SUSY SEARCHES AT THE TEVATRON Xavier Portell On

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SUSY SEARCHES AT THE TEVATRON Xavier Portell (On behalf of CDF and D 0

SUSY SEARCHES AT THE TEVATRON Xavier Portell (On behalf of CDF and D 0 Collaborations) HCP (Duke, NC) May 2006 SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 1

THE TEVATRON p-pbar collider: Chicago 36 x 36 bunches at 396 ns crossing time

THE TEVATRON p-pbar collider: Chicago 36 x 36 bunches at 396 ns crossing time s = 1. 96 Te. V (Run I 1. 8 Te. V ) Booster CDF Tevatron, CDF and D 0 were highly upgraded in Run II. Great performance: 1. 6 fb-1 delivered DØ Tevatron p source Main Injector 1. 3 fb-1 to tape Data collecting efficiencies ~ 85% SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 2

WHY DO WE NEED SUSY? Q|Boson> = Fermion The SM works very well. .

WHY DO WE NEED SUSY? Q|Boson> = Fermion The SM works very well. . . but there exist some unresolved problems: SUSY: • Mass hierarchy problem The introduction of SUSY have very interesting implications: • Unification Q|Fermion> = Boson ü Solves the hierarchy problem • Dark Matter • Matter-antimatter asymmetry ü Unification of forces at GUT scale ü Provides a Dark Matter candidate ü. . . But SUSY also imply new undiscovered particles. . . SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 3

SUSY BREAKING Symmetry Need to be broken determines phenomenology One of the preferred models:

SUSY BREAKING Symmetry Need to be broken determines phenomenology One of the preferred models: m. SUGRA Ø New superfields in the “hidden” sector Ø Interact gravitationally with MSSM Ø Soft SUSY breaking Ø Only 5 parameters at SUSY scale m 0: common scalar mass at GUT m 1/2: the common gaugino mass at GUT tan : Ratio of Higgs vaccum expectation values A 0: Trilinear coupling Sign( ): Higgs mass term SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 4

R-PARITY Most general SUSY lagrangian Leptonic and Baryonic number violation in the superpotential •

R-PARITY Most general SUSY lagrangian Leptonic and Baryonic number violation in the superpotential • l and l’ violate leptonic number and l’’ the baryonic number • ijk denote the families involved New quantum number: Rp=(-1)3(B-L)+2 s ~ 01 e ~ l 121 e 1 2 1 SM particles: Rp=1 Superpartners: Rp=-1 When Rp is conserved: Ø Superpartners are pair produced Ø Lightest SUSY Particle (LSP) SUSY Searches at Tevatron; HCP, Duke, May 2006 Dark Matter candidate! Xavier Portell, 5

Cross Section (pb) T. Plehn, PROSPINO Cross Section (pb) Tevatron: 1. 96 Te. V

Cross Section (pb) T. Plehn, PROSPINO Cross Section (pb) Tevatron: 1. 96 Te. V LHC: 14 Te. V WHY AT THE TEVATRON? increase by 3 -4 orders of magnitude w. r. t. Tevatron. comparable to Tevatron (and with more background). Good prospects for finding SUSY at the Tevatron! 100 events per fb-1 SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 6

OUTLINE R P C SQUARKS AND GLUINOS CHARGINOS AND NEUTRALINOS MET+jets 3 -leptons GMSB

OUTLINE R P C SQUARKS AND GLUINOS CHARGINOS AND NEUTRALINOS MET+jets 3 -leptons GMSB CHARGINO/NEUTRALINO gg + MET R P V CHARGINO/ NEUTRALINO STOP b-jets and taus INDIRECT 4 -leptons INDIRECT SEARCHES: BS SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 7

OUTLINE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 8

OUTLINE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 8

SQUARKS AND GLUINOS DIRECT SQUARK-GLUINO PRODUCTION: DECAY: Strong interaction: large production expected Missing ET

SQUARKS AND GLUINOS DIRECT SQUARK-GLUINO PRODUCTION: DECAY: Strong interaction: large production expected Missing ET Multiple jets Missing ET (MET) + jets Missing ET Studied an m. SUGRA scenario with first 4 flavors degenerate (sbottom/stop not considered) - Always 3 or more jets Optimized for three cases: - Optimization for three different ranges of gluino masses. 2 -jets (when Mgl>Msq) 3 -jets (when Mgl~Msq) 4 -jets (when Mgl<Msq) Backgrounds are challenging (specially QCD) SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 9

