = 450 GeV
๏ Example: CMS PAS-EXO-16-056
• Calorimeter scouting m > 0.5 TeV:
• Particle-Flow scouting m > 1.25 TeV:
!15 [GeV]Z’
m
400 600 800 1000 1200 1400 1600 1800 2000
qg
0.02
0.04
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|y*| < 0.3 |y*| < 0.6
1− 3.6 fb 1− 29.3 fb
ATLAS
= 13 TeVs
95% CL upper limits
TLA Observed
)σ 1-2±TLA Expected (
Dijet Observed
Eve
nts
/ B
in
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02
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nific
an
ce
ATLAS
, |y*| < 0.3-1Data, 3.6 fbBackground fitBumpHunter interval
x 500σZ’, = 0.1
q = 550 GeV, gZ’m
, |y*| < 0.6-1Data, 29.3 fbBackground fitBumpHunter interval
x 500σZ’, = 0.1
q = 750 GeV, gZ’m
-value = 0.6pBH
-value = 0.42p 2χ
-value = 0.44pBH
-value = 0.13p 2χ
arXiv:1804.03496
arXiv:1804.03496
Martino Borsato - USC.....
.....
.....
......
.....
.....
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.....
......
.....
.....
.....
......
.....
......
.....
.....
.
50 100 200 300 1000 2000
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1−10
1
qg
'
5% = Z'M / Z'Γ
10% = Z'M / Z'Γ
30% = Z'M / Z'Γ
50% = Z'M / Z'Γ
100% = Z'M / Z'Γ
qq→Z'
95% CL exclusions
~100% < Z'M / Z'Γ[ATLAS-EXOT-2017-01]
ATLAS Boosted Dijet, 13 TeV
[EXO-16-046]
, 13 TeVχCMS Dijet
[ATLAS-EXOT-2016-21]
ATLAS Dijet, 13 TeV
~10% < Z'M / Z'Γ[ATLAS-CONF-2016-030]
ATLAS TLA, 13 TeV
[EXO-16-056]
CMS Dijet, 13 TeV
[ATLAS-CONF-2016-070]
, 13 TeVγATLAS Dijet+ISR
[EXO-14-005]
CMS Dijet, 8 TeV
[ATLAS-CONF-2016-070]
ATLAS Dijet+ISR j, 13 TeV
[EXO-16-057]
CMS Dijet b tagged, 8 TeV[Nucl. Phys. B 400, 3 (1993)]UA2
[EXO-17-001]
CMS Boosted Dijet, 13 TeV[Phys. Rev. D 55, 5263 (1997)]CDF Run1
[Phys. Rev. D 79, 112002 (2009)]CDF Run2
[arXiv:1404.3947]
)Z'
/MZ'
ΓZ width (all
CMS Preliminary
Limits on the universal coupling between a leptophobic boson and quarks [EXO- 6- ] from various dijet analyses from CMS,ATLAS, CDF, and UA . The limits are shown in solid lines, with the excluded area above the lines. The grey dashed lines show thevalues at fixed values of . Most of the analyses, with the exception of Dijet , assume that the intrinsic width is negligiblecompared to the experimental resolution and hence are valid for . The Dijet analysis is valid for
. Also shown is an indirect constraint on from the boson width, which is valid for all values of .
