Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho,...
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![Page 1: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/1.jpg)
Mass and Spin measurement
with mT2 at the LHC
Yeong Gyun Kim(KAIST)
In collaboration withW.S.Cho, K.Choi, C.B.Park
![Page 2: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/2.jpg)
SUSY at the LHC
Mass measurement with mT2
Spin measurement with mT2
Conclusion
Contents
![Page 3: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/3.jpg)
We are entering exciting period in particle physics.
The LHC is about to explore for the first timethe TeV energy scale.
The origin of EWSB ?The nature of dark matter ?Supersymmetry ?Extra dimensions ?
![Page 4: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/4.jpg)
General features for SUSY at the LHC
SUSY production is dominated by gluinos and squarks, unless they are too heavy
The gluinos and squarks cascade down, generally in several steps, to the final states including multi-jets (and/or leptons) and two invisible LSPs
![Page 5: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/5.jpg)
Characteristic signals of SUSY with Rp
Invisible LSPs
Large Missing Transverse Energy
Decays of squarks and gluinos
Energetic hadronic jets
and/or Decays of sleptons and gauginos
Isolated leptons
![Page 6: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/6.jpg)
Supersymmetry searches
LHC focus weekTokyo 24/6/2008
T. LariINFN Milano
Discovery potential
5 evidence after 1 fb-1 (including systematics) expected if squarks lighter than 1300 GeV 0-lepton and 1-lepton best modes for mSUGRANo attempt to combine channels yet
~~
preliminary
(Taken from T.Lari’s talk in LHC focus week at IPMU, 2008)
![Page 7: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/7.jpg)
Discovery of New Physics
Mass measurements
Spin measurements, etc.
![Page 8: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/8.jpg)
Mass measurement of SUSY particles
Reconstruction of SUSY theory (SUSY breaking sector)
Weighing Dark Matter with collider
M1: M2: M3 = 1 : 2 : 6 mSUGRA pattern 3.3 : 1 : 9 AMSB pattern etc.
(Thermal relic DM density)
![Page 9: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/9.jpg)
Distinguishing SUSY from other models
The production rate of KK-gluon vs. gluino
(Datta, Kane, Toharia 2007)
Mass (GeV)
![Page 10: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/10.jpg)
SUSY events always contain two invisible LSPs
No masses can be reconstructed directly
Final state momentum in beam direction is unknown a priori, due to our ignorance of initial partonic center of mass frame
The Mass measurement is Not an easy task at the LHC !
![Page 11: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/11.jpg)
Several approaches (and variants) of mass measurements proposed
Invariant mass Edge method Hinchliffe, Paige, Shapiro, Soderqvist, Yao ; Allanach, Lester, Parker, Webber
… Mass relation method Kawagoe, Nojiri, Polesello ; Cheng, Gunion, Han, Marandellea, McElrath
Transverse mass (MT2 ) kink method
Lester, Summers; Cho, Choi, YGK, Park ; Barr, Gripaios, Lester; Ross, Serna; Burns, Kong, Park, Machev …
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Basic idea
Identify a particular long decay chain and measure kinematic endpoints of various invariant mass distributions of visible particles
The endpoints are given by functions of SUSY particle masses
Invariant mass edge method
Hinchliffe, Paige, etal.(1997)
![Page 13: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/13.jpg)
If a long enough decay chain is identified, It would be possible to measure all sparticle masses Through several endpoint measurements
3 step two-body decays
![Page 14: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/14.jpg)
Mass relation method
Consider the following cascade decay chain (4 step two-body decays)
Kawagoe, Nojiri, Polesello (2004)
Completely solve the kinematics of the cascade decay by using mass shell conditions of the sparticles
![Page 15: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/15.jpg)
One can write five mass shell conditions
which contain 4 unknown d.o.f of LSP momentum
Each event describes a 4-dim. hypersurface in 5-dim. mass space, and the hypersurfcae differs event by event
Many events determine a solution for masses through intersections of hypersurfaces
![Page 16: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/16.jpg)
Both the Edge method and the Mass relation method rely on a long decay chain to determine sparticle masses
What if we don’t have long enough decay chain but only short one ?
In such case, MT2 variable would be useful to get information on sparticle masses
![Page 17: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/17.jpg)
Mass measurement with MT2
![Page 18: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/18.jpg)
Cambridge mT2 variableLester, Summers (1999)
![Page 19: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/19.jpg)
Cambridge mT2(Lester and Summers, 1999)
Massive particles pair produced
Each decays to one visible and one invisible particle.
