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1 Search for ๐’† + ๐’† โˆ’ โ†’๐œผฯˆ(๐Ÿ๐‘บ) above center-of-mass energy ๐’” =๐Ÿ’.๐Ÿ๐Ÿ”๐‘ฎ๐’†๐‘ฝ
๐ท๐‘œ๐‘›๐‘” ๐ถโ„Ž๐‘Ž๐‘œ 1,2 , ๐ฟ๐‘– ๐พ๐‘’ 2,3 ,Song Jiaojiao 2,3 , ๐‘Œ๐‘ข๐‘Ž๐‘› ๐ถโ„Ž๐‘Ž๐‘›๐‘”๐‘งโ„Ž๐‘’๐‘›๐‘” 2 ๐‘๐‘Ž๐‘›๐‘˜๐‘Ž๐‘– ๐‘ˆ๐‘›๐‘–๐‘ฃ๐‘’๐‘Ÿ๐‘ ๐‘–๐‘ก๐‘ฆ 1 ๐ผ๐ป๐ธ๐‘ƒ 2 , ๐‘†๐ท๐‘ˆ 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 ๐‘“๐‘ โˆ’1 data above 4.0GeV. It is a good opportunity to investigate hidden charm decays, such as ๐‘’ + ๐‘’ โˆ’ โ†’ ฮทฯˆ 2S .

4 Data set ๏ƒ˜Decay channels: ๏ƒ˜Data sets:
๐‘’ + ๐‘’ โˆ’ โ†’ ๐œ‚๐œ“ 2๐‘† ; ฮท โ†’ ๐›พ๐›พ, ๐œ“(2S) โ†’ ๐œ‹ + ๐œ‹ โˆ’ J/ ฯˆ; J/ ฯˆ โ†’ ๐‘’ + ๐‘’ โˆ’ / ๐œ‡ + ๐œ‡ โˆ’ ; ๐‘‡โ„Ž๐‘’ ๐‘กโ„Ž๐‘Ÿ๐‘’๐‘ โ„Ž๐‘œ๐‘™๐‘‘ ๐‘–๐‘  4.234๐บ๐‘’๐‘‰! ๏ƒ˜Data sets: ๐‘  (GeV) Luminosity( ๐‘๐‘ โˆ’1 ) 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 ๏ƒ˜ Inclusive MC: ~500 pb ๏ƒ˜ Signal MC: 10k events for each channel; ๏ƒ˜ BOSS version: 7.0.2

5 Event selection Charged tracks: Good photon: Particle identification:
Rxy < 1cm,|Rz |< 10cm; ๐‘๐‘œ๐‘ ๐œƒ <0.93; โˆ‘Q=0; ๐‘ ๐‘”๐‘œ๐‘œ๐‘‘ =4. 0โ‰ค๐‘‡๐ท๐ถโ‰ค14; Barrel: ๐ธ>25๐‘€๐‘’๐‘‰, ๐‘๐‘œ๐‘ ๐œƒ <0.8 ; Endcap: ๐ธ>50๐‘€๐‘’๐‘‰ , 0.86< ๐‘๐‘œ๐‘ ๐œƒ <0.92 ; ๐‘ ๐›พ โ‰ฅ2. ๐œ‹ ยฑ : ๐‘ƒ ๐‘š๐‘‘๐‘ <0.6๐บ๐‘’๐‘‰; ๐‘’ ยฑ : ๐‘ƒ ๐‘š๐‘‘๐‘ >1.0๐บ๐‘’๐‘‰& ๐ธ ๐‘’๐‘š๐‘ >1.0๐บ๐‘’๐‘‰; ๐œ‡ ยฑ : ๐‘ƒ ๐‘š๐‘‘๐‘ >1.0๐บ๐‘’๐‘‰& ๐ธ ๐‘’๐‘š๐‘ <0.6๐บ๐‘’๐‘‰; Good photon: Particle identification: ๐œ‹ ยฑ ๐œ‡ ยฑ ๐‘™ ยฑ ๐‘’ ยฑ

6 Event selection 4C kinematic fit: Other selections: ๐œ’ 4๐ถ 2 <40;
left: J/ ฯˆ โ†’ ๐‘’ + ๐‘’ โˆ’ Right: J/ ฯˆ โ†’ ๐œ‡ + ๐œ‡ โˆ’ Other selections: J/ฯˆ ๐‘š๐‘Ž๐‘ ๐‘  ๐‘ค๐‘–๐‘›๐‘‘๐‘œ๐‘ค: 3.08โˆ’3.12 ๐บ๐‘’๐‘‰ ฯˆ 2๐‘† ๐‘š๐‘Ž๐‘ ๐‘  ๐‘ค๐‘–๐‘›๐‘‘๐‘œ๐‘ค: 3.678โˆ’3.706 ๐บ๐‘’๐‘‰

7 Data and background analysis
๐‘€(๐›พ๐›พ) VS. ๐‘€( ฯ€ + ฯ€ โˆ’ ๐‘™ + ๐‘™ โˆ’ )โˆ’๐‘€ ๐‘™ + ๐‘™ โˆ’ +๐‘€(๐ฝ/ฯˆ) Full data samples