|
boosted dijet
b-tagged
8 TeV
Dijet X
Dijet
Dijet ATLAS
Dijet 8 TeV
boosted dijet
(ATLAS)
UA2
Summary of dijet searches
•Searched also Z’→
‣CMS PAS-EXO-16-031
‣ATLAS arXiv:1707.02424
!16
[PRL 117,031802(2016)]
[JHEP 1801(2018)097]
[arXiv:1802.06149]
[arXiv:1803.08030]
CMS TLA jets
ATLAS
ATLAS TLA, 13 TeV
[arXiv:1804.03496]
Martino Borsato - USC
Mediator Mass [TeV]
0 0.5 1 1.5 2 2.5 3
DM
Mass [T
eV
]
0.2
0.4
0.6
0.8
1
1.2DM Simplified Model Exclusions Preliminary July 2017ATLAS
= 1DM
= 0, gl
= 0.25, gq
gAxial-vector mediator, Dirac DM
All limits at 95% CL
Pert
urb
ativ
e U
nita
rity
Dije
t
arXiv:1703.09127 [hep-ex]
-1 = 13 TeV, 37.0 fbs
Dijet
Dije
t 8 T
eV
Phys. Rev. D. 91 052007 (2015)
-1 = 8 TeV, 20.3 fbs
Dijet 8 TeVD
ijet T
LA
ATLAS-CONF-2016-030
-1 = 13 TeV, 3.4 fbs
Dijet TLA
Dije
t +
IS
R
ATLAS-CONF-2016-070
-1 = 13 TeV, 15.5 fbs
Dijet + ISR
γ+missTE
Eur. Phys. J. C 77 (2017) 393
-1 = 13 TeV, 36.1 fbs
γ+missTE
+jetmissTE
ATLAS-CONF-2017-060
-1 = 13 TeV, 36.1 fbs
+jetmissTE
+ZmissTE
ATLAS-CONF-2017-040
-1 = 13 TeV, 36.1 fbs
+ZmissTE
DM
Mas
s =
Med
iato
r Mas
s
×2
= 0
.12
2hcΩ
Therm
al R
elic
Mono-X vs mediator searches
!17
gq = 0.25, g = 0 arXiv:1708.09674
Martino Borsato - USC
Mono-X vs mediator searches
!18
gq = 0.1, g = 0.01
Francesco Lo Sterzo Mediator Mass [TeV]
0 0.5 1 1.5 2 2.5 3
DM
Ma
ss [
Te
V]
0.2
0.4
0.6
0.8
1
1.2DM Simplified Model Exclusions Preliminary July 2017ATLAS
= 1DM
= 0.01, gl
= 0.1, gq
gVector mediator, Dirac DM
All limits at 95% CL
Dije
tDijet
Phys. Rev. D. 91 052007 (2015)
-1 = 8 TeV, 20.3 fbsDijet 8 TeV
arXiv:1703.09127 [hep-ex]
-1 = 13 TeV, 37.0 fbsDijet
ATLAS-CONF-2016-030
-1 = 13 TeV, 3.4 fbsDijet TLA
ATLAS-CONF-2016-070
-1 = 13 TeV, 15.5 fbsDijet + ISR
+XmissTE
+XmissTE
Eur. Phys. J. C 77 (2017) 393
-1 = 13 TeV, 36.1 fbs γ+
miss
TE
ATLAS-CONF-2017-060
-1 = 13 TeV, 36.1 fbs+jet
miss
TE
Dile
pto
n
CERN-EP-2017-119
-1 = 13 TeV, 36.1 fbs
Dilepton
DM
Mas
s =
Med
iato
r Mas
s
×2
= 0
.12
2hcΩ
Therm
al R
elic
arXiv:1708.09674
Lighter mediators → SM
!19
Martino Borsato - USC
a
γ
γ
Dark Sectors at the LHC
๏ Address SM problems with light very-
weakly interacting states → Dark Sectors
‣ Can get also DM candidate (e.g. freeze-in)
๏ Dark sector portals:
• Scalar portal (φ)
