# Towards the Assignment for the Ground Scalar Meson

Authors: Xue-Chao Feng; Peng Chen; Ji-Min Shang
Journal: Advances in High Energy Physics
 (2013)

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## Abstract

Combining three complementary approaches, nonrelativistic constituent quark model, Regge phenomenology, and meson-meson mixing, we obtain the mass relations which relate different meson multiplets. With the help of known meson masses, these relations can be used for the prediction of unknown meson states masses. The utility of this new analysis technique is applied for the scalar meson and results in a possible allocation scheme for the ground scalar meson.


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## Body

## 1. Introduction

It is well known that the strong interactions are described by the non-Abelian gauge field theory quantum chromodynamics (QCD). However, we are still far from deriving the spectrum of mesons from first principles so far. Therefore, the phenomenological analysis of meson states is important for the hadronic physics [1–3].The study of scalar mesons plays an important role in particle physics. The scalar mesons with vacuum quantum numbers could provide a full understanding of the symmetry breaking mechanisms in QCD and the confinement [4]. Moreover, scalar mesons are very important intermediate state in Goldstone boson interactions away from threshold, where chiral perturbation theory is not applicable [5]. Therefore, the investigation of scalar mesons becomes an attention focus in theory and experiments [5–13]. Nevertheless, the interpretation of the nature of scalar mesons is a long-standing problem of particle physics to this day. According to the new edition of Particle Data Group (PDG), for the light quark sector, the number of resonances found in experiment below 2GeV exceeds the number of states that conventional quark models can accommodate [14]. There are ten resonances are observed in the experiments, including the isoscalar resonances f0(600), f0(980), f0(1370), f0(1500), and f0(1710), the isovector resonances a0(980), and a0(1450), and the isodoublet resonances K0*(1430), K0*(800), and K0*(1950). Up to now, none of the ten reported scalar states can be definitely assigned as ground scalar nonet members. Considering that some resonances cannot be explained by the conventional qq- quark model, different theoretical models have also been established such as KK- molecule [15], MIT bag model [16], QCD sum rules [17], and chiral Lagrangians [18]. For the heavy-light quark meson, two resonances, DSJ*(2317) and D0*(2400), are observed in the experiments. The resonances DSJ*(2317) with a mass 2317.8±0.6MeV and width 349.3±0.6MeV are assigned as charm-strange meson of scalar state. However, the experimental value is considerably smaller than the results in many theoretical predictions [19, 20]. The disagreement results in the different interpretations about the DSJ*(2317) such as the molecule state [21], the four-quark state [22], or the Dπ atom [23]. On the other hand, considering the fact that the mass DSJ*(2317) is smaller than its partner D0*(2400), we also argue that the assignment of the DSJ*(2317) needs further tests in the experiments.In the present work, based on the relations derive from three complementary approaches, nonrelativistic constituent quark model, Regge phenomenology, and meson-meson mixing, we investigate the scalar meson mass spectrum and propose a possible assignment for the ground scalar meson nonet.