8 Background shape estimation (sideband)
ฯˆ 2๐‘† ๐‘ ๐‘–๐‘”๐‘›๐‘Ž๐‘™ ๐‘Ÿ๐‘Ž๐‘›๐‘”๐‘’ : 3.666, ๐บ๐‘’๐‘‰; ฯˆ 2๐‘† ๐‘ ๐‘–๐‘‘๐‘’๐‘๐‘Ž๐‘›๐‘‘ ๐‘Ÿ๐‘Ž๐‘›๐‘”๐‘’: 3.626, ๐บ๐‘’๐‘‰ ๐‘Ž๐‘›๐‘‘ , ๐บ๐‘’๐‘‰. 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œ– ๐‘– ๐ต ๐‘–. ) Background shape: Linear function at all energy points. ๐น๐‘ข๐‘™๐‘™ ๐‘ ๐‘œ๐‘๐‘  ๐‘–๐‘  19ยฑ6; ๐‘†๐‘ก๐‘Ž๐‘ก๐‘–๐‘ ๐‘ก๐‘–๐‘๐‘Ž๐‘™ ๐‘ ๐‘–๐‘”๐‘›๐‘–๐‘“๐‘–๐‘๐‘Ž๐‘›๐‘๐‘’ ๐‘–๐‘  ๐‘™๐‘’๐‘ ๐‘  ๐‘กโ„Ž๐‘Ž๐‘› 5ฯƒ ๐‘Ž๐‘ก ๐‘œ๐‘กโ„Ž๐‘’๐‘Ÿ ๐‘’๐‘›๐‘’๐‘Ÿ๐‘”๐‘ฆ ๐‘๐‘œ๐‘–๐‘›๐‘ก๐‘ , ๐‘Ž๐‘›๐‘‘ ๐‘กโ„Ž๐‘’ ๐‘๐‘–๐‘”๐‘”๐‘’๐‘ ๐‘ก ๐‘œ๐‘›๐‘’ ๐‘–๐‘  3.1ฯƒ. 5.8ฯƒ

10 Signal extraction: Simultaneous fit
4260 4420

11 Signal extraction: Simultaneous fit
4470 4600

12 Cross section measurement
๐‘‡โ„Ž๐‘’ ๐ต๐‘œ๐‘Ÿ๐‘› ๐‘๐‘Ÿ๐‘œ๐‘ ๐‘  ๐‘ ๐‘’๐‘๐‘ก๐‘–๐‘œ๐‘› ๐‘–๐‘  ๐‘๐‘Ž๐‘™๐‘๐‘ข๐‘™๐‘Ž๐‘ก๐‘’๐‘‘ ๐‘ข๐‘ ๐‘–๐‘›๐‘” ๐‘กโ„Ž๐‘’ ๐‘“๐‘œ๐‘Ÿ๐‘š๐‘ข๐‘™๐‘Ž: ๐ผ๐‘›๐‘๐‘ข๐‘ก ๐‘กโ„Ž๐‘–๐‘  ๐‘ โ„Ž๐‘Ž๐‘๐‘’ ๐‘–๐‘› ๐‘”๐‘’๐‘›๐‘’๐‘Ÿ๐‘Ž๐‘ก๐‘œ๐‘Ÿ! ๐ถ๐‘ข๐‘๐‘–๐‘ ๐‘ ๐‘๐‘™๐‘–๐‘›๐‘’

