Download presentation
Presentation is loading. Please wait.
1
Search for ๐ + ๐ โ โ๐ผฯ(๐๐บ) above center-of-mass energy ๐ =๐.๐๐๐ฎ๐๐ฝ
๐ท๐๐๐ ๐ถโ๐๐ 1,2 , ๐ฟ๐ ๐พ๐ 2,3 ,Song Jiaojiao 2,3 , ๐๐ข๐๐ ๐ถโ๐๐๐๐งโ๐๐๐ 2 ๐๐๐๐๐๐ ๐๐๐๐ฃ๐๐๐ ๐๐ก๐ฆ 1 ๐ผ๐ป๐ธ๐ 2 , ๐๐ท๐ 3
2
Outline Motivation Data set Event selection
Data and Background analysis Signal extraction Cross section measurement Systematic error estimation Summary and plans
3
Motivation Many exotic charmoniumlike states have been
discovered around 4GeV, which means hidden charm coupling is also prominent for new states lying in this energy region. Thus, careful investigation of hidden charm cross section is necessary and will give us a chance to clarify new charmoniumlike states. BESIII have collected ~4 ๐๐ โ1 data above 4.0GeV. It is a good opportunity to investigate hidden charm decays, such as ๐ + ๐ โ โ ฮทฯ 2S .
4
Data set ๏Decay channels: ๏Data sets:
๐ + ๐ โ โ ๐๐ 2๐ ; ฮท โ ๐พ๐พ, ๐(2S) โ ๐ + ๐ โ J/ ฯ; J/ ฯ โ ๐ + ๐ โ / ๐ + ๐ โ ; ๐โ๐ ๐กโ๐๐๐ โ๐๐๐ ๐๐ 4.234๐บ๐๐! ๏Data sets: ๐ (GeV) Luminosity( ๐๐ โ1 ) 4.260 825.7 4.310 44.9 4.360 544.5 4.390 55.2 4.420 1023.3 4.470 110.7 4.530 110.5 4.575 47.7 4.600 567.7 ๏ Inclusive MC: ~500 pb ๏ Signal MC: 10k events for each channel; ๏ BOSS version: 7.0.2
5
Event selection Charged tracks: Good photon: Particle identification:
Rxy < 1cm,|Rz |< 10cm; ๐๐๐ ๐ <0.93; โQ=0; ๐ ๐๐๐๐ =4. 0โค๐๐ท๐ถโค14; Barrel: ๐ธ>25๐๐๐, ๐๐๐ ๐ <0.8 ; Endcap: ๐ธ>50๐๐๐ , 0.86< ๐๐๐ ๐ <0.92 ; ๐ ๐พ โฅ2. ๐ ยฑ : ๐ ๐๐๐ <0.6๐บ๐๐; ๐ ยฑ : ๐ ๐๐๐ >1.0๐บ๐๐& ๐ธ ๐๐๐ >1.0๐บ๐๐; ๐ ยฑ : ๐ ๐๐๐ >1.0๐บ๐๐& ๐ธ ๐๐๐ <0.6๐บ๐๐; Good photon: Particle identification: ๐ ยฑ ๐ ยฑ ๐ ยฑ ๐ ยฑ
6
Event selection 4C kinematic fit: Other selections: ๐ 4๐ถ 2 <40;
left: J/ ฯ โ ๐ + ๐ โ Right: J/ ฯ โ ๐ + ๐ โ Other selections: J/ฯ ๐๐๐ ๐ ๐ค๐๐๐๐๐ค: 3.08โ3.12 ๐บ๐๐ ฯ 2๐ ๐๐๐ ๐ ๐ค๐๐๐๐๐ค: 3.678โ3.706 ๐บ๐๐
7
Data and background analysis
๐(๐พ๐พ) VS. ๐( ฯ + ฯ โ ๐ + ๐ โ )โ๐ ๐ + ๐ โ +๐(๐ฝ/ฯ) Full data samples
8
Background shape estimation (sideband)