## 2. Nonrelativistic Constituent Quark Model for Scalar Meson

In the framework of the non-relativistic constituent quark model, one typically assumes that theqq- wave functions are a solution of a non-relativistic Schrödinger equation with the Breit-Fermi Hamitonian H [24–26], which contain
(1)Hψn(r)=(mq+mq-+mq+mq-2mqmq-p2→-(mq3+mq-38mq3mq-3)p4→=+VNR(r)+HLS+SS+T(mq3+mq-38mq3mq-3))ψn(r)
with
(2)VNR(r)=Vv(r)+Vs(r),HLS+SS+T=HLS+HSS+HT,
where mq and mq- are the constituent quark masses, VNR is the confining potential consisting of vector, and scalar contributions, HLS, HSS, and HT, are the spin-spin, spin-orbit, and tensor terms, respectively. Following, we apply the Breit-Fermi Hamitonian to the S-wave and P-wave meson multiplets.For the S-wave mesons, consider the fact the matrix element of the tensor and spin-orbit interactions vanishes, one arrive at the following relation:(3)M=mq+mq-+a0+e0〈SqSq-〉mqmq-.Sq and Sq- are the constituent quark spins, and e0 is the spin-spin interaction coefficient. The constant a0 is small compared to the constituent quark masses mq and mq- and may be absorbed into the constituent quark masses [24, 29, 30]. Therefore, the relation (3) can be expressed as
(4)M=mq+mq-+e0〈SqSq-〉mqmq-.For theP-wave mesons, the phenomenological form of the matrix element of the Breit-Fermi Hamitonian has the following relation:
(5)M=mq+mq-+a1+b1(1mq+1mq-)+c1(1mq2+1mq-2)+d1mqmq-+g1[(mq+mq-)2+2mqmq-4mq2mq-2〈L·S〉g1cccc-mq2-mq-24mq2mq-2〈L(Sq-Sq-)〉(mq+mq-)24mq2mq-2]+e1〈SqSq-〉mqmq-+f1(1mq3+1mq-3)+h1a(j,1)mqmq-
with
(6)a(j,1)=45〈S2L2-32(LS)-3(LS)2〉,〈LS〉=12[j(j+1)-3S-2],
where a1, b1, c1, d1, e1, f1, g1, and h1 are the constants, and the angular momentum parts of the matrix elements are shown in Table 1. With the help of the parameters in Table 1, from the relations (4) and (5), we obtain the following formulas:
(7)Mπ+3Mρ2MK+6MK*-Mπ-3Mρ=mnms,(8)Mss-(13P2)-Mss-(13P0)Mnn-(13P2)-Mnn-(13P0)=(mnms)2,
where Mnn- is the mass of isovector state, Mss- refers to the mass of the bare strange member of the isoscalar states, and ms and mn (n stands for nonstrange u- and d-quark) are the corresponding constituent quark masses. In view of relation (8), we can obtain the scalar mesons masses from the masses of other meson states, which quark model assignment is firmly established. Due to the isovector meson act as a beacon for the mass scales of meson nonet, we should firstly determine the mass of isovector state. In the following section, we are going to calculate the mass of isovector states in the framework of Regge phenomenology and mass mixing matrix.Table 1
Angular momentum part of the matrix elements of relations (4) and (5).
n
2
s
+
1
l
J
1
1
S
0
1
3
S
1
1
3
P
2
1
3
P
0
〈
L
S
〉
1
−2
a
(
j
,
1
)
−2/5
−4
〈
S
q
S
q
-
〉
−3/4
1/4
1/4
1/4
〈
L
(
S
q
-
S
q
-
)
〉
0
0


## 3. Mass Mixing Matrix of Isoscalar States

In the quark model, mesons areqq′- bound states of quark q and antiquark q′-. Three light flavors of quarks -u, -d, and -s combined with three antiquarks yield nine meson nonet, which contain two bare isoscalar states. In general, the two bare isoscalar states can mix, which result in two physical isoscalar states. Therefore, the mix of isoscalar states is important for the meson, due to providing a clue for the assignment of a resonance in a meson nonet.In the nonstrangeN=(uu-+dd-)/2 and strange S=ss- basis, the mass-squared matrix describing the mixing of the two physical isoscalar states can be written as [31]
(9)M2=(MN2+2A2AX2AXMss-2+AX2),
where MN and Mss- are the masses of bare states N and S, respectively; A are the mixing parameters which describe the qq-↔q′q′-  transition amplitudes. The X that is a phenomenological parameter describes the SU(3) broken ratio of the nonstrange (u- and d-quark) and strange quark propagators via the constituent quark mass ratio. The value of X is determined to be 0.63 by inserting the corresponding masses into relation (7) [29]. Here and below, all the masses used as input for our calculation are taken from PDG [14].In the meson nonet, the physical isoscalar statesφ and φ′ are the eigenstates of mass-squared matrix M2, as well as the square masses Mφ2 and Mφ′2 are the eigenvalues, respectively. The physical states φ and φ′ can be related to the ss- and N=(uu-+dd-)/2 by
(10)(phy1phy2)=U(NS)
and the unitary matrix U can be described as
(11)UM2U†=(Mphy1200Mphy22).The mix of the physical isoscalar states can be also described as(12)(phy1phy2)=(cosθ-sinθsinθcosθ)(φ8φ1)
with
(13)φ1=(uu-+dd-+ss-)3,φ8=(uu-+dd--2ss-)6,
where θ is the nonet mixing angle.From the relations (9), (10), (11), and (12), one will obtain
(14)U=(cosθ-sinθsinθcosθ)(13-232313).Based on the relations (9) and (11), one can have the following relations:
(15)MN2+2A=(13cosθ-23sinθ)2Mphy12+(23cosθ+13sinθ)2Mphy22,Mss-2+AX2=(13cosθ-23sinθ)2Mphy22+(23cosθ+13sinθ)2Mphy12.Applying the relations (15) for the meson states 11S0, 13S1, 13P2, 13D3, and 21S0, we obtain the bare ss- member masses, and the results are present in Table 2. Here and below, all the masses and the mixing angle used as input for our calculation are taken from the PDG [14].Table 2
Predicted mass of baress- for meson nonet. θquad is the nonet mixing angle from the quadratic mass formulae [14].
Nonet
1
1
S
0
1
3
S
1
1
3
P
2
1
3
D
3
2
1
S
0
M
s
s
- (MeV)
Present work
685
1018
1530
1858
1323
[27]
697
1009
1546
[28]
702
1010
1538
[19]
960
1020
1530
1900
1630
θ
quad (°)
−11.5
38.7
29.6
32
−22.4


