study of the processes โ (๐)๐ with the cmd-3 detector at ...ย ยท the cmd-3 detector at...
TRANSCRIPT
Study of the processes ๐+๐โ โ ๐ฒ๐ฒ (๐)๐ with
the CMD-3 detector at VEPP-2000 collider
Vyacheslav Ivanov
phd student, CMD-3 collaboration
Novosibirsk, Russia
Pion-Kaon Interactions Workshop
JLab, 14.02.2018 1
Outline
1. VEPP-2000 collider and CMD-3 detector
2. ๐+๐โ โ ๐พ๐พ (๐)๐ processes: charged kaons/pions identification
3. ๐+๐โ โ ๐พ๐พ (๐)๐ processes
3.1 ๐พ+๐พโ๐+๐โ final state
3.2 ๐+๐โ โ ๐พ+๐พโ๐ and ๐พ+๐พโ๐(782) processes
3.3 ๐พ+๐พโ๐0 final state
4. Plans & Conclusion
2
3
โข ๐+๐โ symmetric beams machine for the energy scan
in range ๐ โ (2๐๐; 2.005 GeV)
โข Round beams technology used
โข The maximum luminosity is 1032 cmโ2sโ1 at
2.0 GeV
โข Compton backscattering beam energy measurement
(ยฑ60 keV precision)
โข ~ 120 pb-1 is collected by each detector, the goal is to
collect ~1 fb-1 in ~5 years
1. VEPP-2000 collider & CMD-3 detector
SND
CMD-3
4
CMD-3 detector
Drift chamber
Z chamber
LXe calorimeter CsI calorimeter
BGO calorimeter
TOF
๐ veto system
4
1.3 T solenoid
Physics program of CMD-3
โข (๐๐โ2) puzzle: precise measurement of ๐ =๐(๐+๐โโโ๐๐๐๐๐๐ )
๐(๐+๐โโ๐+๐โ) - the goal is to achieve <1%
systematic for major channels
โข Study of exclusive hadronic channels of ๐+๐โ annihilation, test of isotopic relations
โข Study of the โexcitedโ vector mesons: ๐โฒ, ๐โฒโฒ, ๐โฒ, ๐โฒโฆ
โข CVC tests: comparison of isovector part of ๐(๐+๐โ โ โ๐๐๐๐๐๐ ) with ๐ โdecay spectra
โข Study of GE/GM for nucleons near threshold
โข Diphoton physics (e.g. ๐โฒ production)
5
CMD-3 data analysis status
Conversion decays
Dark photon search
- Preliminary results reported at conferences
- Final results are published
- Is being studied, not reported
+ also ๐ฒ+๐ฒโ๐๐ ๐,
๐ฒ๐บ๐ฒยฑ๐ โ๐ ๐ etc.
2. ๐+๐โ โ ๐ฒ๐ฒ (๐)๐ processes: kaon/pion separation โข ๐พ/๐ separation is the starting point and key issue for such processes
๐ฒ+๐ฒโ๐ +๐ โ events (MC)
โข We use the ๐๐ธ/๐๐ฅ in drift chamber
(DC), but for single kaons and pions it
works reliably only up to ๐ <450 MeV/c
โข For the final states ๐พ+๐พโ, ๐พ+๐พโ๐0, ๐พ+๐พโ2๐0 the use of ๐๐ธ/๐๐ฅ๐ท๐ถ is
insufficient
โข We are developing the PID procedure
with the use of ๐๐ธ/๐๐ฅ๐ฟ๐๐ in 14 layer
LXe-calorimeter
MC MC
LXe-calorimeter of CMD-3
๐๐๐
๐๐๐
DC
CsI
BGO
CsI
BGO
BGO
BGO
The PID with LXe โข For each DC-track we calculate the 10 values of the responses of the boosted decision trees (BDT)
classifiers, trained for the separation of particular pair of charged particles in particular ranges of
momenta and path length in LXe-layer (2200 classifiers in total):