SQUARKS AND GLUINOS Distributions after all cuts for CDF and D 0 agree with

SQUARKS AND GLUINOS Distributions after all cuts for CDF and D 0 agree with data in all cases. 4 -jet optimization Mgl~240 Ge. V/c 2 Mgl~507 Ge. V/c 2 3 -jet optimization CDF background contributions after all the cuts. Mgl~Msq~330 Ge. V/c 2 SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 10

SQUARKS AND GLUINOS: LIMITS D 0: 310 pb-1, A 0=0, <0 and tan =3

SQUARKS AND GLUINOS: LIMITS D 0: 310 pb-1, A 0=0, <0 and tan =3 CDF: 371 pb-1, A 0=0, <0 and tan =5 CDF: Includes theoretical uncertainties when calculating the observed limit D 0: Reduce theoretical cross section by 1 s (more conservative) Mgl > 387 Ge. V/c 2 (when Mgl~Msq) Mgl > 241 Ge. V/c 2 ; Msq > 325 Ge. V/c 2 SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 11

3 rd GENERATION SQUARKS SUSY: Predicts left- and right-handed scalar partner eigenstates for each

3 rd GENERATION SQUARKS SUSY: Predicts left- and right-handed scalar partner eigenstates for each SM fermion As 3 rd generation is heavier, stop and sbottom could be the lightest SUSY particles. Important to have specific analyses for them! SBOTTOM Signatures of 2 or 4 b-jets and MET STOP Depending on the mass: Ø Heavy: A Light stop is preferred (consistent with baryogenesis) Balazs, Carena, Wagner (hep-ph/0403224) Ø Medium: Ø Light: Soft jets (experimental challenge) SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 12

SBOTTOM SELECTION CRITERIA RESULTS ü At least two jets, one b-tagged. ü Good agreement

SBOTTOM SELECTION CRITERIA RESULTS ü At least two jets, one b-tagged. ü Good agreement data/MC ü Three different jet/MET thresholds (increasing sbottom mass): ü Exclude sbottom masses up to 200 Ge. V (depending on neutralino mass) ET 1 st > 40 -70 Ge. V ET 2 nd > 15 -40 Ge. V MET > 60 -100 Ge. V ET 1 st > 40 Ge. V ET 2 nd > 15 Ge. V MET > 60 Ge. V (m , m ) = (140, 80) Ge. V/c 2 SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 13

STOP ü D 0: 2 different analyses to improve sensitivity: e , ü e

STOP ü D 0: 2 different analyses to improve sensitivity: e , ü e analysis: optimized for different Dm= (Mstop – Msneutrino) values ü Missing ET > 15 Ge. V ü Topological cuts The sneutrino usually decays into neutrino and neutralino (MET) Optimization Background Data e (Dm low) 23. 0 3. 1 21 e (Dm high) 40. 7 4. 4 42 2. 9 0. 4 1 Numbers compatible with SM Great improvement with respect to Run I (excluding up to the top mass) SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 14

OUTLINE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 15

OUTLINE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 15

CHARGINOS AND NEUTRALINOS PRODUCTION Mix to form the mass states Always one lepton from

CHARGINOS AND NEUTRALINOS PRODUCTION Mix to form the mass states Always one lepton from + Missing ET Always two leptons from In m. SUGRA: M ~M ~2 M We have always 2 like-sign leptons (one from each superpartner) Clean signature and relatively high cross sections GOLDEN CHANNEL SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 16

CHARGINOS AND NEUTRALINOS The third lepton tends to be very soft tan determines the

CHARGINOS AND NEUTRALINOS The third lepton tends to be very soft tan determines the lepton flavor composition Cuts in lepton PT: PT 1 st~20 Ge. V/c PT 2 nd~10 Ge. V/c taus dominate IMPORTANT ANALYSES VARIETY - 3 leptons (ee+l, e / e+l) Low p. T zone - 2 leptons + track - 2 like-sign (LS) leptons (ee, , e ) Different trigger paths and cut optimizations for e/ and tracks in general SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 17

