Ghil-Seok Yang, Yongseok Oh, Hyun-Chul Kim NTG (Nuclear Theory Group), (Nuclear Theory Group), Inha...

Dependence of the decay width

for exotic pentaquark Θ+(1540) on its mass

and the mass of N(1685) in a chiral soliton model

Ghil-Seok Yang Yongseok Oh Hyun-Chul Kim

NTG (Nuclear Theory Group)

Inha University

HEP (Center for High Energy

Physics) Kyungpook Natlsquol

University

ldquoNew Frontiers in QCDrdquo 27th ndash 28th October 2011 Engineering Research Park Yonsei University Seoul Republic of Korea

bull Prehistory of SU(3) Baryons

bull Motivation (Θ+ N )

bull Chiral Soliton Model

bull Masses and Decay Width

bull Summary

Outline

Naiumlve Quark Model (up down strange light quarks)

SU(3) scheme to classify particles with the same spin

and parity

Fundamental Particles

multiplets (proton neutron) isospin [ SU(2) ] rarr higher symmetry (Σ

K) SU(3)

SU(3) Baryons SU(3) Baryons

Hadron [ baryon (qqq) meson (qq) ] SU(3) color singlet Hadron [ baryon (qqq) meson (qq) ] SU(3) color singlet

Why not 4 5 6 hellip quark states

representation 10 (10)

Nothing prevents such states to exist

Y s Oh and H c Kim Phys Rev D 70 094022 (2004)

1997 Diakonov Petrov and Polyakov Narrow 5-quark resonance (q4q Θ+) ( M = 1530 Γ~ 15 MeV from Chiral Soliton Model)

(uddss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32

Ξ032Ξ-32Ξ--32

Σ-10

Σ010

Σ+10

(uudss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)

Motivation Motivation

S = -1

S = -2

Successful searches for Θ+ (2003~2005) 2007 PDG


Unsuccessful searches for Θ+ (2006~2008) 2010 PDG



Experimental Status

New positive experiments (2005 - 2010)

DIANA 2010 (Θ+) M = 1538plusmn2 Γ= 039plusmn010

MeV

(K+n rarr K0p higher statistical significance 6σ - 8σ)

[Signals are confirmed by LEPS SVD KEK hellip]

GRAAL (N ) M = 1685plusmn0012 MeV (CBELSATAPS LNS-Sendai hellip)

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)

Various experimental data for Θ+

and N

Mass of Θ+ 1525 ndash 1565 MeV

Mass of N 1665 ndash 1695 MeV

Chiral Soliton Model Chiral Soliton Model

Effective and relativistic low energy theory

Large Nc limit meson field

rarr soliton

Quantizing SU(3) rotated-meson fields rarr Collective Hamiltonian model baryon states

Chiral Soliton Model

Hedgehog Ansatz

Collective quantization

SU(2) Witten imbedding into SU(3) SU(2) X U(1)

Model baryon state

Constraint for the collective quantization

Mixings of baryon states


Mixing coefficients


Octet (8) J p = 12 + Decuplet (10) J p = 32 +

Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

-frac12 frac12

940

11161193

1318

Mass

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass

SU(3) flavor symmetry breaking

Chiral Soliton Model (mass) Chiral Soliton Model (mass)

Collective Hamiltonian for flavor symmetry breakings

α β γ

Two advantages offered by the model-independent approach in the χSM

1 the very same set of dynamical model-parameters allows us

to calculate the physical observables of all SU(3) baryons regardless of different

SU(3) flavor representations of baryons namely octet decuplet antidecuplet

and so on

2 these dynamical model-parameters can be adjusted to the experimental data

of

the baryon octet which are well established with high precisions


Mass α β γ (for octet decuplet antide-cuplethellip)

Vector transitions wi (i=12hellip6)

Axial transitions ai (i=12hellip6)

[10] [10]

Baryonsl = l0(1 + c ΔT) linear expansion coefficient of a wire c

[8]

model-parame-tersHowever


DPP EKP χQSM

Considered Effects SU(3) H SU(3) H SU(3) H

Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )

ΣπN [MeV] 45 73 Predicted rarr 41

Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037

ΓΘ+ [MeV] 15 for sym

111 for sym

071 for symDPP Diakonov Petrov Polyakov Z Physics A 359 305-314 (1997)EKP Ellis Karliner Praszalowicz JHEP 0405 002 (2004)χQSM Tim Ledwig H-Ch Kim K Goeke Phys Rev D 78 054005 amp Nucl Phys A 811 353 2008

Problems in the previous solitonic approaches1


Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )

( dss)Ξ- Ξ0 ( uss )

Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass

SU(3) flavor symmetry breaking+ Isospin symmetry breaking

Chiral Soliton Model (mass) Chiral Soliton Model (mass)Collective Hamiltonian for flavor symmetry breakings

α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3

In order to determine the values of model parame-ters ldquoModel-independent approachrdquo needs more informa-tion(at least 2 inputs for antidecuplet baryons)

