Some predictions of diquark model for hidden charm pentaquark discovered at the LHCb

The LHCb has discovered two new states with preferred JP quantum numbers 3/2− and 5/2+ from Λb decays. These new states can be interpreted as hidden charm pentaquarks. It has been argued that the main features of these pentaquarks can be described by diquark model. The diquark model predicts that the 3/2− and 5/2+ are in two separate octet multiplets of flavor SU(3) and there is also an additional decuplet pentaquark multiplet. Finding the states in these multiplets can provide crucial evidence for this model. The weak decays of b-baryon to a light meson and a pentaquark can have Cabibbo allowed and suppressed decay channels. We find that in the SU(3) limit, for U-spin related decay modes the ratio of the decay rates of Cabibbo suppressed to Cabibbo allowed decay channels is given by |Vcd|2/|Vcs|2. There are also other testable relations for b-baryon weak decays into a pentaquark and a light pseudoscalar. These relations can be used as tests for the diquark model for pentaquark.


Introduction
The LHCb collaboration has recently discovered two new states [1] which can be interpreted as two different pentaquarks P from Λ b → P + K, followed by P → J/ψ + p. This has generated a lot of theoretical investigations [2][3][4][5][6][7][8][9][10][11][12][13][14][15]. The quark contents can be identified asccuud. Although the states contain charm quarks, they are hidden charm pentaquarks because c andc appear together and the net charm quantum number is zero. The best fit quantum numbers J P and their masses are J P = 3/2 − with a mass of 4380 MeV, and J P = 5/2 + with a mass of 4450 MeV .
The existence of these states P c (4380) and P c (4450) need to be further confirmed as there may be some other effects which can minic similar effects [8,11,13]. If these states are genuine pentaquarks, one may ask whether they are molecular states of two hadrons or composite hadron systems [2-5, 7, 10, 14], or a tightly bound five quark system [ccqq ′ q ′′ ], or the quarks bound in other forms [9,12,15]. It is intriguing that the Σ cD * in the S-wave state has a mass very close to the P c (4450). Such a molecular state was actually studied just before the experimental discovery [2]. With Σ cD * and Σ * cD * bound sates one can obtain both P c (4380) and P c (4450) states [3]. These prompt the speculation that the pentaquarks might be molecular states. On the other hand, it has been argued that the two pentaquarks from the LHCb are five quark systems organized in [q ′ q ′′ ] and [cq] diquarks [9], and thec, the diquark model for pentaquark. The diquark model also has supports from tetraquark studies [9]. At present, with limited data it is not possible to distinguish whether the pentaquarks are molecular states or more tightly bound quark states or even mixture of these states. The diquark model has simple structure to analysis. We also find it very predictive. Therefore in this work we choose to study some properties of diquark model for the pentaquarks discovered at the LHCb.

JHEP12(2015)128 2 Diquark model for pentaquarks
In the diquark model the two pentaquarks from the LHCb are five quark systems organized in [q ′ q ′′ ] and [cq] diquarks [9], and thec. More explicitly indicated as the following P = ǫ αβγ {c α [cq] β, s=0,1 [q ′ q ′′ ] γ, s=0,1 , L} (2.1) where the greek letters are color indices and s indicates the spin. Under flavor SU(3) symmetry, the diquark [q ′ q ′′ ] transforms as3 and 6 and the diquark [cq] transforms as a 3. Therefore the pentaquarks can have 3 ×3 = 1 + 8 and 3 × 6 = 8 + 10 multiplets. We indicate the pentaquarks with3 and 6 by P A and P S , respectively. Assuming that the two pentaquarks have J P = 3/2 − and J P = 5/2 + , these two fields are component fields in octet multiplets with the following spin diquark combinations fit the picture well [9] We denote the octet pentaquark component fields as For J P = 3/2 − , there should also be a decuplet P ijk (totally symmetric in sub-indices) multiplet. The component pentaquark fields are The two observed pentaquarks are identified as p 8 (3/2 − ) and p 8 (5/2 + ), respectively. It is clear that there are other members of pentaquarks. Similar to the decay channels p 8 (3/2 − , 5/2 + ) → J/ψ + p, the pentaquarks in the octet and decuplet will be able to decay into a J/ψ plus baryons in the low-lying octet and decuplet, respectively. For J P = 5/2 + , there should be a companion singlet pentaquark S. However, there is no low-lying baryon singlet, S will not be able to decay into a J/ψ plus an ordinary low-lying baryon, but may be an ordinary baryon and multi-mesons forming a SU(3) singlet. The masses of the pentaquarks are degenerate in the SU(3) limit. But may be different due to s-quark mass being much larger than u-and d-quarks. Estimate of mass differences for some of the pentaquarks in the diquark model has been carried out in ref. [15]. Discoverying these additional pentaquarks identified above is one of the way to verify the diquark model for pentaquark which can in principle be carried out at the LHCb.