## 4. Regge Phenomenology and Mass of Isovector Scalar Meson

Regge phenomenology is widely used for the calculation of the meson and baryonium spectrum [28, 36–38]. In [28], Li et al. indicate that the quasi-linear Regge trajectories could provide a reasonable description for the meson mass spectrum. Anisovich et al. also conclude that the meson states can fit to the quasi-linear Regge trajectories at the (N, M2) and (J, M2) planes with good accuracy [36]. In the last decade, Regge trajectories are reanalysis to make predictions for the masses of states not yet to be discovered in experiment or to determine the quantum numbers of the newly discovered states.Based on the assumption that the hadrons with identicalJPC quantum numbers obey quasi-linear form of Regge trajectories, one have the following relations [28]:
(16)l=αii′-(0)+αii′-′Mii′-2,l=αij′-(0)+αij′-′Mij′-2,l=αjj′-(0)+αjj′-′Mjj′-2,
where ii′- denotes the quark and antiquark flavors, and l and Mii′- are the orbital momentum and mass of the ii′- meson. The parameters αii′-′ and αii′-(0) are, respectively, the slope and intercept of the Regge trajectory. The intercepts and slopes can be expressed by [28, 39]
(17)αii-(0)+αjj-(0)=2αij-(0),(18)1αii′-′+1αjj′-′=2αij′-′.The relation (17) is satisfied in two-dimensional QCD [40], the dual-analytic model [41], and the quark bremsstrahlung model [42]. The relation (18) is deprived from the topological and the qq--string picture of hadrons [43]. Recently, based on the available data for mesonic resonances of light, medium, and heavy flavors, Filipponi et al. [44] and Burakovsky and Goldman [45] construct different form slopes (19) of linear Regge trajectories for all quark flavors. One has the following:
(19)αij-′=0.9GeV-21+0.22((mi+mj)/GeV)3/2,αij-′=α′π/4+(π/4)α′(mi+mj)/2.
According to the relations (19), we find the slope of Regge trajectory depends on the constituent quark masses through the combination (mi+mj). The relations (19) are obtained by fitting experimental data, and these relations are possible to update with the increasing amount of experimental data. In the present work, we adopt the assumption presented by [28, 31, 46] that the slopes of the parity partners (e.g., the 0+, 1-, 2+, and 1- are parity partners) trajectories coincide, and further, that the slopes do not depend on charge conjugation in accordance with the C-invariance of QCD. Under this assumption, the corresponding slopes of the 13P2 are the same as those of the 13P0 trajectories, and we have the following relations:
(20)1+M2(13P0)nn-M2(13P2)ns--M2(13P0)ns-M2(13P2)ss-M2(13P0)ns-M2(13P2)ss--M2(13P0)ss-M2(13P2)ns-=4M2(13P0)nn-M2(13P2)ns--4M2(13P0)ns-M2(13P2)ss-M2(13P0)nn-M2(13P2)ss--M2(13P0)ss-M2(13P2)nn-,1+M2(13P0)cc-M2(13P2)cn--M2(13P0)cn-M2(13P2)nn-M2(13P0)cs-M2(13P2)nn--M2(13P0)nn-M2(13P2)cn-=4M2(13P0)cc-M2(13P2)cn--4M2(13P0)cn-M2(13P2)nn-M2(13P0)cc-M2(13P2)nn--M2(13P0)nn-M2(13P2)cc-,1+M2(13P0)cc-M2(13P2)cs--M2(13P0)cs-M2(13P2)ss-M2(13P0)cs-M2(13P2)ss--M2(13P0)ss-M2(13P2)cs-=4M2(13P0)cc-M2(13P2)cs--4M2(13P0)cs-M2(13P2)ss-M2(13P0)cc-M2(13P2)ss--M2(13P0)ss-M2(13P2)cc-.In relations (20), we eliminate the slopes and obtain masses expressions which relate six meson states. Inserting the masses of the corresponding mesons into relations (20), we obtain the masses of Mnn-, Mns-, Mss-, and Mcs- of ground scalar meson. In our previous work, a series of relations between meson mass and the parameters of radial trajectories are established in the framework of Regge phenomenology [47, 48]. The relations are still applicable for the scalar meson. Inserting the ground scalar meson masses and the parameters in [47, 48], the radial excited meson masses are predicted. The results are compared with other predictions and shown in Table 3. Moreover, the radial excited masses of the light quark sector are shown in Figure 1.Table 3
Predicted massMnn-,Mns-,Mss-, and Mcs- of ground scalar meson. (All in MeV and the values used as input for our analysis are shown in boldface.)
Nonet
Mass
M
n
n
-
M
n
s
-
M
s
s
-
M
c
n
-
M
c
s
-
M
c
c
-
1
3
P
0
Present work
1024
1279
1414
2318
2423
3415
[32]
960 ± 30
1220
-
150
+
50
1220 ± 40
[24]
983 ± 10
1204 ± 10
1397 ± 16
[19]
1090
1240
1360
2400
2480
3440
2
3
P
0
Present work
1611
1826
1924
2835
3099
3958
[33]
2880
2970
[34, 35]
2919
3054
[19]
1780
1890
1990
3920
3
3
P
0
Present work
2034
2243
2390
3270
3653
4434The quasi-linear trajectory forN3P0 meson nonet.
(a)
(b)
(c)