Mass splittings within a Chiral Soliton Model

Formulae for Baryon Octet Masses

hadronic mass part in terms of δ1 and δ2


Formulae for Baryon Decuplet Masses



Formulae for Baryon Anti-Decuplet Masses

hadronic mass part in terms of δ3



DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3


In order to take fully into account the masses of

the baryon octet as input it is inevitable to consider

the breakdown of isospin symmetry

Two sources for the isospin symmetry breaking

1 mass differences of up and down quarks (hadronic part)

2Electromagnetic interactions (EM part)

ΔMB = MB1 ndash MB2

= (ΔMB )H + (ΔMB )EM

B(p) B(p)

k

p pp - k

EM mass corrections

Electromagnetic (EM ) self-energy

EM [MeV] Exp

(p ndash n)EM 076plusmn030

(Σ+ ndash Σ-)EM-017plusmn030

(Ξ0 ndashΞ-)EM-086plusmn030

( p ndash n )exp~ ndash 1293 MeV ( p ndash n ) EM ~076 MeV

9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y

Gasser Leutwyler PhysRep 87 77 ldquoQuark Massesrdquo



In the ChSM

It can be further reduced to

Because of Bose symmetry

G S Yang H-Ch Kim and M V Polyakov Phys Lett B 695 214 (2011)


Weinberg-Treiman formulaM EM(T3) = αT3

2 + βT3 + γDashen ansatzΔM EM ~ κT3

2 ~ κrsquoQ 2


Coleman-Glashow relation

EM [MeV] Exp [input]

(Mp ndash Mn)EM076plusmn030

(MΣ+ ndash MΣ-)EM-017plusmn030

(MΞ0 ndashMΞ-)EM-086plusmn030


EM [MeV] Exp [input] reproduced

(Mp ndash Mn)EM076plusmn030 074plusmn022

(MΣ+ ndash MΣ-)EM-017plusmn030 -015plusmn023

(MΞ0 ndashMΞ-)EM-086plusmn030 -088plusmn028


Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]

Physical mass differences of baryon decuplet




(ΔM)EM(ΔM)H




DPP EKP χQSM This Work

Considered Effects SU(3) H SU(3) H SU(3) H EM + iso H + SU(3) H

Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym

DPP Diakonov Petrov Polyakov Z Physics A 359 305-314 (1997)EKP Ellis Karliner Praszalowicz JHEP 0405 002 (2004)χQSM Tim Ledwig H-Ch Kim K Goeke Phys Rev D 78 054005 amp Nucl Phys A 811 353 2008

Problems in the previous solitonic approaches

1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N



Chiral Soliton Model (axial-vector) Chiral Soliton Model (axial-vector)

Axial-vector transitions

with

The full expression for the axial-vector transitions g 1BBrsquo = g 1BBrsquo

(0) + g 1BBrsquo(op)

+ g 1BBrsquo(wf)

SU(3) baryons Motivation Mass splitting Vector Axial-vector Summary



036plusmn008

ResultsResults

Baryon octet masses

ResultsResults

Baryon decuplet masses

ResultsResults


and N



DIANALEPS

NA49 Mass of Ξ--32 = 1862 MeV

DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA

Chiral Soliton Model ldquomodel-independent approachrdquo

Mass splittings SU(3) and isospin symmetry breakings with EM

in the range of MΘ+ = 1500-1600MeV used as input

Masses of octet and decuplet are not sensitive to the MΘ+ input rarr very good agreement with experimental data

Small value of pion-nucleon sigma term is estimated (ΣπN = 35 - 40MeV)

MΘ+ = 1524 MeV [LEPS]

MN = 1685 MeV [GRAAL]

ΓΘ+ = 038plusmn011 MeV [DIANA]

reliable values within a chiral soliton model

Summary Summary

Спасибо

Thank you

ありがとうございます 감사합니다

Danke schoumln

謝謝TERIMA KASIH

Slide 1

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Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39

bull Prehistory of SU(3) Baryons

bull Motivation (Θ+ N )

bull Chiral Soliton Model

bull Masses and Decay Width

bull Summary

Outline



and parity



K) SU(3)








(uddss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32

Ξ032Ξ-32Ξ--32

Σ-10

Σ010

Σ+10

(uudss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


S = -1

S = -2






Experimental Status



MeV




(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N






rarr soliton



Hedgehog Ansatz



Model baryon state




Mixing coefficients



Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

-frac12 frac12

940

11161193

1318

Mass

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass




α β γ





and so on


of






[10] [10]


[8]



DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym




Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

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Slide 4

Slide 5

Slide 6

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Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39



and parity



K) SU(3)








(uddss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32

Ξ032Ξ-32Ξ--32

Σ-10

Σ010

Σ+10

(uudss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


S = -1

S = -2






Experimental Status



MeV




(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N






rarr soliton



Hedgehog Ansatz



Model baryon state




Mixing coefficients



Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

-frac12 frac12

940

11161193

1318

Mass

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass




α β γ





and so on


of






[10] [10]


[8]



DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym




Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

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Slide 29

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Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39