CHARGINOS AND NEUTRALINOS Ø Minimum p. T for the 2 leading leptons Requirements to

CHARGINOS AND NEUTRALINOS Ø Minimum p. T for the 2 leading leptons Requirements to reduce SM background Ø Dilepton mass and angle cuts (avoid Z and Drell-Yan) Ø Small jet activity (DY, diboson, conversions. . . ) Ø Missing transverse energy significant Observed/Expected Events All is compatible with SM. . . D 0 t+t et+t CDF SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 18

CHARGINOS AND NEUTRALINOS Low tan and slepton mass degenerate Low tan and no slepton

CHARGINOS AND NEUTRALINOS Low tan and slepton mass degenerate Low tan and no slepton mixing Different luminosities, different number of analyses and slightly different scenarios M > 117 Ge. V/c 2 M > 127 Ge. V/c 2 Results are model dependent (for e. g. with slepton mixing the acceptance is worse and there are no new constraints yet) Ø Beyond LEP (in these scenarios) Ø More luminosity is being added Ø Already implementing some improvements. . . SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 19

OUTLINE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 20

OUTLINE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 20

GMSB: gg+MET In Gauge Mediated Supersymmetry Breaking (GMSB) model the neutralino is the NLSP

GMSB: gg+MET In Gauge Mediated Supersymmetry Breaking (GMSB) model the neutralino is the NLSP and the gravitino the LSP (~1 ke. V/c 2). D 0 with 760 pb-1: ü 2 photons (ET>25 Ge. V) NLO ü MET > 45 Ge. V Previous D 0 result (263 pb-1) SM expect: 2. 1 events New D 0 result (760 pb-1) Observation: 1 event Neutralino Chargino New constraints for this process L is the only dimensioned parameter of the GMSB model. SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 21

OUTLINE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 22

OUTLINE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 22

ASSUMPTIONS RPV: CHARGINO/NEUTRALINO ü Only first term of WRPV is considered (protect proton lifetime)

ASSUMPTIONS RPV: CHARGINO/NEUTRALINO ü Only first term of WRPV is considered (protect proton lifetime) ü Charge current universality |l|<0. 135 Ge. V i, j, k denote the leptonic families involved. ü RPV vertex: only in the last decay. ü The decay is inside the detector ü In general: l 121 > l 122 >> l 133 Ø CDF: performing analyses only in l 121 and l 122 Ø D 0: analysing also l 133 (high tan , low m 0) A pair of at least 4 leptons and two neutrinos Also optimizing for 3 leptons to improve acceptance Only one RPV at a time l 121 0 eeee, eee , ee l 122 0 , e, ee Low background just for asking 4 leptons or more! SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 23

RPV: 4 LEPTONS Trilepton Signal Regions Dataset λ 121 : eel Λ 122: l

RPV: 4 LEPTONS Trilepton Signal Regions Dataset λ 121 : eel Λ 122: l Background 2. 9 ± 0. 8 1. 8 ± 1. 0 Rp. V SUSY 3. 8 ± 0. 4 4. 0 ± 0. 4 Data 5 1 ≥ 4 Signal Region Dataset Signal Background 0. 008 ± 0. 004 Rp. V SUSY 1. 5 ± 0. 3 Data 0 Probability to see >=5 with 2. 9 0. 8 is 17% Very low background! No event found after cuts m 0=1 Te. V ; tanb=5 m 0=100 Ge. V ; tanb=20 Dataset λ 121 : eel l 122: l l 133: eet Background 0. 9 ± 0. 4 ± 0. 1 1. 3 ± 1. 7 m (Ge. V/c 2) 119 118 86 115 m (Ge. V/c 2) 231 229 166 217 SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 24

RPV: STOP • 2 b-jets RPV vertex • 1 t hadronic (64. 8%) •

RPV: STOP • 2 b-jets RPV vertex • 1 t hadronic (64. 8%) • 1 t semi-leptonic (35. 2%) CHALLENGE: t identification Jets and leptons t misidentification RPV vertex Used Z tt for hadronic t ID: Eff ~ 56% Expected events: 2. 2 Observed events: 2 (1 e + 1 ) New mass limits are obtained with 322 pb-1 SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 25

