HADRON 2015 XVI International Conference on Hadron Spectroscopy
![HADRON 2015 XVI International Conference on Hadron Spectroscopy Newport News VA, September 2015 HADRON 2015 XVI International Conference on Hadron Spectroscopy Newport News VA, September 2015](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-1.jpg)
![CHARMONIUM DESCRIPTION FROM A GENERALIZED SCREENED POTENTIAL MODEL P. González Universitat de València and CHARMONIUM DESCRIPTION FROM A GENERALIZED SCREENED POTENTIAL MODEL P. González Universitat de València and](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-2.jpg)
![13 New Neutral Charmonium States since PDG 2000 8 - 9 X (Unconventional) States 13 New Neutral Charmonium States since PDG 2000 8 - 9 X (Unconventional) States](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-3.jpg)
![Conventional States S. Godfrey, N. Isgur PRD 32, 189 (1985) Conventional States S. Godfrey, N. Isgur PRD 32, 189 (1985)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-4.jpg)
![X(4660) X(4350) X(4260) X(3940) DD 1 X(4140 -60) D*D*|(2++) X(3915) DD*(1++) X(3872) DD(0++) X X(4660) X(4350) X(4260) X(3940) DD 1 X(4140 -60) D*D*|(2++) X(3915) DD*(1++) X(3872) DD(0++) X](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-5.jpg)
![Decay properties of some X states very different from conventionally expected. Conventional description: with Decay properties of some X states very different from conventionally expected. Conventional description: with](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-6.jpg)
![What are they ? Hybrid (Quark-Antiquark + Gluon) States ? Molecular Sates ? Tetraquarks What are they ? Hybrid (Quark-Antiquark + Gluon) States ? Molecular Sates ? Tetraquarks](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-7.jpg)
![What is the effect of Meson-Meson Thresholds ? Can we implement threshold effects within What is the effect of Meson-Meson Thresholds ? Can we implement threshold effects within](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-8.jpg)
![INDEX i) Quenched versus Threshold-Unquenched Quark-Antiquark Static Energy from Lattice. Static Potential. ii) Generalized INDEX i) Quenched versus Threshold-Unquenched Quark-Antiquark Static Energy from Lattice. Static Potential. ii) Generalized](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-9.jpg)
![Quenched vs Threshold-Unquenched Quark-Antiquark Energy G. S. Bali, Phis. Rep. 343, 1 (2001) G. Quenched vs Threshold-Unquenched Quark-Antiquark Energy G. S. Bali, Phis. Rep. 343, 1 (2001) G.](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-10.jpg)
![Generalized Screened Potential Model (GSPM) Generalized Screened Potential Model (GSPM)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-11.jpg)
![Cornell potential modulated by thresholds Cornell potential modulated by thresholds](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-12.jpg)
![Possible Shortcomings - Non relativistic potential (effective). - No spin dependent terms in the Possible Shortcomings - Non relativistic potential (effective). - No spin dependent terms in the](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-13.jpg)
![Heavy Quarkonia Description The lowest lying spectrum is described by the Cornell potential Calculated Heavy Quarkonia Description The lowest lying spectrum is described by the Cornell potential Calculated](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-14.jpg)
![Charmonium J++ Thresholds Charmonium J++ Thresholds](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-15.jpg)
![GSPM J++ Spectrum GSPM J++ Spectrum](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-16.jpg)
![X(4350) X(4140 -60) C(4017) X(3915) X(3872) X(4350) X(4140 -60) C(4017) X(3915) X(3872)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-17.jpg)
![Threshold Effect Threshold Effect](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-18.jpg)
![Attraction + Additional States results from the interaction between Additionally a new state appears. Attraction + Additional States results from the interaction between Additionally a new state appears.](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-19.jpg)
![Additional States Additional States](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-20.jpg)
![](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-21.jpg)
![X(4350) X(4140 -60) C(4017) X(3915) X(3872) X(4350) X(4140 -60) C(4017) X(3915) X(3872)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-22.jpg)
![Electromagnetic Decays Electromagnetic Decays](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-23.jpg)
![](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-24.jpg)
![](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-25.jpg)
![](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-26.jpg)