๐ยฑ ๐ยฑ ๐ยฑ ๐พยฑ
๐ยฑ ๐ ๐๐ ๐๐๐๐ ๐๐๐(๐ยฑ/๐ยฑ) - - -
๐ยฑ ๐ ๐๐ ๐๐๐๐ ๐๐๐(๐ยฑ/๐ยฑ) ๐ ๐๐ ๐๐๐๐ ๐๐๐(๐
ยฑ/๐ยฑ) - -
๐พยฑ ๐ ๐๐ ๐๐๐๐ ๐๐๐(๐พยฑ/๐ยฑ) ๐ ๐๐ ๐๐๐๐ ๐๐๐(๐พ
ยฑ/๐ยฑ) ๐ ๐๐ ๐๐๐๐ ๐๐๐(๐พยฑ/๐ยฑ) -
๐ยฑ ๐ ๐๐ ๐๐๐๐ ๐๐๐(๐ยฑ/๐ยฑ) ๐ ๐๐ ๐๐๐๐ ๐๐๐(๐
ยฑ/๐ยฑ) ๐ ๐๐ ๐๐๐๐ ๐๐๐(๐ยฑ/๐ยฑ) ๐ ๐๐ ๐๐๐๐ ๐๐๐(๐
ยฑ/๐พยฑ)
โข The training samples: MC for ๐พยฑ, MC &
experimental events for others
โข Input variables: ๐๐ธ/๐๐ฅ๐ท๐ถ , 14 values of
๐๐ธ/๐๐ฅ๐ฟ๐๐
โข Sophisticated detector response simulation is
required: determination of the layers
transparency coefficients, correlative and
anticorrelative redistribution of induced
charge between upper and lower strips etc.,
โgeometric effectโ, recombination etc.
rotation in magnetic field
โข Main problem: bad simulation of ๐โ, ๐พโ interactions with nuclei (the PID only for ๐+, ๐พ+
will be used at first)
๐ ๐ฌ/๐ ๐๐ณ๐ฟ๐ in 14 layers: MC/exp comparison for ๐ +
โข ๐+ sample is selected from 2๐+2๐โ events, ๐ โ (1.6 GeV; 2 GeV)
EXP MC
๐ ๐ฌ/๐ ๐๐ณ๐ฟ๐ in 14 layers: MC/exp comparison for ๐ โ
โข ๐โ sample is selected from 2๐+2๐โ events, ๐ โ (1.6 GeV; 2 GeV)
EXP MC
MC/exp comparison for ๐ โ & ๐ +
๐ โ ๐ +
๐ โ ๐ +
LXe cluster energy / path, MeV/c LXe cluster energy / path, MeV/c
total cluster energy / path, MeV/c total cluster energy / path, MeV/c
๐ ๐ฌ/๐ ๐๐ณ๐ฟ๐ in 14 layers: MC/exp comparison for ๐ฒ+
โข ๐พ+ sample is selected from ๐พ+๐พโ๐+๐โ events, ๐ โ (1.6 GeV; 2 GeV)
EXP MC
๐ ๐ฌ/๐ ๐๐ณ๐ฟ๐ in 14 layers: MC/exp comparison for ๐ฒโ
โข ๐พโ sample is selected from ๐พ+๐พโ๐+๐โ events, ๐ โ (1.6 GeV; 2 GeV)
EXP MC
โข Background suppression via cuts on BDT responses:
electrons muons pions
Example: selection of ๐+๐โ โ ๐ฒ+๐ฒโ(๐ธ) at ๐ > ๐. ๐ ๐๐๐
Example: selection of ๐+๐โ โ ๐ฒ+๐ฒโ(๐ธ) at ๐ > ๐. ๐ ๐๐๐
๐ยฑ suppression ๐ยฑ & ๐ยฑ suppression
๐ยฑ & ๐ยฑ & ๐ยฑ suppression
3.1 Study of ๐+๐โ โ ๐ฒ+๐ฒโ๐ +๐ โ process
โข The major intermediate states were found to be
โข ๐0(500)๐ & ๐0(980)๐ โข ๐ 770 ๐พ๐พ ๐โ๐ค๐๐ฃ๐ โข (๐พ1 1270 ๐พ)๐โ๐ค๐๐ฃ๐โ (๐พโ(892)๐)๐โ๐ค๐๐ฃ๐๐พ โข (๐พ1 1400 ๐พ)๐โ๐ค๐๐ฃ๐โ (๐พโ(892)๐)๐โ๐ค๐๐ฃ๐๐พ โข (๐พ1 1400 ๐พ)๐โ๐ค๐๐ฃ๐โ (๐ 770 ๐พ)๐โ๐ค๐๐ฃ๐๐พ
โข Their relative amplitudes were found from the unbinned fit
of the data (relative phases were fixed at 0)
โข 2011-2012 energy scan, 23 pbโ1
โข Event selection: 4 or 3 tracks
โข Kaon/pion separation using log-likelihood function
based on ๐๐ธ/๐๐ฅ๐ท๐ถ:
โข 4-tracks events: signal events selection using energy-
momentum conservation
โข 3-tracks events: signal/background separation by fitting
energy disbalance distribution
โข => ~24k of signal events selected
MC for signal
data