For example,
For the decay,
( )
![Page 20: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/20.jpg)
( : total MET vector in the event )
However, not knowing the form of the MET vector splitting,the best we can say is that :
with minimization over all possible trial LSP momenta
![Page 21: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/21.jpg)
MT2 distribution for
LHC point 5, with 30 fb-1,
(Lester and Summers, 1999)Endpoint measurement of mT2 distribution determinesthe mother particle mass
( with )
![Page 22: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/22.jpg)
Varying “” …
mT2()
mB mA
Does not just translate …
Shape may also change …
(Taken from Lester’s talk in the LHC focus week at IPMU)
(trial LSP mass)
![Page 23: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/23.jpg)
Maximum of mT2 as a function of trial LSP mass
(Lester and Summers, 1999)
The correlation from a numerical calculationcan be expressed by an analytic formulain terms of trueSUSY particle masses
![Page 24: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/24.jpg)
Well described by the above Analytic expression with truemother mass and true LSP mass
The maximum of the squark mT2 as a function of
(Cho, Choi, YGK and Park, 2007)
Mother mass and LSP mass are Not determined separately
without ISR
![Page 25: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/25.jpg)
(Cho, Choi, YGK and Park, arXiv:0709.0288)
Transverse Mass for Pairs of Gluinos (Gluino mT2)
![Page 26: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/26.jpg)
Gluino mT2
A new observable, which is an application of mT2 variable tothe process
Gluinos are pair produced in proton-proton collision
Each gluino decays into two quarks and one LSP through three body decay (off-shell squark)
or two body cascade decay (on-shell squark)
![Page 27: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/27.jpg)
mqq value for three body gluino decay
Each mother particleproducesone invisible LSPand more than one visible particle
![Page 28: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/28.jpg)
MT2 maximum as a function of trial LSP mass depends on di-quark invariant mass (mqq)
mqq=minimum
mqq=mqq
mqq=maximum
Trial LSP mass
MT2maximum
(Assume mqq(1) = mqq(2), for simplicity )
![Page 29: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/29.jpg)
Experimental feasibility
An example (a point in mAMSB)
with a few TeV sfermion masses (gluino undergoes three body decay)
We have generated a MC sample of SUSY events, which corresponds to 300 fb-1 by PYTHIA
The generated events further processed with PGS detector simulation,which approximates an ATLAS or CMS-like detector
![Page 30: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/30.jpg)
Gluino mT2 distributionwith the trial LSP mass mx = 90 GeV
Fitting with a linear functionwith a linear background,We get the endpoints
mT2 (max) =
The blue histogram :SM background
![Page 31: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/31.jpg)
as a function of the trial LSP mass for a benchmark point (Monte Carlo study)
Fitting the data points with the abovetwo theoretical curves, we obtain
The true values are GeV
![Page 32: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/32.jpg)
With the invariant mass edge method, we get only the mass difference of mother and LSP
Now, with the gluino mT2, We can get the absolute mass scale of SUSY particles
![Page 33: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/33.jpg)
Top quark mass with mT2
![Page 34: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/34.jpg)
(Cho,Choi, YGK, Park, arXiv:0804.2185) PRD 78, 034019 (2008)
Standard Candle for MT2 study
We can consider Top-quark mT2
Large statistics available at the LHC
Mass of invisible particle is already known (m_nu=0)
![Page 35: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/35.jpg)
Top quark mT2 distribution with m_nu = 0
With 10 fb-1 ,2 b-jets, 2 leptons,Large missing ET
for input mt=170.9 GeV.No systematic error included
Standard Candle for MT2 study
(Cho,Choi, YGK, Park, arXiv:0804.2185)
![Page 36: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/36.jpg)
mT2 max vs. trial neutrino mass Shape of mT2 distribution
The di-leptonic channel : A good playground for mT2 exercise
Standard Candle for MT2 study
(Cho,Choi, YGK, Park, arXiv:0804.2185)
![Page 37: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/37.jpg)
When MT2 met Real collider data...
![Page 38: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/38.jpg)
3 fb-1 of data collected with the CDF detector at Tevatron
~ 100 signal eventsin Dilepton channelafter event selection
Top events at CDF
(CDF note 9679)
![Page 39: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/39.jpg)
MT2 distributions for b-tagged Dilepton events (Full Monte Carlo) with various top masses at CDF
(CDF note 9679)
![Page 40: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/40.jpg)
MT2 distribution with Real Data(CDF II Preliminary, 3.0 fb-1)
![Page 41: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/41.jpg)
It is the first measurement using mT2 in the real data
It works quite well. The result is compatiblewith other measurements, giving a confidenceon mT2 method
When combined with other measurements,It improves precision in top mass measurement
![Page 42: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/42.jpg)
consider W as invisible
(ignoring lepton momentum)
MT2 distributionwhen trial W mass = true W mass
With 10 fb-1at the LHC (14 TeV)
![Page 43: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/43.jpg)
MT2 maximum as a function of trial W mass
An analog of slepton (or squark) mT2
![Page 44: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/44.jpg)
Spin measurement with MT2
![Page 45: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/45.jpg)
Is there any other usefulness of MT2, after determining new particle masses ?
