Zahra Haddadi, KVI-CART (University of Groningen) for the...
Transcript of Zahra Haddadi, KVI-CART (University of Groningen) for the...
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kvi - center for advanced radiation technology
Zahra Haddadi, KVI-CART (University of Groningen)
for the BESIII collaboration 1 Sep. 2015 EUNPC 2015, Groningen
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Outline:
Charmonium spectroscopy
spin-singlet states puzzle
BESIII & precision measurements
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QCD bound systems
QCD:
Is well tested at high energies.
In low-energy region, many aspects are not understood.
Charmonium spectroscopy:
Precise measurements on basic properties of known states.
Clean system to study non-perturbative QCD dynamics.
The mesonic bound state of cc.
Simplest bound state of QCD.
mc ≈ 1.4 GeV : Non-relativistic potential model.
Charmonium:
1 fm
C
C
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Charmonium spectrum
Potential model
describes spectrum very well;
Below the open-charm threshold
Narrow states
Good agreement between theory
and experiment
XYZ states:
Talk by Landdiao Liu Hadron Structure, Spectroscopy and dynamics II
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Charmonium spectrum
Vsdcvsdhsd chv,ejsd hc csd
Db cb dcvm
Mndsb cmnd b
Dnbcv
N bdfvcjb
Nb dcvkjvfdbk
Potential model
describes spectrum very well;
Below the open-charm threshold
Narrow states
Good agreement between theory
and experiment
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Charmonium spectrum
Vsdcvsdhsd chv,ejsd hc csd
Db cb dcvm
Mndsb cmnd b
Dnbcv
N bdfvcjb
Nb dcvkjvfdbk
Lattice QCD
Experiment
Phys. Rev. D 87, 034501 (2013)
Potential model
describes spectrum very well;
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Charmonium spectrum
Vsdcvsdhsd chv,ejsd hc csd
Db cb dcvm
Mndsb cmnd b
Dnbcv
N bdfvcjb
Nb dcvkjvfdbk
Lattice QCD
Experiment
Phys. Rev. D 87, 034501 (2013)
Potential model
describes spectrum very well;
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Mass Width
3
radiative transition
γ γ processes, pp, B→Kηc
Mass & Width of the ground state: ηc
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Mass Width
3
radiative transition
γ γ processes, pp, B→Kηc
Mass & width of the ground state: ηc
After 30 years: We still have problem with the basic properties of ηc.
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2.8
3.0
3.2
3.4
3.6
3.8
ηc
J/ψ
ψ′ η′c
χc0
χc1 χc2
Open-charm
ηc studies from e+e- annihilation
hc
ψˊ decay & e+e- annihilation:
clean and simple environment
L = 0 0 1 1 1 1 JPC = 0 -+ 1-- 1+- 0++ 1++ 2++
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2.8
3.0
3.2
3.4
3.6
3.8
ηc
J/ψ
ψ′ η′c
χc0
χc1 χc2
L = 0 0 1 1 1 1 JPC = 0 -+ 1-- 1+- 0++ 1++ 2++
Open-charm
hc
γ
ψˊ decay & e+e- annihilation:
clean and simple environment
ηc:
Mass and width and lineshape
ψˊ→γηc
suppressed M1 transition!
ηc studies from e+e- annihilation
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2.8
3.0
3.2
3.4
3.6
3.8
ηc
J/ψ
ψ′ η′c
χc0
χc1 χc2
Open-charm
hc
γ
π° ηc:
Mass and width and lineshape
ψˊ→γηc
suppressed M1 transition!
ψˊ→π°hc, hc→γηc
Isospin forbidden!
γ
ψˊ decay & e+e- annihilation:
clean and simple environment
L = 0 0 1 1 1 1 JPC = 0 -+ 1-- 1+- 0++ 1++ 2++
ηc studies from e+e- annihilation
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2.8
3.0
3.2
3.4
3.6
3.8
ηc
J/ψ
ψ′ η′c
χc0
χc1 χc2
Open-charm
hc
γ γ
π° ψˊ decay & e+e- annihilation:
clean and simple environment
ηc:
Mass, width and lineshape
ψˊ→γηc
Suppressed M1 transition!
ψˊ→π°hc, hc→γηc
Isospin forbidden!
J/ψ→γηc Suppressed M1 transition!
γ
L = 0 0 1 1 1 1 JPC = 0 -+ 1-- 1+- 0++ 1++ 2++
ηc studies from e+e- annihilation
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BESIII: BEijing Spectrometer (BES)
Magnet yoke
Main Drift Chamber
Time of Flight
Electromagnetic Calorimeter
SC magnet : 1T
e+
e-
Linac : 200 m
Storage ring :
240 m
BES III Detector
5
IP
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BESIII: BEijing Spectrometer (BES)
e+
e-
5
Magnet Yoke
Time of flight
Main drift chamber
SC magnet : 1T
Electromagnetic Calorimeter
Collected data by BESIII
By the end of 2012 :
450 ˣ 106 ψˊ
We are well equipped for measuring these transitions.
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2.8
3.0
3.2
3.4
3.6
3.8
ηc
J/ψ
ψ′ η′c hc
γ
6 exclusive decay modes
ψˊ→γηc
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1 of 6 decay
modes
ψˊ→γηc, ηc→ 2K2ππ°
7
Interference was found to be 15σ.
