pentaquark baryons and tetraquark mesoniums from lattice qcd
DESCRIPTION
Pentaquark Baryons and Tetraquark Mesoniums from Lattice QCD . Hadron Calculation with overlap fermion Pentaquark Baryons and Tetraquark Mesoniums on the Lattice . χ QCD Collaboration : A. Alexandru, Y. Chen, S.J. Dong, T. Draper, I. Horvath, B. Joo, - PowerPoint PPT PresentationTRANSCRIPT
Charm 2006, page 1
Pentaquark Baryons and Tetraquark Mesoniums from
Lattice QCD
• Hadron Calculation with overlap fermion • Pentaquark Baryons and Tetraquark Mesoniums on the Lattice
χQCD Collaboration: A. Alexandru, Y. Chen, S.J. Dong, T. Draper, I. Horvath, B.
Joo, F .X. Lee, K.F. Liu, N. Mathur, S. Tamhankar, H.Thacker, J.B.
Zhang Charm 2006, June 6, 2006
ITP, 2005, page 2
Hadron Mass and Decay ConstantHadron Mass and Decay Constant
)(2
3
)(1
00
00
0 ||2
0||)()(||0
)()((),,(
ttE
p
p
p
ttEtt
x
xpiNN
pp
eEmE
VEepNpN
xxTepttG
The two-point Green’s function decays exponentially at large separation of time
0t t
Mass M= Ep(p=0), decay constant ~ Φ
CreationCreationOperatoOperatorr
QCD QCD VacuumVacuum
ΘΘ++
????PentaquarkPentaquark
TetraquarkTetraquark????
Charm 2006, page 6
Le Taureau of Pablo Picasso (1945)
Dynamical chiral fermion Quenched approximation with chiral symmetry, and light quark masses
5th stage 11th stage
Charm 2006, page 7
Masses of N, Masses of N, ρρ, and , and ππ
• 16163 3 x 28 quenched x 28 quenched lattice, Iwasaki action lattice, Iwasaki action with a = 0.200(3) fmwith a = 0.200(3) fm
• Overlap fermionOverlap fermion• Critical slowing down is Critical slowing down is
gentlegentle• Smallest Smallest mmππ ~ 180 MeV~ 180 MeV• mmππ L > 3L > 3
Charm 2006, page 8
Evidence of Evidence of ηη’N GHOST State in S’N GHOST State in S11 11 (1535) (1535) ChannelChannel
-- --η η
W > 0
W<0
Charm 2006, page 9
Possible Pentaquark candidatePossible Pentaquark candidate
Possible candidate Signal reported to be “observed” recently θ+(1540)
ud
su d
ud
Su d u
dSu d
NN
KK
NN
KK
uu d
S d
uu d
S d
Not sufficient to study the masses/energies of the Not sufficient to study the masses/energies of the ٭٭ states, particularly in the 1/2states, particularly in the 1/2- - channel.channel. Volume study of spectral weight W is much more Volume study of spectral weight W is much more ٭٭ sensitive.sensitive.
mmKK+ m+ mN N
~ 1432 MeV~ 1432 MeV
m(m(ΘΘ++) ~1540MeV) ~1540MeV
i
tmi
ieWtG )(
1) Need to discern the nature of the states
Lattice Pentaquark Volume Variational Light enough Ghost Lattice Pentaquark Volume Variational Light enough Ghost Group signal claim Test Calculation Quark Mass Group signal claim Test Calculation Quark Mass StateState
Csikor Csikor YesYes No No Yes (2)Yes (2) No No No No et.al et.al NoNo No No Yes (9/6) Yes (9/6) No No No No Sasaki Sasaki Yes Yes No No No NoNo No No No Chiu Chiu et.alet.al Yes Yes NoNo Yes Yes No No No No
Mathur Mathur et.alet.al No No Yes Yes No No Yes Yes YesYes Ishii Ishii et.al et.al NoNo YesYes No No No No No No AlexandrouAlexandrou YesYes Yes Yes No No No No No No TakahashiTakahashi YesYes Yes Yes Yes(2)Yes(2) No No No No
Negele Negele et.al et.al ?? Yes Yes Yes(19)Yes(19)
Lasscock et. alLasscock et. al No No NoNo No No NoNo No No Holland et. alHolland et. al No No NoNo Yes Yes No NoNo No
Lattice Results on Lattice Results on ΘΘ++ PentaquarkPentaquark
Charm 2006, page 12
Status of Lattice Pentaquark Status of Lattice Pentaquark CalculationCalculation
KFL and N. Mathur (hep-lat/0510036)KFL and N. Mathur (hep-lat/0510036)• No convincing evidence for the No convincing evidence for the
claims of observing pentaquarks on claims of observing pentaquarks on the lattice.the lattice.
• Absence of evidence is not evidence Absence of evidence is not evidence of absence.of absence.
• Definite calculation should involve Definite calculation should involve dynamic chiral fermion with light dynamic chiral fermion with light quarks, variational approach, volume quarks, variational approach, volume test, and removal of ghosts.test, and removal of ghosts.
Charm 2006, page 13
Tetraquark MesoniumsTetraquark Mesoniums
QCD allows a state with more than three quarksFour quarks : Two quarks + two anti-quarks Like molecular state? Like di-quark anti-diquark state?
q12q
q21q
0¯ ¯(1)1¯+(1)
0++(0)0+ ¯(1)1+ ¯(1)
π(137)
0+ (1/2)
ρ(770)
σ(600)
f0(980)
f0(1370)
f0(1500)
a0(980)
a0(1450)
a1(1230)
K0*(1430)
JPG(I))
M (M
eV)
a2(1320)
2+ ¯(1)
f0(1710)
K0*(800)
Charm 2006, page 15
Is aIs a00 (1450) (0 (1450) (0++++) a two quark ) a two quark state?state?