• Vector portal (A’)
• Neutrino portal (N)
• Axion portal (a)
๏ Search at (low-energy) intensity frontier
• LHC can exploit huge cross-sections
• Main challenge: triggering
!20
portals
Recent review: 1608.08632
φ
h f
f
f
fA0
γ/Z
N ναsin θαN ν
Martino Borsato - USC
The LHCb potential
๏ Designed to exploit the LHC
intensity frontier to do B physics
๏ Only LHC detector fully
instrumented in forward region
๏ ~10x lower luminosity (low pile-up)
๏ Excellent vertex and mass resolution
๏ Capable of very soft triggers:
• At hardware level (L0):
‣Muons with pT > 1.8 GeV
‣Calo deposits with ET > 3 GeV
• At Software level (HLT):
‣Triggers on detached vertices
!21
Int.J.Mod.Phys. A 30, 1530022 (2015)
LHCb
MS
Cherenkov
drift tube
pixel silicon strip ECAL
HCAL muon
CMS
LHCb 2<η<5
๏ “Trigger-less” upgrade (2021)• Read-out detector in real time• Can trigger on detached vertices,
precise particle ID and more
TDR: [LHCB-TDR-016]
Martino Borsato - USC
๏ Look for new hidden-sector bosons
in b→s penguin transitions
๏ World record samples of B→K(*)µµ
• search for narrow µµ peak
๏ Allow detached µµ (within VELO)
• small SM mixing can give lifetime
๏ Constrain on light scalars
• mixing with SM Higgs
• world-best limits below 2mτ
• Complementary to Ship
!22
Dark Bosons from b→sPhys Rev Lett 115 161802 (2015)
Phys Rev D 95, 071101(R) (2017)
b
d
Vtb Vts
s
d
µ−
µ+
t
W+
χ
0 K
d/u d/u
B0(+)
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K∗(+)
<latexit sha1_base64="MKdkWGTkK1kC+oeEee1cXeXP934=">AAAB8XicbZDLSsNAFIZP6q3WW9Wlm2ARKkJJRFBXFtwIbioYW0hjmUwn7dDJhZkToYQ+hou60OLWJ/A13Pk2Ti8Lbf1h4OP/z2HOOX4iuELL+jZyS8srq2v59cLG5tb2TnF370HFqaTMobGIZcMnigkeMQc5CtZIJCOhL1jd712P8/oTk4rH0T32E+aFpBPxgFOC2nJvH7MmUVg+OR60iiWrYk1kLoI9g9LV53A4AoBaq/jVbMc0DVmEVBClXNtK0MuIRE4FGxSaqWIJoT3SYa7GiIRMedlk5IF5pJ22GcRSvwjNifu7IyOhUv3Q15Uhwa6az8bmf5mbYnDhZTxKUmQRnX4UpMLE2Bzvb7a5ZBRFXwOhkutZTdolklDUVyroI9jzKy+Cc1q5rNh3Vql6BlPl4QAOoQw2nEMVbqAGDlCI4Rle4c1A48UYGe/T0pwx69mHPzI+fgCNzpM1</latexit><latexit