![X(4660) X(4350) X(4260) DD 1 X(4140 -60) C(4017) X(3915) D*D*|(2++) DD*(1++) X(3872) DD(0++) X(4660) X(4350) X(4260) DD 1 X(4140 -60) C(4017) X(3915) D*D*|(2++) DD*(1++) X(3872) DD(0++)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-27.jpg)
![1 -- Thresholds Overlapping Thresholds 1 -- Thresholds Overlapping Thresholds](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-28.jpg)
![S. Godfrey, N. Isgur PRD 32, 189 (1985) Bottomonium G(11020) BB 1 B*B* (2++) S. Godfrey, N. Isgur PRD 32, 189 (1985) Bottomonium G(11020) BB 1 B*B* (2++)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-29.jpg)
![J++ States P. González, J. Phys. G 41 (2014) 095001 J++ States P. González, J. Phys. G 41 (2014) 095001](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-30.jpg)
![](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-31.jpg)
![Summary i) There is a spectral puzzle concerning experimentally unconventional charmonium states. ii) There Summary i) There is a spectral puzzle concerning experimentally unconventional charmonium states. ii) There](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-32.jpg)
![THE END THE END](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-33.jpg)
- Slides: 33
![HADRON 2015 XVI International Conference on Hadron Spectroscopy Newport News VA September 2015 HADRON 2015 XVI International Conference on Hadron Spectroscopy Newport News VA, September 2015](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-1.jpg)
HADRON 2015 XVI International Conference on Hadron Spectroscopy Newport News VA, September 2015
![CHARMONIUM DESCRIPTION FROM A GENERALIZED SCREENED POTENTIAL MODEL P González Universitat de València and CHARMONIUM DESCRIPTION FROM A GENERALIZED SCREENED POTENTIAL MODEL P. González Universitat de València and](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-2.jpg)
CHARMONIUM DESCRIPTION FROM A GENERALIZED SCREENED POTENTIAL MODEL P. González Universitat de València and IFIC (SPAIN)
![13 New Neutral Charmonium States since PDG 2000 8 9 X Unconventional States 13 New Neutral Charmonium States since PDG 2000 8 - 9 X (Unconventional) States](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-3.jpg)
13 New Neutral Charmonium States since PDG 2000 8 - 9 X (Unconventional) States K. A. Olive et al. (PDG) Ch. Phys. C 86, 090001 (2014)
![Conventional States S Godfrey N Isgur PRD 32 189 1985 Conventional States S. Godfrey, N. Isgur PRD 32, 189 (1985)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-4.jpg)
Conventional States S. Godfrey, N. Isgur PRD 32, 189 (1985)
![X4660 X4350 X4260 X3940 DD 1 X4140 60 DD2 X3915 DD1 X3872 DD0 X X(4660) X(4350) X(4260) X(3940) DD 1 X(4140 -60) D*D*|(2++) X(3915) DD*(1++) X(3872) DD(0++) X](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-5.jpg)
X(4660) X(4350) X(4260) X(3940) DD 1 X(4140 -60) D*D*|(2++) X(3915) DD*(1++) X(3872) DD(0++) X states : Close-below or Above their First S-wave M-M Threshold
![Decay properties of some X states very different from conventionally expected Conventional description with Decay properties of some X states very different from conventionally expected. Conventional description: with](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-6.jpg)
Decay properties of some X states very different from conventionally expected. Conventional description: with parallel properties to However strong decay properties completely different Conventional description: However or aan order of magnitude higher than expected
![What are they Hybrid QuarkAntiquark Gluon States Molecular Sates Tetraquarks What are they ? Hybrid (Quark-Antiquark + Gluon) States ? Molecular Sates ? Tetraquarks](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-7.jpg)
What are they ? Hybrid (Quark-Antiquark + Gluon) States ? Molecular Sates ? Tetraquarks (compact states) ? Quark-Antiquark + Molecular States ?
![What is the effect of MesonMeson Thresholds Can we implement threshold effects within What is the effect of Meson-Meson Thresholds ? Can we implement threshold effects within](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-8.jpg)
What is the effect of Meson-Meson Thresholds ? Can we implement threshold effects within a quark-antiquark model framework? Quark-Antiquark effective potential description implicitly incorporating molecular components. P. G. : J. Phys. G 41, 095001 (2014), Phys. Rev. D 92, 014017 (2015)
![INDEX i Quenched versus ThresholdUnquenched QuarkAntiquark Static Energy from Lattice Static Potential ii Generalized INDEX i) Quenched versus Threshold-Unquenched Quark-Antiquark Static Energy from Lattice. Static Potential. ii) Generalized](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-9.jpg)
INDEX i) Quenched versus Threshold-Unquenched Quark-Antiquark Static Energy from Lattice. Static Potential. ii) Generalized Screened Potential Model (GSPM). iii) Heavy Quarkonia Spectral Description from the GSPM. iv) Summary.