JHEP12(2015)128 3 Pentaquark weak decays
We now discuss weak decay modes of b-baryon into an octet or a decuplet pentaquark and a light pseudoscalar octet meson. The leading effective Hamiltonian inducing B → M + P decays in the SM has both parity conserving and violating parts given by where q can be d or s. V ij is the CKM matrix element. The coefficients c 1,2 are the Wilson Coefficients (WC) which have been studied by several groups and can be found in ref. [16]. The operators O i are given by where (āb) V ±A =āγ µ (1±γ 5 )b. In the above, we have neglected contributions from penguin diagrams since they are significantly smaller than the tree contributions given above.
For q = s, the decay amplitude is proportional to V cs , which we refer to as Cabibbo allowed interaction. For q = d, the decay amplitude is proportional to V cd , which is Cabibbo suppressed interaction.
The low-lying  [17]. The anti-triplet B and the sextet C b-baryons will be indicated by The pseudoscalar octet mesons will be indicated by M. They are At the hadron level, the decay amplitude can be generically written as

JHEP12(2015)128
To obtain the SU(3) invariant decay amplitude for a b-baryon, one first uses the Hamiltonian to annihilate the b-quark in B (or C) and then contract SU(3) indices in an appropriate way with final states P and M. Taking the anti-triplet tree amplitude T t (q) and sextet tree amplitude T s (q) as examples, following the procedures for b-baryon charmless two-body decays in ref. [18,19], we have and The SU(3) invariant decay amplitude involving decuplet pentaquarks can be written as For B baryons decay into P, there are six possible terms as far as SU (3) properties are concerned. The dominant contributions are from terms with coefficients c t (3), d t (3), e t (3) and f t (3). In figure 1, we show diagrams corresponding to these terms. In these figures, the quarks q i , q i ′ and q i ′′ are contracted by the totally antisymmetric tensor ǫ ii ′ i ′′ or ǫ ii ′ i ′′ . This property plays an important role in determining whether3 or sextet diquarks are allowed to form. The two terms with coefficients a t (3) and b t (3) are allowed, but it turns out that for these two terms the P state is actually a higher order fork state with the same SU(3) quantum numbers but with more quark contents as can be seen in figure 2. Therefore, one expects that the coefficients a t (3) and b t (3) to be smaller than c t (3), d t (3), e t (3) and f t (3). We will include all in our later discussions. For the properties we emphasis will not be affected whether to include a t (3) and b t (3) or not.
For C baryons decay into P, there are only three possible terms, terms with coefficients, d s (3), e s (3) and f s (3). The corresponding diagrams are shown in figure 1.b, 1.c, and 1.d. Because the two light quarks in C are symmetric, similar terms to those with coefficients For B and C baryons decay into decuplet, the final light quarks need to be in totally symmetric state. There are less possibilities. In figure 3 we show the corresponding diagrams for the allowed terms.
In the above, we have suppressed the Lorentz indices and spinor forms, but concentrated in SU(3) flavor indices. The results apply to 3/2 − and also 5/2 + multiplets. Expanding the above amplitudes, one can obtain the individual decay amplitude. The full expansions are given in the appendices. From these results, one can read off many properties concerning weak decays of b-baryons to a pentaquark and a light pseudoscalar. We present some of the interesting properties in the following.

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corresponds to the term with coefficients e t (3) and e s (3). Possible 3 diquarks can be formed by In the above two figures, the quarks q i ′ q i ′′ are in3 flavor state. (a) corresponds to the term with coefficient a t (3). Possible 3 diquarks can be formed by (q i q i ′ ), (q i q i ′′ ) and (q i ′ q i ′′ ) pairs. The P k l can be viewed as a singlet pentaquark formed by ccq i q i ′ q i ′′ bounded with an octet (q k q l ) state. (b) corresponds to the term with coefficient b t (3). Possible 3 diquarks can be formed by (q i q i ′ ), (q i q i ′′ ) and (q i ′ q i ′′ ) pairs. The P k j can be viewed as a pentaquark formed by ccq i ′ q i ′′ q i bounded with an octet (q k q j ) state. In figures 2.a and 2.b the P states having the same quantum number as the LHCb observed pentaqaurk are higher order fork states. The corresponding coefficients a t (3) and b t (3) are expected to be smaller than c t (3). Figure 3. (a) corresponds to the term with coefficients a t10 and a s10 . Possible sextet diquarks can be formed by (q j q k ), (q j q l ) and (q k q l ) pairs. (b) corresponds to the term with coefficient b s10 . Possible sextet diquarks can be formed by (q i q j ), (q i q k ) and (q j q k ) pairs. related to these two pentaquarks. But within each multiplet with the same J P , there are relations which can be tested experimentally. We find the U -spin related amplitudes (∆S = 0 and ∆S = −1) for anti-triplet satisfy the following relations