## 5. Results and Discussion

According to the introduction in Section1, the isovector member of nonet is important for the assignment of isoscalar meson, due to providing a beacon for the mass scale of meson nonet. However, both states the a0(980) and a0(1450) are observed in the experiments and could be considered as candidates. In Table 3, our results favor the interpretation of the state a0(980) rather than the a0(1450) as the isovector ground scalar meson. The assignment is supported by the different theoretical models prediction. In the naive quark model, for S=1 states, spin-orbit coupling results in mass order m(2++)≥m(1++)≥m(0++), which supports the fact that a0(980) (not the a0(1450)) is the isovector member of scalar nonet [49, 50]. In the scheme of K-matrix analysis, Anvisoch also indicate that the mass of the 13P0 isovector state is about 960±30MeV, which is in excellent agreement with our prediction [32].Apart from the isovector member, the isoscalar sector is also ambiguous, both experimentally and theoretically. In Table3, we propose the bare nonstrange and strange members masses of isoscalar meson.In the last decade, the heavy-light mesons that attract more attention with many new resonances have been observed in the experiments, such asDs0*(2317), Ds1*(2460), DsJ*(2715), and DsJ*(2860). For the Ds0*(2317), it was first observed in DS+π by the Babar Collaboration at the Stanford Linear Accelerator Center with a mass of about 2317 MeV and width of about 350 MeV [51]. Subsequently, this state has also been reported by the Bell Collaboration [52] and the CLEO [53]. In our present work, the mass of the charm-strange meson is about 100 MeV higher than the measured mass of Ds0*(2317), which is consistent with the predictions by Godfrey and Isgur [19]. Consequently, we suggest that the assignment for the Ds0*(2317) as a 13P0 charm-strange meson needs further testing in the experiment.In summary, the understanding of scalar meson is quite puzzling for the theorists and experimentalists. Until now, there is no one state that can be assigned as the scalar meson member without dispute. In the present work, combining three complementary approaches, non-relativistic constituent quark model, Regge phenomenology, and meson-meson mixing, we investigate the assignment of ground scalar meson. Our results are useful for the assignment of the scalar meson in the future.Moreover, we also find a bridge which relate the heavy and light flavor mesons in the process of analyzing scalar meson. The bridge is significant for the assignment of the discovered states and searching the new resonances which have not been observed in the experiments.



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