13 Cross section measurement

14 Systematic error estimation
๐‘†๐‘œ๐‘ข๐‘Ÿ๐‘๐‘’๐‘  ๐‘€๐‘’๐‘กโ„Ž๐‘œ๐‘‘ ๐ฟ๐‘ข๐‘š๐‘–๐‘›๐‘œ๐‘ ๐‘–๐‘ก๐‘ฆ 1.0% ๐‘ข๐‘ ๐‘–๐‘›๐‘” ๐ตโ„Ž๐‘Ž๐‘โ„Ž๐‘Ž ๐‘’๐‘ฃ๐‘’๐‘›๐‘ก๐‘  ๐ต๐‘Ž๐‘๐‘˜๐‘”๐‘Ÿ๐‘œ๐‘ข๐‘›๐‘‘ ๐‘ โ„Ž๐‘Ž๐‘๐‘’ ๐‘‡๐‘Ÿ๐‘ฆ ๐‘Ž 2 ๐‘›๐‘‘ ๐‘œ๐‘Ÿ๐‘‘๐‘’๐‘Ÿ ๐‘๐‘œ๐‘™๐‘ฆ๐‘›๐‘œ๐‘š๐‘–๐‘Ž๐‘™ ๐น๐‘–๐‘ก๐‘ก๐‘–๐‘›๐‘” ๐‘Ÿ๐‘Ž๐‘›๐‘”๐‘’ ๐‘‰๐‘Ž๐‘Ÿ๐‘ฆ ๐‘กโ„Ž๐‘’ ๐‘“๐‘–๐‘ก๐‘ก๐‘–๐‘›๐‘” ๐‘Ÿ๐‘Ž๐‘›๐‘”๐‘’ ๐ผ๐‘†๐‘… ๐‘๐‘œ๐‘Ÿ๐‘Ÿ๐‘’๐‘๐‘ก๐‘–๐‘œ๐‘› ๐‘ˆ๐‘ ๐‘’ ๐‘‘๐‘–๐‘“๐‘“๐‘’๐‘Ÿ๐‘’๐‘›๐‘ก ๐‘ โ„Ž๐‘Ž๐‘๐‘’๐‘  ๐‘œ๐‘“ ฯƒ ๐‘ƒโ„Ž๐‘œ๐‘ก๐‘œ๐‘› 1.0% ๐‘๐‘’๐‘Ÿ ๐‘โ„Ž๐‘œ๐‘ก๐‘œ๐‘› ๐‘‡๐‘Ÿ๐‘Ž๐‘๐‘˜๐‘–๐‘›๐‘” 1.0% ๐‘๐‘’๐‘Ÿ ๐‘โ„Ž๐‘Ž๐‘Ÿ๐‘”๐‘’๐‘‘ ๐‘ก๐‘Ÿ๐‘Ž๐‘๐‘˜ ๐ฝ/๐œ“ ๐‘š๐‘Ž๐‘ ๐‘  ๐‘ค๐‘–๐‘›๐‘‘๐‘œ๐‘ค ๐‘ˆ๐‘ ๐‘’ ๐›พ ๐ผ๐‘†๐‘… ๐œ“ 2๐‘† ๐‘๐‘œ๐‘›๐‘ก๐‘Ÿ๐‘Ž๐‘™ ๐‘ ๐‘Ž๐‘š๐‘๐‘™๐‘’ ๐‘ก๐‘œ ๐‘’๐‘ ๐‘ก๐‘–๐‘š๐‘Ž๐‘ก๐‘’ ๐œ“ 2๐‘† ๐‘š๐‘Ž๐‘ ๐‘  ๐‘ค๐‘–๐‘›๐‘‘๐‘œ๐‘ค ๐‘‰๐‘Ž๐‘Ÿ๐‘ฆ ๐‘กโ„Ž๐‘’ ๐‘š๐‘Ž๐‘ ๐‘  ๐‘Ÿ๐‘Ž๐‘›๐‘”๐‘’ ๐พ๐‘–๐‘›๐‘’๐‘š๐‘Ž๐‘ก๐‘–๐‘ ๐‘“๐‘–๐‘ก ๐ถ๐‘œ๐‘Ÿ๐‘Ÿ๐‘’๐‘๐‘ก ๐‘กโ„Ž๐‘’ ๐‘ก๐‘Ÿ๐‘Ž๐‘๐‘˜ โ„Ž๐‘’๐‘™๐‘–๐‘ฅ ๐‘๐‘Ž๐‘Ÿ๐‘Ž๐‘š๐‘’๐‘ก๐‘’๐‘Ÿ๐‘  ๐‘Ž๐‘›๐‘‘ ๐‘ก๐‘Ž๐‘˜๐‘’ ๐‘กโ„Ž๐‘’ ๐‘‘๐‘–๐‘“๐‘“๐‘’๐‘Ÿ๐‘’๐‘›๐‘๐‘’ ๐‘๐‘’๐‘ก๐‘ค๐‘’๐‘’๐‘› ๐‘€๐ถ ๐‘ค๐‘–๐‘กโ„Ž ๐‘Ž๐‘›๐‘‘ ๐‘ค๐‘–๐‘กโ„Ž๐‘œ๐‘ข๐‘ก ๐‘๐‘œ๐‘Ÿ๐‘Ÿ๐‘’๐‘๐‘ก๐‘–๐‘œ๐‘› ๐ต๐‘Ÿ๐‘Ž๐‘›๐‘โ„Ž๐‘–๐‘›๐‘” ๐‘“๐‘Ÿ๐‘Ž๐‘๐‘ก๐‘–๐‘œ๐‘› ๐‘‡๐‘Ž๐‘˜๐‘’๐‘› ๐‘“๐‘Ÿ๐‘œ๐‘š ๐‘ƒ๐ท๐บ

15 ๐‘ก๐‘ค๐‘œ ๐‘๐‘œ๐‘‘๐‘ฆ ๐‘โ„Ž๐‘Ž๐‘ ๐‘’ ๐‘ ๐‘๐‘Ž๐‘๐‘’ ๐‘“๐‘ข๐‘›๐‘๐‘ก๐‘–๐‘œ๐‘›
ISR correction

16 Thanks for your attention.
Summary and plans Observed the ๐‘’ + ๐‘’ โˆ’ โ†’๐œ‚๐œ“(2๐‘†) process with a statistical significance of 5.8๐œŽ 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œ“(2S), ๐œ‚โ†’3๐œ‹, and ๐œ“ 2๐‘† โ†’ ๐‘™ + ๐‘™ โˆ’ , by Song Jiaojiao Analyze the data at GeV and the coming data. Thanks for your attention.


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