Yes! M.A.O.S (MT2-Assissted On-Shell) reconstruction of WIMP momentum.
![Page 46: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/46.jpg)
MAOS reconstruction of WIMP momenta
(Cho, Choi, YGK, Park, arXiv:0810.4853)
![Page 47: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/47.jpg)
kT the values that determine MT2 , thenkz on-shell condition on the mother particle
MAOS reconstruction of WIMP momenta
(Cho, Choi, YGK, Park, arXiv:0810.4853)
A scheme to assign a 4-momentum to each WIMP in new physics events
MAOS WIMP momentum is given by
![Page 48: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/48.jpg)
MAOS WIMP momentum is rather well correlated to the true WIMP momentum.
MAOS mom. – TRUE mom. of WIMP
Full event set Top 10 % near mT2 max.
Example:
![Page 49: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/49.jpg)
Application of MAOS reconstruction (1)
Dalitz plot analysis ofGluino 3-body decay & UED equivalent
![Page 50: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/50.jpg)
• Gluino 3-body decay and UED equivalent
Di-quark invariant mass distribution
UED (blue/dashed)SUSY (red/solid)
(Csaki etal, 2007)
![Page 51: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/51.jpg)
• Gluino 3-body decay and UED equivalent
SUSY UED
TrueDistributions(partonic level)
Dalitz Plots of (Mqq)2 vs. (Mqx)2
MAOSReconstructions(partonic level)
![Page 52: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/52.jpg)
For 300 fb-1 , Detector-level study, No background
SUSY UED
(SPS2 point in mSUGRA)
![Page 53: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/53.jpg)
Application of MAOS reconstruction (2)
Angular distribution in Drell-Yan slepton production& UED equivalent
![Page 54: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/54.jpg)
• Drell-Yan slepton production & UED equiv.
Production angular distributions of mother particle pairin their center of mass frame, w.r.t. proton beam direction
(A.Barr, 2004)For SUSY
For UED
![Page 55: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/55.jpg)
• Drell-Yan slepton production & UED equiv.
For events near mT2 max
With MAOS reconstructionof the WIMP momenta andthus mother particle momenta
SUSY (blue/solid)UED (red/dotted)
Production angular distributions of mother particle pairin their center of mass frame, w.r.t. proton beam direction
![Page 56: Mass and Spin measurement with mT2 at the LHC Yeong Gyun Kim (KAIST) In collaboration with W.S.Cho, K.Choi, C.B.Park.](https://reader036.fdocuments.in/reader036/viewer/2022062516/56649e445503460f94b385d1/html5/thumbnails/56.jpg)
Application of MAOS reconstruction (3)
Analysis of top quark eventsin dilepton channel (Top mass and spin correlation)
Work in progress
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Consider WW sub-system in the dilepton channel of top events
Construct the MAOS momentumof neutrino for the sub-system,considering W bosons as mother particles (W mass is known well)
Calculate the invariant massof bW system, using the MAOS momentum of W boson
Top mass measurement with MAOS reconstruction
Construct MAOS momentum ofW boson by adding lepton mom.to the MAOS neutrino momentum
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Invariant mass distribution of the bW system(W momentum reconstructed with MAOS)
M(peak) ~ 170 GeV
MT2 (W-boson) > 60 GeV
Work in progress
Preliminary resultBased on parton-level MC
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Detector level simulation
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Top quark pair spin correlation
At Tevatron, the correlation C is -40 % (70 % of the pairs have the opposite helicity, while 30% have the same helicity)
At LHC, the correlation is +31 %
Can we measure the spin correlation in dilepton channel,with ‘improved’ MAOS neutrino momentum ?
Work in progress
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Conclusion
Maximum of gluino MT2 as a function of trial LSP mass shows a kink structure at true LSP mass from which gluino mass and LSP mass can be determined altogether.
Top-quark MT2 provides an independent way of measuring the top-quark mass and can serve as a Standard Candle for general MT2 analysis.
MAOS reconstruction of WIMP momentum may open a new window for investigating New physics structures
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The Horror of the Heights
Arther Conan Doyle
(1913)
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The Horror of the Heights(2008-)
Nothing new in the TeV scale….
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“ There are jungles of the upper air, and there are worse things than tigers which inhabit them. I believe in time they will map these jungles accurately out “
- Armstrong in ‘the Horror of the Height’
The Hope of the Heights (2008-)
SUSY jungle (sps1a)
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Backup Slides
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MAOS WIMP momentum is rather well correlated to the true WIMP momentum.
vs.