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While the U -spin related amplitudes for sextet satisfy The above relations can be directly read off from the diagrams shown in figures 1 and 2 when specific quarks are assigned for each decay modes. For illustrations we take the pairs a).
Note that for each pairs one just needs to exchange all s quarks with all d quarks to go from one to another within a given pair. If U spin is a good symmetry, the amplitudes defined in eq.15 and eq.16 are therefore equal in magnitude. The relative minus sign for the amplitude in each pair in eq.15 and eq.16 comes from the fact that each diagram is contracted by ǫ ii ′ i ′′ and ǫ ii ′ i ′′ for B and C decays, respectively. For the pair in a), (i = 3, i ′ = 1, i ′′ = 2) and (i = 2, i ′ = 1, i ′′ = 3) for Ξ 0 b and Λ 0 b decays, and for the pair in b), (i = 1, i ′ = 2, i ′′ = 3) and (i = 1, i ′ = 3, i ′′ = 2) for Ω − b and Σ − b decays, respectively. These specific values for i, i ′ and i ′′ explain the relative minus sign in the relations.
The above relations also hold even one include small penguin contributions [18,19]. These relations apply to both octets with J P = 3/2 − and J P = 5/2 + . Due to mixing between η 8 and η 1 , the decay modes with η 8 in the final sates is not as clean as those with π and K in the final state to study. We have not listed processes involve η 8 above.
The above relations lead to the following relations for each pairs above, When more data become available, with more pentaquarks discovered, the above relations can be tested. To study the Cabbibo suppressed decays, 20 times more data are needed.
and for ∆S = −1 amplitudes, we have

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Since there is only one unknown invariant amplitude a t10 , all ∆S = −1 decays are related among themselves. Also for ∆S = 0 decays. There are also relations between ∆S = −1 and ∆S = 0 decays. For example, indicating the decay width of Λ 0 and Similar one can work out relations for Ξ 0,− decays.
With more data from LHCb, these relations can be tested and provide important information for diquark model for pentaquark.
The b-baryon Ω − b is a member in the sextet C. Expanding the second equation in eq. (3.9), we obtain, for ∆S = 0 amplitudes, and, for ∆S = −1 amplitudes, (4.10) Since there are two invariant amplitudes, a s and b s , there are no simple relations for ∆S = 0 and ∆S = −1 amplitudes, but within each of them, there are direct simple relations and can be tested. We have In summary, we have studied some properties of the diquark model for explanations of the 3/2 − and 5/2 + pentaquarks discovered at the LHCb. In the diquark model, these two pentaquarks are in octet multiplets of flavor SU(3). There is also an additional decuplet pentaquark multiplet and a singlet pentaquark. Finding the states in these multiplets can provide crucial evidence for this model. The weak decays of b-baryon to a light meson and a pentaquark can have Cabibbo allowed and suppressed decay channels. We find that in JHEP12(2015)128 the SU(3) limit, for U -spin related decay modes the ratio of the decay rates of Cabibbo suppressed to Cabibbo allowed decay channels is given by |V cd | 2 /|V cs | 2 . There are also other testable relations for b-baryon weak decays. These relations can be used as tests for the diquark model for pentaquark.

Acknowledgments
The work was supported in part by MOE Academic Excellent Program (Grant No: 102R891505) and MOST of ROC, and in part by NSFC (Grant No: 11175115) and Shanghai Science and Technology Commission (Grant No: 11DZ2260700) of PRC.

JHEP12(2015)128 B SU(3) amplitudes for an sextet decays into a decuplet pentaquark
For ∆S = 0 amplitudes, we have Open Access. This article is distributed under the terms of the Creative Commons Attribution License (CC-BY 4.0), which permits any use, distribution and reproduction in any medium, provided the original author(s) and source are credited.