sha1_base64="W9PAAnX3ohJW/9H3t8deChSzF78=">AAAB8XicbZDNSsNAFIUn/tb6V3XpZrAIFaEkIqgrC24ENxWMLaSxTKaTduhkEmZuhBL6GC7sQsWtT+BruPNtnLRdaOuBgY9z7mXuvUEiuAbb/rYWFpeWV1YLa8X1jc2t7dLO7r2OU0WZS2MRq2ZANBNcMhc4CNZMFCNRIFgj6F/leeORKc1jeQeDhPkR6UoeckrAWN7NQ9YiGirHR8N2qWxX7bHwPDhTKF9+Puca1dulr1YnpmnEJFBBtPYcOwE/Iwo4FWxYbKWaJYT2SZd5BiWJmPaz8chDfGicDg5jZZ4EPHZ/d2Qk0noQBaYyItDTs1lu/pd5KYTnfsZlkgKTdPJRmAoMMc73xx2uGAUxMECo4mZWTHtEEQrmSkVzBGd25XlwT6oXVefWLtdO0UQFtI8OUAU56AzV0DWqIxdRFKMn9IJeLbBG1pv1PildsKY9e+iPrI8f6UaU+g==</latexit><latexit sha1_base64="W9PAAnX3ohJW/9H3t8deChSzF78=">AAAB8XicbZDNSsNAFIUn/tb6V3XpZrAIFaEkIqgrC24ENxWMLaSxTKaTduhkEmZuhBL6GC7sQsWtT+BruPNtnLRdaOuBgY9z7mXuvUEiuAbb/rYWFpeWV1YLa8X1jc2t7dLO7r2OU0WZS2MRq2ZANBNcMhc4CNZMFCNRIFgj6F/leeORKc1jeQeDhPkR6UoeckrAWN7NQ9YiGirHR8N2qWxX7bHwPDhTKF9+Puca1dulr1YnpmnEJFBBtPYcOwE/Iwo4FWxYbKWaJYT2SZd5BiWJmPaz8chDfGicDg5jZZ4EPHZ/d2Qk0noQBaYyItDTs1lu/pd5KYTnfsZlkgKTdPJRmAoMMc73xx2uGAUxMECo4mZWTHtEEQrmSkVzBGd25XlwT6oXVefWLtdO0UQFtI8OUAU56AzV0DWqIxdRFKMn9IJeLbBG1pv1PildsKY9e+iPrI8f6UaU+g==</latexit><latexit sha1_base64="ezGy9HAVxpiq5MtlN30VZ5WNhic=">AAAB8XicbVBNS8NAEN34WetX1aOXxSJUhJKIoN4KXgQvFYwtpLFstpt26WY37E6EEvozvHhQ8eq/8ea/cdvmoK0PBh7vzTAzL0oFN+C6387S8srq2nppo7y5tb2zW9nbfzAq05T5VAml2xExTHDJfOAgWDvVjCSRYK1oeD3xW09MG67kPYxSFiakL3nMKQErBbePeYcYqJ2ejLuVqlt3p8CLxCtIFRVoditfnZ6iWcIkUEGMCTw3hTAnGjgVbFzuZIalhA5JnwWWSpIwE+bTk8f42Co9HCttSwKeqr8ncpIYM0oi25kQGJh5byL+5wUZxJdhzmWaAZN0tijOBAaFJ//jHteMghhZQqjm9lZMB0QTCjalsg3Bm395kfhn9au6d+dWG+dFGiV0iI5QDXnoAjXQDWoiH1Gk0DN6RW8OOC/Ou/Mxa11yipkD9AfO5w/L+pBr</latexit>
0.5 1.0 2.0 4.0
mϕ (GeV)
10−12
10−10
10−8
10−6
sin2θ
CODEX-bSHiP
MATHUSLA
CHARM
LHCb, 3 fb−1
LHCb, 300 fb−1
Plot from arXiv:1708.09395
B.Batell, M.Pospelov, A.Ritz, PRD 83, 054005 (2011)F.Bezrukov, D.Gorbunov, JHEP05(2010)010, JHEP07(2013)140
as τ ∝ 1=θ2.from Ref. [2].
as BðBþ→ K
þχÞ ∝ θ2,
fraction into muons is directly
Martino Borsato - USC
310
410
510
210
310
410
510
610
710
m(µµ) [MeV ]
Can
didates/σ[m
(µµ)]/2
LHCb√
s = 13TeVµ+µ−
µ±µ±
prompt-like sample
pT(µ) > 1GeV, p(µ) > 20GeV
Dark Photons at LHCb
!23
๏ Can search for Dark Photons (A') in µµ
‣ Can be very light, produced as γ*
‣ Large fraction in forward region, very soft pT
๏ Data scouting technique in LHCb Run 2:
‣ Online reconstruction and tight µ-ID
‣ Only interesting part of the event to disk → no pre-scale down to threshold 2 mµ
γ*/A'
γ*/A'
PRL 120 (2018) no.6, 061801
Prompt-like dimuon
sample with no pre-scale
down to threshold!