OUTLINE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 26

OUTLINE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 26

INDIRECT SEARCHES: BS SM: Bs-> is heavily suppressed: SUSY: BR enhancement by 1 -3

INDIRECT SEARCHES: BS SM: Bs-> is heavily suppressed: SUSY: BR enhancement by 1 -3 orders of magn. (Buchalla & Buras, Misiak & Urban) New CDF result: 780 (Babu, Kolda: hep-ph/9909476+ many more) pb-1 Using B+ J/ K+ for normalization R. Dermisek et al. hep-ph/0507233 (2005) High resolution! s(M ) ~ 0. 23 Me. V Found 1 event; expected background 0. 9 0. 3 New limits at 95% C. L: BR(Bs ) < 1. 0· 10 -7 SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 27

DISCLAIMER Due to time constraints I couldn’t cover all the analyses for both detectors.

DISCLAIMER Due to time constraints I couldn’t cover all the analyses for both detectors. Some of the most interesting analyses, not covered here, are: Ø Stopped gluinos (split SUSY) (350 pb-1) Ø Long lived charginos (AMSB) (380 pb-1) This topic will be covered in the next talk Ø Resonant slepton production (RPV) (380 pb-1) Ø sneutrino e (RPV) (344 pb-1) You can find them all at the CDF or D 0 webpages: http: //www-cdf. fnal. gov/physics/exotic. html http: //www-d 0. fnal. gov/Run 2 Physics/WWW/results/np. htm SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 28

SUMMARY ØTevatron and detectors are performing very well: ü 1. 6 fb-1 delivered (collected:

SUMMARY ØTevatron and detectors are performing very well: ü 1. 6 fb-1 delivered (collected: 1. 3 fb-1) ü Upgrades have been performed during this shutdown ü This week Tevatron will start again fully operational and 2 fb-1 benchmark is getting closer. Ø Plenty of SUSY analyses going on at CDF/D 0 detectors. They are being improved with the addition of new data. Ø No SUSY particles have been discovered yet but both direct and indirect analyses are constraining the SUSY parameter space. Tevatron will keep constraining the SUSY parameters until the LHC era. . . and perhaps a surprise is found! SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 29

BACKUPS SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 30

BACKUPS SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 30

Different 3 -Leptons Scenarios In Standard m. Sugra the BR into taus is enhanced

Different 3 -Leptons Scenarios In Standard m. Sugra the BR into taus is enhanced smaller acceptance SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 31

CDF 3 -Leptons Analyses CHANNEL LUM TRIGGER PATH e e , e , 710

CDF 3 -Leptons Analyses CHANNEL LUM TRIGGER PATH e e , e , 710 High p. T Single Lepton + e/ 750 High p. T Single Lepton ee + e/ 350 High p. T Single Lepton + e/ 310 Low p. T Dilepton ee + track 610 Low p. T Dilepton No third lepton requirement => Higher acceptance Use e/mu only =>Very small backgrounds Sensitive to taus as 3 rd lepton => Keeps acceptance at high tan SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 32

-SUSY • DATA N events/2 Ge. V/c 2 §Drell-Yan §WZ §ZZ §ttbar §Fakes MET

-SUSY • DATA N events/2 Ge. V/c 2 §Drell-Yan §WZ §ZZ §ttbar §Fakes MET CDF 3 -Leptons Control Regions ? ? SIGNAL REGION 15 106 L=607 pb-1 §Drell-Yan §Dibosons §ZZ §bbbar - SUSY • DATA 76 M( ) MET (Ge. V) Dielectron Invariant Mass(Ge. V/c 2) LS-dilepton analysis has additional Control Regions to test conversion removal Dimuon PT(Ge. V/c) SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 33

CDF 3 -electron Event SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell,

CDF 3 -electron Event SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 34

3 -LEPTONS: PROJECTIONS SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 35

3 -LEPTONS: PROJECTIONS SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 35

Bs : PROJECTIONS SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 36

Bs : PROJECTIONS SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 36

SQUARKS/GLUINOS: FUTURE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 37

SQUARKS/GLUINOS: FUTURE SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 37

SQUARKS AND GLUINOS SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 38

SQUARKS AND GLUINOS SUSY Searches at Tevatron; HCP, Duke, May 2006 Xavier Portell, 38