(uddss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32

Ξ032Ξ-32Ξ--32

Σ-10

Σ010

Σ+10

(uudss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


S = -1

S = -2






Experimental Status



MeV




(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N






rarr soliton



Hedgehog Ansatz



Model baryon state




Mixing coefficients



Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

-frac12 frac12

940

11161193

1318

Mass

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass




α β γ





and so on


of






[10] [10]


[8]



DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym




Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39






Experimental Status



MeV




(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N






rarr soliton



Hedgehog Ansatz



Model baryon state




Mixing coefficients



Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

-frac12 frac12

940

11161193

1318

Mass

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass




α β γ





and so on


of






[10] [10]


[8]



DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym




Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39




rarr soliton



Hedgehog Ansatz



Model baryon state




Mixing coefficients



Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

-frac12 frac12

940

11161193

1318

Mass

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass




α β γ





and so on


of






[10] [10]


[8]



DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym




Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39

Model baryon state




Mixing coefficients



Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

-frac12 frac12

940

11161193

1318

Mass

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass




α β γ





and so on


of






[10] [10]


[8]



DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym




Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39

Mixing coefficients



Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

-frac12 frac12

940

11161193

1318

Mass

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass




α β γ





and so on


of






[10] [10]


[8]



DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym




Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39


Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

-frac12 frac12

940

11161193

1318

Mass

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass




α β γ





and so on


of






[10] [10]


[8]



DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym




Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39





and so on


of






[10] [10]


[8]



DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym




Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym




Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39


Y

T3

YY

T3

-1

1 N

Ξ

Λ

Σ0

1

-1

-2

Δ

Σ

Ξ

Ω-

( udd ) n p ( uud )


Σ- Σ+

Λ

Σ0

-frac12 frac12

940

11161193

1318

Mass

( ddd )Δ- Δ++ ( uuu )Δ0 Δ+

Ω-( sss )

Ξ- Ξ0

Σ- Σ0 Σ+

-frac12 frac12-32 -32

1232

1385

1533

1673

Mass



α β γ

+ α β γ


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39


DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3













DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39












DPP EKP χQSM


Input Masses

[MeV]

N(1710 )Θ+(1539plusmn2)

Ξ--

(1862plusmn2 )


Results

I2 [fm] 04 049 048

msα [MeV]

msβ [MeV]

msγ [MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym



2

3










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39










B(p) B(p)

k

p pp - k

EM mass corrections


EM [MeV] Exp





9383 9396

1197 1189

1321 1315

( udd ) n p ( uud )

T3


Σ- Σ+

Λ

Σ0

-frac12-1 1frac12

-1

1

Y




In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39


In the ChSM







2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39




2 ~ κrsquoQ 2













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

Slide 8

Slide 9

Slide 10

Slide 11

Slide 12

Slide 13

Slide 14

Slide 15

Slide 16

Slide 17

Slide 18

Slide 19

Slide 20

Slide 21

Slide 22

Slide 23

Slide 24

Slide 25

Slide 26

Slide 27

Slide 28

Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39













Χ 2 fit


[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

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[ DWThomas et al]

[ PDG 2010 ]

[ GW 2006 ]

[ Gatchina 1981 ]





(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

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(ΔM)EM(ΔM)H






Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

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Input Masses

[MeV]

N(1710 )

Θ+(1539plusmn2)

Ξ--(1862plusmn2 )

Θ+ 1500-1580 MeV


Re-sults

I2 [fm] 04 049 048

msα [MeV]

msβ

[MeV]

msγ

[MeV]

-218-156-107

-605-23152

-197-94-53

c10 0084 0088 0037


111 for sym

071 for sym



1

2

3

(ud-dss)

T3

1

Θ+(uudds)

frac12-frac12

-1

2

Ξ+32Ξ0

32Ξ-32Ξ--32

Σ-10 Σ010 Σ+

10

(u-udss)

p ( uud )( udd ) n

Y

S = 1

S = 0

Anti-decuplet (10)


and N





with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

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with



+ g 1BBrsquo(wf)




036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

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036plusmn008

ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

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Slide 2

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ResultsResults

Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

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Slide 32

Slide 33

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Baryon octet masses

ResultsResults


ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

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ResultsResults


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

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Slide 29

Slide 30

Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39


and N



DIANALEPS


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

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Slide 30

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Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39


DIANALEPS

GRAALSAID

MAMI

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

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Slide 33

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Slide 38

Slide 39

DIANA

LEPS DIANA










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

Slide 7

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Slide 31

Slide 32

Slide 33

Slide 34

Slide 35

Slide 36

Slide 37

Slide 38

Slide 39










Summary Summary

Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

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Спасибо

Thank you


Danke schoumln

謝謝TERIMA KASIH

Slide 1

Slide 2

Slide 3

Slide 4

Slide 5

Slide 6

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Ghil-Seok Yang, Yongseok Oh, Hyun-Chul Kim NTG (Nuclear Theory Group), (Nuclear Theory Group), Inha...

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Transcript of Ghil-Seok Yang, Yongseok Oh, Hyun-Chul Kim NTG (Nuclear Theory Group), (Nuclear Theory Group), Inha...