Martino Borsato - USC !24
2−10
1−10 1 10
12−10
11−10
10−10
9−10
8−10
7−10
6−10
5−10
4−10
m(A0) [ GeV ]
ε2
LHCb
LHCb
Previous Experiments
90% CL exclusion regions on [m(A0), ε2]
PRL 120 (2018) no.6, 061801
Dark Photons at LHCb
Already competitive below 1 GeV
LHCb
Previous Experiments
First limits above 10 GeV
Martino Borsato - USC
Dark Photons at LHCb
๏ Proof of concept for soft µ searches at LHCb
• Multiple dimuons from dark cascade
• Heavy neutral leptons in displaced πµ
!25
2−10
1−10 1 10
12−10
11−10
10−10
9−10
8−10
7−10
6−10
5−10
4−10
m(A0) [ GeV ]
ε2
LHCb
LHCb
Previous Experiments
90% CL exclusion regions on [m(A0), ε2]
First limits above 10 GeV
PRL 120 (2018) no.6, 061801
Already competitive below 1 GeV
First non-beam-dump long lived A’ sensitivity LHCb
Previous Experiments
Other analysis filled the gap
A.Pierce et al. arXiv:1708.05389
Can recast to light scalar searches
Haisch et al. 1802.021566 8 10 12 14
m(φ) [GeV]
0
5
10
15
20
σ(gg→
φ)×B(
φ→
µµ)[pb]
Υ(1S)
Υ(2S)
Υ(3S)
LHCb√s = 8TeV
95% CL upper limits
Median expected
68% expected
95% expected
Observed
CMS expected
CMS observed
Today on the arXiv! 1805.09820
Martino Borsato - USC
LHCb Upgrade Dark Photon Reach
!26
-
/ /
/
-
-
/ /
-
-
-
-
-
-
-
-
[ ]
≡
α
w-mass BSM searches, including dark photons (predictions assume 15/fb).
Inclusive A’ →μμ @ LHCb
Ilten, Soreq, Thaler, MW, Xue
[1603.08926]
Radiative Charm Decays @ LHCb
Ilten, Thaler, MW, Xue
[1509.06765]
See talk by W.Xue
on Tu evening
Inclusive A’→µµ at LHCbIlten, Soreq, Thaler, Williams, Xue [1603.08926]
Radiative D Decays at LHCbIlten, Thaler, Williams, Xue [1509.06765]
10
10
ε2
10
m(A0) [ GeV ]
Run 3 reach for dark photons
๏Using D*0 → D0A’(ee)
๏With upgraded trigger
expect 300⨉109 D*0 → D0γ
per fb-1 (15/fb in Run 3)
Martino Borsato - USC
Conclusions
๏ Investigating the origin of Dark Matter is one of the main goals of the LHC program
๏ Different and often complementary searches:
• Mediator → DM (holistic)
‣ Mono-X searches
‣ Higgs to invisible searches
• Mediator → SM (peak search)
‣ Searching structure in dijet (dilepton) spectrum
‣ Data scouting and boosted jets to reach lower masses
• Lighter mediators → SM (dark sectors)
‣ LHCb recently demonstrated to be very sensitive
!27
BACKUP
!28
Martino Borsato - USC
Theory uncertainties for mono-X
!29