Long tail on the low mass side.
The signal drops rapidly on the
high-mass side.
Obviously asymmetric lineshape:
Interference between ηc and non-
resonant background is significant:
BES III (2012)
Mηc = 2984.3 ± 0.6 ± 0.6 MeV/c2
Γηc = 32.0 ± 1.2 ±1.0 MeV
PRL 108, 222002 (2012)
Simultaneous fit to 6 modes
Phases are consistent within 3σ
106 M ψˊ
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BES III (2012) Mηc = 2984.3 ± 0.6 ± 0.6 MeV/c2
ΔMhf(1S) = 112.6 ± 0.8 MeV/c2
Agrees well with recent lattice computations!
BESIII
Lattice 2012
arXiv:1211.2253
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BES III (2012) Mηc = 2984.3 ± 0.6 ± 0.6 MeV/c2
ΔMhf(1S) = 112.6 ± 0.8 MeV/c2
Agrees well with recent lattice computations!
BESIII
Lattice 2012
arXiv:1211.2253
Question : Can we see this distortion in the other radiative transition like
hc→γηc
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2.8
3.0
3.2
3.4
3.6
3.8
ηc
J/ψ
ψ′ η′c hc
16 exclusive decay modes
γ
π°
ψˊ→π°hc, hc→γηc
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lineshape in E1 transition hc→γηc ηc
Mηc = 2984.40 ± 1.16 ± 0.52 MeV/c2
Γηc = 36.4 ± 3.2 ± 1.7 MeV
Weaker interference
Larger amplitude
B(ψˊ→ γηc) = 0.3%
B(hc→ γηc) = 50%
Signal can be described by a simple Breit-Wigner
Sum of 16 ηc
decay modes
PRD 86,092009 Background
subtracted
106 M ψˊ
106 M ψˊ
compared with the result from ψˊ→γηc:
Mηc = 2984.3 ± 0.6 ± 0.6 MeV/c2
Γηc = 32.0 ± 1.2 ±1.0 MeV
Statistic error is dominated!
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Comparison of the latest results:
Understanding the nature of interference is the key point!
Ke Li
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Comparison of the latest results:
Understanding the nature of interference is the key point!
Ke Li
Ongoing analysis related to ηc: ψˊ→γηc : 450ˣ106 ψˊ hc→γηc : 450ˣ106 ψˊ Ј/ψ→γηc : 1ˣ109 J/ψ
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2.8
3.0
3.2
3.4
3.6
3.8
ηc
J/ψ
ψ′ η′c hc
γ
KsKπ KKπ°
ψˊ→γηcˊ
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First observation of the ψˊ→γηˊ
Mηcˊ = 3637.6 ± 2.9 ± 1.6 MeV/c2
Γηcˊ = 16.9 ± 6.4 ± 4.8 MeV
Signal : Significance is larger than 10σ
PRL 109, 042003 (2012)
Experimental challenge : search for photon of 50 MeV.
B( ψˊ→γηcˊ) = (6.8 ± 1.1 ± 4.5)ˣ10-4
CLEO-c < (7.6 ± 1.1) ˣ10-4
PRD81, 052002 (2012)
Found no signal : CLEOc (25M ψˊ)
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Comparison in different production mechanisms:
Belle : PLB 706 139 (2011)
BaBar : PRD 72 031101 (2005)
BaBar : PRD 84 012004 (2011)
Fhnmcn mn mcn bv
BESIII : PRD 87 052005 (2013)
BESIII : PRL 109 042003 (2012)
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Comparison in different production mechanisms:
Belle : PLB 706 139 (2011)
BaBar : PRD 72 031101 (2005)
BaBar : PRD 84 012004 (2011)
Fhnmcn mn mcn bv
BESIII : PRD 87 052005 (2013)
BESIII : PRL 109 042003 (2012)
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Comparison in different production mechanisms:
Belle : PLB 706 139 (2011)
BaBar : PRD 72 031101 (2005)
BaBar : PRD 84 012004 (2011)
Fhnmcn mn mcn bv
BESIII : PRD 87 052005 (2013)
BESIII : PRL 109 042003 (2012)
BESIII will be able to improve mass and width values with more statistic.
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Radiative partial decay widths:
Initial meson J/ψ ψˊ ψˊ
Final meson ηc ηc ηcˊ
2.9 9.7 0.21
1.58 ± 0.37
PDG2014
0.97 ± 0.14
CLEO-c
0.143 ± 0.027 ± 0.092
BESIII
2.51 ± 0.08 0.4 ± 0.8 -------
Finding a procedure to understand interference seems crucial to be able
to extract the exact values.
arXiv:1107.2037v2
Long-standing puzzle on the radiative transition rates of J/ψ and ψˊ→γηc:
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Outlook
precise ηc and ηcˊ studies was done at BESIII:
ψˊ→γηc :
precise measurement on basic properties like mass and width
improving the hyperfine splitting value
considering the interference for the first time
ψˊ→π°hc, hc→γηc
interference free lab for ηc lineshape
promising channel to measure the basic properties of ηc
ψˊ→γηcˊ
first observation even with 106M ψˊ
Nature of interference : More interesting result will come very soon!
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