![Quenched vs ThresholdUnquenched QuarkAntiquark Energy G S Bali Phis Rep 343 1 2001 G Quenched vs Threshold-Unquenched Quark-Antiquark Energy G. S. Bali, Phis. Rep. 343, 1 (2001) G.](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-10.jpg)
Quenched vs Threshold-Unquenched Quark-Antiquark Energy G. S. Bali, Phis. Rep. 343, 1 (2001) G. S. Bali et al. , PRD 71, 11453 (2005)
![Generalized Screened Potential Model GSPM Generalized Screened Potential Model (GSPM)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-11.jpg)
Generalized Screened Potential Model (GSPM)
![Cornell potential modulated by thresholds Cornell potential modulated by thresholds](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-12.jpg)
Cornell potential modulated by thresholds
![Possible Shortcomings Non relativistic potential effective No spin dependent terms in the Possible Shortcomings - Non relativistic potential (effective). - No spin dependent terms in the](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-13.jpg)
Possible Shortcomings - Non relativistic potential (effective). - No spin dependent terms in the Cornell potential. - Only screening from meson-meson channels. - No thresholds widths. - No accumulative effect from degenerate thresholds. Applicability: non degenerate isolated thresholds
![Heavy Quarkonia Description The lowest lying spectrum is described by the Cornell potential Calculated Heavy Quarkonia Description The lowest lying spectrum is described by the Cornell potential Calculated](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-14.jpg)
Heavy Quarkonia Description The lowest lying spectrum is described by the Cornell potential Calculated masses for the lowest lying spin triplet states differing at most 30 Me. V (60 Me. V) for bottomonium (charmonium).
![Charmonium J Thresholds Charmonium J++ Thresholds](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-15.jpg)
Charmonium J++ Thresholds
![GSPM J Spectrum GSPM J++ Spectrum](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-16.jpg)
GSPM J++ Spectrum
![X4350 X4140 60 C4017 X3915 X3872 X(4350) X(4140 -60) C(4017) X(3915) X(3872)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-17.jpg)
X(4350) X(4140 -60) C(4017) X(3915) X(3872)
![Threshold Effect Threshold Effect](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-18.jpg)
Threshold Effect
![Attraction Additional States results from the interaction between Additionally a new state appears Attraction + Additional States results from the interaction between Additionally a new state appears.](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-19.jpg)
Attraction + Additional States results from the interaction between Additionally a new state appears. and the Cornell state
![Additional States Additional States](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-20.jpg)
Additional States
![](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-21.jpg)
![X4350 X4140 60 C4017 X3915 X3872 X(4350) X(4140 -60) C(4017) X(3915) X(3872)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-22.jpg)
X(4350) X(4140 -60) C(4017) X(3915) X(3872)
![Electromagnetic Decays Electromagnetic Decays](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-23.jpg)
Electromagnetic Decays
![](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-24.jpg)
![](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-25.jpg)
![](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-26.jpg)
![X4660 X4350 X4260 DD 1 X4140 60 C4017 X3915 DD2 DD1 X3872 DD0 X(4660) X(4350) X(4260) DD 1 X(4140 -60) C(4017) X(3915) D*D*|(2++) DD*(1++) X(3872) DD(0++)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-27.jpg)
X(4660) X(4350) X(4260) DD 1 X(4140 -60) C(4017) X(3915) D*D*|(2++) DD*(1++) X(3872) DD(0++)
![1 Thresholds Overlapping Thresholds 1 -- Thresholds Overlapping Thresholds](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-28.jpg)
1 -- Thresholds Overlapping Thresholds
![S Godfrey N Isgur PRD 32 189 1985 Bottomonium G11020 BB 1 BB 2 S. Godfrey, N. Isgur PRD 32, 189 (1985) Bottomonium G(11020) BB 1 B*B* (2++)](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-29.jpg)
S. Godfrey, N. Isgur PRD 32, 189 (1985) Bottomonium G(11020) BB 1 B*B* (2++) BB (0++) BB* (1++)
![J States P González J Phys G 41 2014 095001 J++ States P. González, J. Phys. G 41 (2014) 095001](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-30.jpg)
J++ States P. González, J. Phys. G 41 (2014) 095001
![](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-31.jpg)
![Summary i There is a spectral puzzle concerning experimentally unconventional charmonium states ii There Summary i) There is a spectral puzzle concerning experimentally unconventional charmonium states. ii) There](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-32.jpg)
Summary i) There is a spectral puzzle concerning experimentally unconventional charmonium states. ii) There is a plausible explanation for this puzzle based on an Energy Dependent Quark-anti. Quark Potential from threshold effects. iii) The Generalized Screened Potential Model (GSPM) based on this potential allows for a reasonable spectral description of J++ charmonium. iv) New higher energy states in charmonium and bottomonium are predicted.
![THE END THE END](https://slidetodoc.com/presentation_image/cb24a3a85db979dda3857f4305d3b02f/image-33.jpg)
THE END
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