Uncertainty source Process (magnitude) Correlation
Fact. & renorm. scales (QCD)Z → νν/W → `ν (0.1 – 0.5%)Z → νν/γ+jets (0.2 – 0.5%)
Correlated between processes;and in pT
pT shape dependence (QCD)Z → νν/W → `ν (0.4 – 0.1%)Z → νν/γ+jets (0.1 – 0.2%)
Correlated between processes;and in pT
Process dependence (QCD)Z → νν/W → `ν (0.4 – 1.5%)Z → νν/γ+jets (1.5 – 3.0%)
Correlated between processes;and in pT
Effects of unknown Sudakov logs (EW)Z → νν/W → `ν (0 – 0.5%)Z → νν/γ+jets (0.1 – 1.5%)
Correlated between processes;and in pT
Missing NNLO effects (EW)Z → νν (0.2 – 3.0%)W → `ν (0.4 – 4.5%)γ+jets (0.1 – 1.0%)
Uncorrelated between processes;correlated in pT
Effects of NLL Sudakov approx. (EW)Z → νν (0.2 – 4.0%)W → `ν (0 – 1.0%)γ+jets (0.1 – 3.0%)
Uncorrelated between processes;correlated in pT
Unfactorized mixed QCD-EW correctionsZ → νν/W → `ν (0.15 – 0.3%)Z → νν/γ+jets (<0.1%)
Correlated between processes;and in pT
PDFZ → νν/W → `ν (0 – 0.3%)Z → νν/γ+jets (0 – 0.6%)
Correlated between processes;and in pT
CMS mono-X arXiv:1712.02345
Martino Borsato - USC
HNL in B→π+µ−µ−
๏ Lepton number violating B−→π+µ−µ− can
proceed via on-shell Majorana neutrinos
๏ Look for B mass peak, then extract limit
as a function of mN
๏ Limit set on N(πµ) lifetimes up to 1000 ps
๏ Constraints on mixing angle Vµ4
• Recently revisited
๏ Also searched in charm D+→π−µ+µ+
!30
Neutrino mass [MeV]
1000 2000 3000 4000 5000
Upper
lim
it
-910
-810
-710
-610 1 ps
10 ps
100 ps
200 ps
500 ps
1000 ps
LHCb
W
+
+
u N
W
b
B
Can be displaced
Phys Rev Lett 112 131802 (2014)
B Shuve, ME Peskin, PRD94 (2016) no.11, 113007
PLB 724 (2013) 203-212B → ×
B(D+→ π−µ+µ+) < 2.2 (2.5)× 10−8,
B(D+s→ π−µ+µ+) < 1.2 (1.4)× 10−7.
Martino Borsato - USC
Future HNL at LHCb
๏ Inclusive search
๏ Can also search higher masses using
on-shell W−→jet µ−µ−
!31
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π−
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PV (SV) TV
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µ+
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SVjet
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W+