Ground state : Ground state : ππ ηη ghost stateghost state..
First excited state : First excited state : aa00
CorrelationCorrelationfunctionfunctionfor for Scalar Scalar channelchannel
Our results shows scalar mass around 1400-1500 MeV, suggesting Our results shows scalar mass around 1400-1500 MeV, suggesting
aa00(1450)(1450) is a two quark state.is a two quark state.
)(JI PCG ),0(1 )1(1
mmss
Charm 2006, page 17
What is the nature of What is the nature of σσ (600)?(600)?
r
σ (500): Johnson and Teller
Two-pion exchange potential: Chembto, Durso, Riska; Stony Brook, Paris, …
σ enhancement of Δ I = ½ rule
The The σσ in in DD++→→ ππ¯̄ππ++ππ++
σσ
Without a Without a σσ pole pole
With a With a σσ pole pole
MMσσ= 478 = 478 ± ± 24242323 ± ± 17MeV 17MeV ΓΓσσ = 324 ± = 324 ± 4242
40 40 ± 21 MeV± 21 MeV
2423478M
E.M. Aitala et. al. Phys. Rev. Lett. 86, 770, (2001) E.M. Aitala et. al. Phys. Rev. Lett. 86, 770, (2001)
M. Ablikim et al. (BES), Phys. Lett. B598, 149 (2004)
Mσ = 541 ± 39 MeV, Γσ = 504 ± 84 MeV
J/ψ —> ωπ+π-
Charm 2006, page 21
Scattering Length and energy Scattering Length and energy shiftshift
• ππππ energies :energies :
• Threshold energy shift on the finite latticeThreshold energy shift on the finite lattice ::
2 , 2)(
,2)0(
22
LappmppE
mpE
LLL
)(]122)0( 62
20
20
130 LO
LaC
LaC
LampE
Charm 2006, page 22
)]0(0 )(JI ,[ PCG55
Further study is needed to check the Further study is needed to check the volume dependencevolume dependence of the of the observed states.observed states.
Scattering statesScattering states(Negative scattering(Negative scattering length)length)
)0()0( pEpE
)1()1( pEpE
Scattering statesScattering states
Possible BOUND statePossible BOUND state σσ(600)?(600)?
Charm 2006, page 23
Scattering state and its volume dependenceScattering state and its volume dependence ),,|1,,| spn
Vspn
nn
n
tMn
x n
tM
n
x
Mn
W
eW
eVM
n
txTtG
n
n
2|)0(|0
2
|)0(|0
0|))0(),((|0)(
2
2
Normalization condition requires :
Two point function : Lattice Continuum
For one particle bound state spectral weight (W) will NOT be explicitly dependent on lattice volume
Vx
Charm 2006, page 24
Scattering state and its volume dependenceScattering state and its volume dependence ),,|1,,| spn
Vspn
tEE
nn
nn
tEE
nn nnx
x
nn
nn
eVWW
eVMVM
nn
txtxTtG
,
,
222
211
2121
11
21
21
11
21 21
2 2
|)0(|0|)0(|0
0|))0()0(),(),((|0)(
Normalization condition requires :
Two point function : Lattice Continuum
For two particle scattering state spectral weight (W) WILL be explicitly dependent on lattice volume
Vx
Volume dependence of spectral weights
Volume independence suggests the observed state is an Volume independence suggests the observed state is an one particle stateone particle state
WW00
WW11
0¯ ¯(1)1¯+(1)
0++(0)0+ ¯(1)1+ ¯(1)
π(137)
0+ (1/2)
ρ(770)
σ(600)
f0(980)
f0(1370)
f0(1500)
a0(980)
a0(1450)
a1(1230)
K0*(1430)
JPG(I))
M (M
eV)
a2(1320)
2+ ¯(1)
f0(1710)
K0*(800)
MesoniumsKK Kπ Mesoniumππ Mesonium
Charm 2006, page 27
Mixing of Mixing of ssdduu and ,,
First order approximation: exact SU(3)
MeV 33 ,314703
)1370(
14706
2)1500(
14702
147000014700001470
0
0
0
xxssdduuf
ssdduuf
dduua
xxxxxxxxx
x is annihilation diagram
Charm 2006, page 28
Mixing of with GlueballMixing of with Glueballssdduu ,,
First order approximation: exact SU(3)
MeV 5.414701710
mixed;slight are glueball and )1370(
mix)not (does 14706
2)1500(
14702
1710000014700000147000001470
2
0
0
0
xm
f
ssdduuf
dduua
xxxxxxxxxxxxxxxx
Charm 2006, page 29
Scalar Mesons and Scalar Mesons and GlueballGlueball
)1500(0f)1470(0
0a
)1430(*0K)1430(*
0K
)1430(*0K)1430(*
0K
)1470(0a )1470(0
a
)800(*0K
)980(0f)980(0
a )980(0a)980(0
0a
)800(*0K
)800(*0K )800(*
0K
)( KK
)( K
)1370(0f
)600(
)1710(0fglueball
22qq
Charm 2006, page 30
SummarySummary
• No credible evidence of pentaquarks No credible evidence of pentaquarks in lattice calculationsin lattice calculations
• Plenty of tetraquark mesonium Plenty of tetraquark mesonium candidatescandidates
• σσ(600) is very likely to be a tetraquark (600) is very likely to be a tetraquark mesonium.mesonium.
• Pattern of light scalar mesons may be Pattern of light scalar mesons may be repeated in the heavy-light sectors (?)repeated in the heavy-light sectors (?)