ฯ 2๐ ๐ ๐๐๐๐๐ ๐๐๐๐๐ : 3.666, ๐บ๐๐; ฯ 2๐ ๐ ๐๐๐๐๐๐๐ ๐๐๐๐๐: 3.626, ๐บ๐๐ ๐๐๐ , ๐บ๐๐. full 4420
9
Signal extraction: Simultaneous fit
Signal shape: Double Gaussian function. (Resolutions are determined by MC samples and the number of events of each channel is constrained by ๐ ๐ ๐ต ๐. ) Background shape: Linear function at all energy points. ๐น๐ข๐๐ ๐ ๐๐๐ ๐๐ 19ยฑ6; ๐๐ก๐๐ก๐๐ ๐ก๐๐๐๐ ๐ ๐๐๐๐๐๐๐๐๐๐๐ ๐๐ ๐๐๐ ๐ ๐กโ๐๐ 5ฯ ๐๐ก ๐๐กโ๐๐ ๐๐๐๐๐๐ฆ ๐๐๐๐๐ก๐ , ๐๐๐ ๐กโ๐ ๐๐๐๐๐๐ ๐ก ๐๐๐ ๐๐ 3.1ฯ. 5.8ฯ
10
Signal extraction: Simultaneous fit
4260 4420
11
Signal extraction: Simultaneous fit
4470 4600
12
Cross section measurement
๐โ๐ ๐ต๐๐๐ ๐๐๐๐ ๐ ๐ ๐๐๐ก๐๐๐ ๐๐ ๐๐๐๐๐ข๐๐๐ก๐๐ ๐ข๐ ๐๐๐ ๐กโ๐ ๐๐๐๐๐ข๐๐: ๐ผ๐๐๐ข๐ก ๐กโ๐๐ ๐ โ๐๐๐ ๐๐ ๐๐๐๐๐๐๐ก๐๐! ๐ถ๐ข๐๐๐ ๐ ๐๐๐๐๐
13
Cross section measurement
14
Systematic error estimation
๐๐๐ข๐๐๐๐ ๐๐๐กโ๐๐ ๐ฟ๐ข๐๐๐๐๐ ๐๐ก๐ฆ 1.0% ๐ข๐ ๐๐๐ ๐ตโ๐๐โ๐ ๐๐ฃ๐๐๐ก๐ ๐ต๐๐๐๐๐๐๐ข๐๐ ๐ โ๐๐๐ ๐๐๐ฆ ๐ 2 ๐๐ ๐๐๐๐๐ ๐๐๐๐ฆ๐๐๐๐๐๐ ๐น๐๐ก๐ก๐๐๐ ๐๐๐๐๐ ๐๐๐๐ฆ ๐กโ๐ ๐๐๐ก๐ก๐๐๐ ๐๐๐๐๐ ๐ผ๐๐
๐๐๐๐๐๐๐ก๐๐๐ ๐๐ ๐ ๐๐๐๐๐๐๐๐๐ก ๐ โ๐๐๐๐ ๐๐ ฯ ๐โ๐๐ก๐๐ 1.0% ๐๐๐ ๐โ๐๐ก๐๐ ๐๐๐๐๐๐๐๐ 1.0% ๐๐๐ ๐โ๐๐๐๐๐ ๐ก๐๐๐๐ ๐ฝ/๐ ๐๐๐ ๐ ๐ค๐๐๐๐๐ค ๐๐ ๐ ๐พ ๐ผ๐๐
๐ 2๐ ๐๐๐๐ก๐๐๐ ๐ ๐๐๐๐๐ ๐ก๐ ๐๐ ๐ก๐๐๐๐ก๐ ๐ 2๐ ๐๐๐ ๐ ๐ค๐๐๐๐๐ค ๐๐๐๐ฆ ๐กโ๐ ๐๐๐ ๐ ๐๐๐๐๐ ๐พ๐๐๐๐๐๐ก๐๐ ๐๐๐ก ๐ถ๐๐๐๐๐๐ก ๐กโ๐ ๐ก๐๐๐๐ โ๐๐๐๐ฅ ๐๐๐๐๐๐๐ก๐๐๐ ๐๐๐ ๐ก๐๐๐ ๐กโ๐ ๐๐๐๐๐๐๐๐๐๐ ๐๐๐ก๐ค๐๐๐ ๐๐ถ ๐ค๐๐กโ ๐๐๐ ๐ค๐๐กโ๐๐ข๐ก ๐๐๐๐๐๐๐ก๐๐๐ ๐ต๐๐๐๐โ๐๐๐ ๐๐๐๐๐ก๐๐๐ ๐๐๐๐๐ ๐๐๐๐ ๐๐ท๐บ
15
๐ก๐ค๐ ๐๐๐๐ฆ ๐โ๐๐ ๐ ๐ ๐๐๐๐ ๐๐ข๐๐๐ก๐๐๐
ISR correction
16
Thanks for your attention.
Summary and plans Observed the ๐ + ๐ โ โ๐๐(2๐) process with a statistical significance of 5.8๐ from full data sets. Born Cross sections are measured at 4.258, 4.416, and 4.6 GeV with large statistical error. There seems enhancement around the threshold, new data will be very helpful. Systematic uncertainties are estimated. Include more decays of ฮท and ๐(2S), ๐โ3๐, and ๐ 2๐ โ ๐ + ๐ โ , by Song Jiaojiao Analyze the data at GeV and the coming data. Thanks for your attention.
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.