<latexit sha1_base64="khczDvfVNWcrZYn/Bf6NagnUTCg=">AAAB6XicdZDLSsNAFIZP6q3WW9Wlm8EiCEJI2kLryoIbl/USW2hjmUwn7dDJhZmJUEIfwY0LFbe+hCsfwp1v47SpoKI/DHz8/znMOceLOZPKsj6M3MLi0vJKfrWwtr6xuVXc3rmWUSIIdUjEI9H2sKSchdRRTHHajgXFgcdpyxudTvPWLRWSReGVGsfUDfAgZD4jWGnrsnVz1CuWLLNcLdcrVZRBuTaHio1s05qpdPL2egFazV7xvduPSBLQUBGOpezYVqzcFAvFCKeTQjeRNMZkhAe0ozHEAZVuOht1gg6000d+JPQLFZq53ztSHEg5DjxdGWA1lL+zqflX1kmUX3dTFsaJoiHJPvITjlSEpnujPhOUKD7WgIlgelZEhlhgovR1CvoIX5ui/8Epm8emfW6VGnXIlIc92IdDsKEGDTiDJjhAYAB38ACPBjfujSfjOSvNGfOeXfgh4+UTVy2PiQ==</latexit><latexit sha1_base64="fCUL13KFWtJ44Ve5Lc9se2669nI=">AAAB6XicdZDNSsNAFIUn9a/Wv6pLQQaLIAghSQutKwtuXLZobKGNZTKdtEMnkzAzEUrp0qUbFypufYmufAh3PoMv4bSpoKIHBj7OuZe59/oxo1JZ1ruRWVhcWl7JrubW1jc2t/LbO1cySgQmLo5YJJo+koRRTlxFFSPNWBAU+ow0/MHZNG/cECFpxC/VMCZeiHqcBhQjpa2LxvVxJ1+wTKfkVIolmIJTnkPRhrZpzVQ4fZ3UP273J7VO/q3djXASEq4wQ1K2bCtW3ggJRTEj41w7kSRGeIB6pKWRo5BIbzQbdQwPtdOFQST04wrO3O8dIxRKOQx9XRki1Ze/s6n5V9ZKVFDxRpTHiSIcpx8FCYMqgtO9YZcKghUbakBYUD0rxH0kEFb6Ojl9hK9N4f/gOuaJadetQrUCUmXBHjgAR8AGZVAF56AGXIBBD9yBB/BoMOPeeDKe09KMMe/ZBT9kvHwCXuORzg==</latexit><latexit sha1_base64="fCUL13KFWtJ44Ve5Lc9se2669nI=">AAAB6XicdZDNSsNAFIUn9a/Wv6pLQQaLIAghSQutKwtuXLZobKGNZTKdtEMnkzAzEUrp0qUbFypufYmufAh3PoMv4bSpoKIHBj7OuZe59/oxo1JZ1ruRWVhcWl7JrubW1jc2t/LbO1cySgQmLo5YJJo+koRRTlxFFSPNWBAU+ow0/MHZNG/cECFpxC/VMCZeiHqcBhQjpa2LxvVxJ1+wTKfkVIolmIJTnkPRhrZpzVQ4fZ3UP273J7VO/q3djXASEq4wQ1K2bCtW3ggJRTEj41w7kSRGeIB6pKWRo5BIbzQbdQwPtdOFQST04wrO3O8dIxRKOQx9XRki1Ze/s6n5V9ZKVFDxRpTHiSIcpx8FCYMqgtO9YZcKghUbakBYUD0rxH0kEFb6Ojl9hK9N4f/gOuaJadetQrUCUmXBHjgAR8AGZVAF56AGXIBBD9yBB/BoMOPeeDKe09KMMe/ZBT9kvHwCXuORzg==</latexit><latexit sha1_base64="fpbWSJIMcQ28FtNOPZUs1HQsS+0=">AAAB6XicdVBNS8NAEJ3Ur1q/qh69LBZBEEKSFlpvBS8eKxpbaGPZbDft0s0m7G6EUvoTvHhQ8eo/8ua/cdtGUNEHA4/3ZpiZF6acKe04H1ZhZXVtfaO4Wdra3tndK+8f3Kokk4T6JOGJ7IRYUc4E9TXTnHZSSXEcctoOxxdzv31PpWKJuNGTlAYxHgoWMYK1ka7bd2f9csWxvZrXqNbQknj1nFRd5NrOAhXI0eqX33uDhGQxFZpwrFTXdVIdTLHUjHA6K/UyRVNMxnhIu4YKHFMVTBenztCJUQYoSqQpodFC/T4xxbFSkzg0nTHWI/Xbm4t/ed1MR41gykSaaSrIclGUcaQTNP8bDZikRPOJIZhIZm5FZIQlJtqkUzIhfH2K/ie+Z5/b7pVTaTbyNIpwBMdwCi7UoQmX0AIfCAzhAZ7g2eLWo/VivS5bC1Y+cwg/YL19ApqnjYI=</latexit>
b → Xµ+µ+π−
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0.1 1 10 10010-12
10-10
10-8
10-6
10-4
0.01
1
MN HGeVL
VmN
2
BBN Seesaw
KÆmn
E949
NuTeV
DELPHI
L3
CMS
ATLAS
LHC14
SHiPFCC-ee
CHARM
FMMF
EWPD
PS191
BEBC
NA3
KÆmmp
LHCb
Belle
LBNE
arXiv:1502.06541
B(b → Xµ+ν)
B(B+ → µ+ν)> 105
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u/c
W−
N
µ− µ−
π+
W−
W+
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