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Mitja Rosina THE BINDING ENERGY OF THE Ξcc++ BARYON

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Presentation on theme: "Mitja Rosina THE BINDING ENERGY OF THE Ξcc++ BARYON"— Presentation transcript:

1 Mitja Rosina THE BINDING ENERGY OF THE Ξcc++ BARYON
AND THE DD* DIMESON Mitja Rosina Faculty of Mathematics and Physics, University of Ljubljana and Institute Jožef Stefan, Ljubljana, Slovenia Talk presented at the Mini-Workshop BLED, June, 2018 DOUBLE-CHARM BARYONS AND DIMESONS OUR ESTIMATE: m( Ξcc++ ) ≥ or MeV LHCb: m( Ξcc++ ) = 3621 MeV SELEX: m( Ξcc+ ) = 3519 MeV

2 DECAY CHANNELS: c → s LHCb: m( Ξcc++ ) = 3621 MeV
Ξcc++ → Λc+ + K- + π+ + π+ , Λc+ → p + K- + π+ ccu → cud + su + ud + ud SELEX: m( Ξcc+ ) = 3519 MeV Ξcc+ → Λc+ + K- + π+ Ξcc+ → D+ + p + K-

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5 or PHENOMENOLOGICAL ESTIMATE OF THE Ξcc++ MASS u u u b c c c
like D0 meson ( ) MeV like B+ meson ( ) MeV m (c) = MeV m (b) = 5259 MeV m (cc) = MeV m (ccu) = m(D0) - m(c) + m(cc) m (ccu) = m(B+) - m(b) +m(cc) = =3532 MeV = =3557 MeV

6 Vcc = 1 2 Vcc The „Vqq = Vqq ‘‘ rule for diquark meson
12 Vcc = Vcc [A]: (color.color)=4/3 for cc =2/3 for cc [B]: Flux tube model c c c c c

7 𝑝2 2(𝑐/2) +𝑉𝑐𝑐 𝜓 = Ecc 𝜓 𝑝2 2(𝑐/2) + 𝑉𝑐𝑐 𝜓 = 1 2
The „Vqq = Vqq ‘‘ rule for diquark meson 12 𝑝2 2(𝑐/2) +𝑉𝑐𝑐 𝜓 = Ecc 𝜓 𝑝2 2(𝑐/2) + 𝑉𝑐𝑐 𝜓 = 1 2 𝑝𝟐 2(𝑐/4) +𝑉𝑐𝑐 𝜓 = Ecc 𝜓 Ecc = F(c/2) Ecc = F(c/4) notation: particle symbols mean their masses

8 The finite size of the diquark and the extra Coulomb repulsion would raise the mass a little.
The estimate (≥ or MeV) is then not too far from the experimental value MeV. It is considerably above the SELEX value 3519 MeV, but it does not exclude it.

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10 BINDING ENERGY OF THE DD* „MOLECULE“
The nonrelativistic calculation of Janc & Rosina (2004) Used the one-gluon exchange potential (including the chromomagnetic term) + the linear confining potential. The model parameters fitted all relevant mesons and baryons. Janc & Rosina : (DD*) – (D + D*) = MeV (Bhaduri ) - 2.7 MeV (Grenoble AL1) Important questions: 1. How much is binding for other interactions? 2. Can the pion cloud between the u and d antiquarks (the DD*π or DD*ππ configuration) increase binding ? 3. How much does relativity change binding?

11 MOTIVATION Effective quark-quark interaction: Is Vuu = Vcu = Vcc = Vcc = Vbu = Vbb = Vbb (apart from the mass-dependent spin-spin term) ? Interesting 4-body problem, to understand binding and to forsee the production and detection mechanisms. CHALLENGE: New chances to measure LHC and DD*=(cu+cd) at the upgraded KEK (Tsukuba, Japan).

12 COMPARISON BETWEEN DIMESON AND HYDROGEN MOLECULE POTENTIAL
V rcc u cc c c c D + D* d

13 PHENOMENOLOGICAL ESTIMATE OF DIMESON BINDING
u u b u bb b b d b d d Dimeson B+B* ( =10604)MeV like Λb antibaryon ( )MeV Tetraquark u u c u c c cc d c d d like Λ c antibaryon ( )MeV Dimeson D+D* ( =3875)MeV Tetraquark

14 Is the D+D* dimeson bound?
In the restricted 4-body space assuming "cc" in a bound diquark state + general wavefunction of u and d, the energy is above the D+D* threshold. In the restricted "molecular" 4-body space assuming the two c quarks far apart + general wavefunction of ubar and dbar (as assumed by several authors), the energy is also above the D+D* threshold. Only combining both spaces (we took a rich 4-body space) brings the energy below the threshold.

15 Gaussian basis with Jacobi coordinates

16 The nonrelativistic calculation of Janc & Rosina (2004)
Used the one-gluon exchange potential (including the chromomagnetic term) + the linear confining potential. The model parameters fitted all relevant mesons and baryons. A rich 4-body space was used (an s-state Gaussian expansion at optimized distances, with 3 types of Jacobi coordinates in order to mimic also the p-states). (DD*) – (D + D*) = MeV (Bhaduri ) - 2.7 MeV (Grenoble AL1) Can the pion cloud between the u and d antiquarks increase binding, in analogy with the deuteron ? At a distance of 0.5 fm the two-pion-exchange interaction between the D and D* mesons might bring additional 50 MeV??

17 A note on analogy between DD* and DD*
We failed to calculate the energy of X(3872) using the same method and interaction as for DD*, [Bled Proceedings 2005]. The reason is that a perfect variational calculation in a rather complete 4-body space finds the absolute minimum of energy which correspnds to J/psi+eta rather than DD* A demanding coupled channel calculation would be needed for a reliable result, and we have posponed it.


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