Study of the dynamics of ๐ฒ+๐ฒโ๐ +๐ โ production
Ec.m. = 1.95 GeV
๐พโ(892)
๐ 770 ๐(1020)
Ec.m. = 1.95 GeV Ec.m. = 1.95 GeV
Cross section of the ๐+๐โ โ ๐ฒ+๐ฒโ๐ +๐ โ process
CMD-3
CMD-3 โข The results for 2011-2012 scan were
published, but new 2017 scan with ~60
๐๐โ1 of integrated luminosity provided
~3 times more signal events
โข First look: we see a systematic drop near
๐๐ threshold
โข But the result is too preliminary to make
any statement
๐๐ ๐ฆ๐ ๐ก = 6 รท 12%
3.2 Study of ๐+๐โ โ ๐ฒ+๐ฒโ๐ผ & ๐ฒ+๐ฒโ๐(๐๐๐) processes
โข ๐ and ๐(782) are treated as the recoil particles
โข Only ๐๐ intermediate state is seen in ๐พ+๐พโ๐
โข Event classes with 2, 3 and 4 tracks are considered. ๐พ/๐ separation is performed using log-
likelihood function. For instance, in 2-track class the distribution is:
Study of ๐+๐โ โ ๐ฒ+๐ฒโ๐ผ & ๐ฒ+๐ฒโ๐(๐๐๐) processes
โข ๐พ+๐พโ๐+๐โ is the major background in 3- and 4-track classes:
โข But it can be suppressed by the cuts on 2๐พ๐ and 2๐พ2๐ missing masses:
Study of ๐+๐โ โ ๐ฒ+๐ฒโ๐ผ & ๐ฒ+๐ฒโ๐(๐๐๐) processes โข ๐๐ selection:
โข Signal/background separation for both processes is performed by fitting of ๐๐๐๐ ๐ ,2๐พ distribution
๐
๐(782)
๐+๐โ โ ๐๐ผ cross section fitting โข Fitting of the ๐+๐โ โ ๐๐ cross section is the one of the best way for ๐(1680) parameters extraction
โข Cross section of ๐+๐โ โ ๐๐ is parametrized by quasi-two body formula
or, more precisely, as three-body expression
with
โข New data of 2017 scan is being
analyzed and new ๐(1680) -
dedicated scans are planned for
near future => we are at good
disposition to perform the most
precise study of ๐โฒ
๐+๐โ โ ๐ฒ+๐ฒโ๐(๐๐๐) cross section fitting
where
and the components of hadronic current ๐ฝ๐ฅ,๐ฆ are
3.3 ๐ฒ+๐ฒโ๐ ๐ final state
โข Events selection: 2 tracks, >= 2 photons
โข 4C kinematic fit with all the photon pairs (energy-momentum conservation required), ๐2 < 35
โข The main backgrounds: ๐พ+๐พโ๐พ , ๐พ+๐พโ2๐0 ,
๐พยฑ๐พ๐,๐ฟ๐โ, ๐+๐โ๐0, ๐+๐โ2๐0
โข The background suppression is performed by the
training of BDT classifier. The input variables are:
1) ๐๐ธ/๐๐ฅ๐ท๐ถ, 2) momenta and angles of charged
particles & photons 3) ๐2๐๐๐ ๐ ,2๐พ
Conclusion & Plans
Thank you for attention!
โข CMD-3 collaboration is progressing in datataking and data analysis for the ๐+๐โ โ ๐พ๐พ (๐)๐
processes
โข ๐พ/๐ separation is the starting point and key issue for such processes => the charged PID
procedure using ๐๐ธ/๐๐ฅ๐ฟ๐๐ is being developed
โข ๐+๐โ โ ๐พ๐พ (๐)๐ processes has reach dynamics, provide a case for isotopic relations test and,
especially, for ๐ 1680 parameters measurement