contents ・ introduction ・ formalism ・ results ・ conclusion the 17 th international spin...
TRANSCRIPT
![Page 1: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/1.jpg)
Contents ・ Introduction
・ Formalism
・ Results
・ Conclusion
The 17th International Spin Physics Symposium (SPIN 2006)October 2-7, 2006
Kyoto University, Kyoto, Japan
Hideaki IidaProf. Hideo Suganuma
Dr. T.T.Takahashi
![Page 2: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/2.jpg)
Introduction
Origin of the massOrigin of the massMotivation
There are two types of the origin of mass:
current quark ~ 3MeV
constituent quark ~ 350MeV
Strong interaction (QCD)
⇒ Most of the mass in the world is from strong interaction (QCD)
(for light quarks)M ~ (300-400) MeV
Strong-interaction origin … about 99% !
constituent quark mass:
Higgs origin … about 1%
mu (μ=1GeV)= (1.5-3)MeVmd (μ=1GeV)= (3-7)MeVμ: renormalization scale
from the data of Particle Data Group (2006)
current quark mass:
mass of leptons: electron…me=0.51MeV
![Page 3: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/3.jpg)
IntroductionWhat is the mechanism of the generation of such a large constituent quark mass?
Spontaneous breaking of chiral symmetry
…Important mechanism of mass generation for light fermions
Y.Nambu, G.Jona-Lasinio,Phys.Rev.122(1961)345: in Nambu-Jona-Lasinio (NJL) model
π
σ
π
σ
Chiral-symmetry is broken Chiral-symmetry is restored
m ~ (1.5-7) MeV:
At high temperature or high density
M ~ (300-400) MeV:
Our present world
Study of partial chiral restoration: (theory) T.Kunihiro, T.Hatsuda (1983) (experiment) H.Enyo group, K.Imai group
One possible answer is
![Page 4: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/4.jpg)
Question:In the strong-interaction world, is chiral symmetry breaking necessary for mass generation?
IntroductionNote however that chiral symmetry is the symmetry for massless fermions
① Gluon (colored vector particle, which is originally massless):
J.E.Mandula and M.Ogilvie (Landau geuge) Phys.Lett.B185(1987),127K.Amemiya, H.Suganuma ( MA gauge ) Phys.Rev.D60(1999)114509
Large mass measured in lattice QCD:
Glueball: hadron made by only gluons
even the lightest glueball (0++) is rather heavy…1.5GeV experimental candidate: f0(1500)
massless massive
…
② Charm quark ・ Current quark mass mc : about 1.2GeV (Particle Data Group)
・ In the quark model, constituent quark mass is about 1.6GeVThe difference (1.6-1.2)GeV=400MeV is the mass generated by strong interaction without chiral symmetry breaking.
We notice following examples of mass generation without chiral symmetry breaking:
![Page 5: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/5.jpg)
In this way, we conjecture that there should be other type of mass generation
without chiral symmetry breaking or Higgs mechanism.(non-chiral origin but strong-interaction origin)
Our conjecture:Even without chiral symmetry, large mass generation generally occurs in the strong-interaction world.
In fact, all colored particles (scalar, fermion, vector) have a large mass generated by dressed gluon effect.
Introduction
colored particles
dressed gluons large mass
![Page 6: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/6.jpg)
In this talk, we study “light” colored scalar particle, which does not have chiral symmetry.
We investigate bound states of colored scalar particles, namely, hadrons made by scalar quarks in lattice QCD in terms of mass generation of scalar quark.
First study for scalar-quark systems in lattice QCDFirst study for scalar-quark systems in lattice QCD
Lattice QCD: first-principle calculation of strong interaction (non-perturbative) ⇒ powerful method in non-perturbative QCD
We call this colored scalar particle as “scalar quark”.Here, the bare scalar-quark mass is set to be almost zero.
Can we observe large mass generation even in this scalar-quark systemwithout chiral symmetry?
![Page 7: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/7.jpg)
Scalar-quark hadron
Scalar-quark hadron is made by two or three scalar quarks.
★ Statistics are different from that of ordinary hadrons
Here, we investigate hadrons made by scalar quarks.
Baryon(Fermion)
Meson(Boson)
: quark
: anti-quark
cf) ordinary hadron
Scalar-quark baryon (Boson)
Scalar-quark meson (Boson)
: scalar quark
:anti scalar-quark
Scalar-quark hadron
![Page 8: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/8.jpg)
Chimera hadronChimera hadron is made by quarks and scalar quarks.
“chimera hadron” is new terminology.
We calculate the masses of scalar-quark hadrons and chimera hadrons in quenched lattice QCD.
chimera baryon (Boson)
chimera meson (Fermion)
: quark
:anti-quark
: scalar quark
:anti scalar-quark
chimera baryon (Fermion)
Chimera hadron
![Page 9: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/9.jpg)
Formalism
: scalar quark ( color triplet )
QCD
Scalar QCD
: field strength tensor
: quark field ( color triplet ):covariant derivative
QCD including the quarks and scalar quarks
― continuum ( Minkovsky space )―
![Page 10: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/10.jpg)
Gauge invariant
Scalar-quark sector
Wilson quark action:Quark sector
Formalism― discretization (Euclid space) ―
: mass of scalar quark
: space coordinate: link variable: hopping parameter
![Page 11: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/11.jpg)
・ scalar-quark meson :
・ scalar-quark baryon :
Scalar
Scalar
・ chimera meson :
・ chimera baryon :
Spinor
Spinor
Scalar
Summary of scalar and chimera hadrons
For the study of scalar-quark system,we calculate the masses of following scalar hadrons and chimera hadrons:
Ψ: quarkφ: scalar quark
Scalar-quark hadrons
Chimera hadrons
![Page 12: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/12.jpg)
: quark ( : index of spinor)
・ operators of scalar-quark hadrons
・ operators of chimera hadrons
: scalar quark ( : index of color)
( scalar-quark baryon )
( chimera meson )
( chimera baryon )
( chimera baryon )
( scalar-quark meson )
Hadronic operators and correlators
⇒ using these operators, we calculate the correlators of these hadrons
( total momentum is projected to be zero )
from , we extract the mass of these hadrons
We use the following operators of scalar-quark hadrons and chimera hadrons:
![Page 13: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/13.jpg)
β=5.70 ( )β=5.75 ( )β=6.10 ( )
Lattice size: 163×24 (for φ†φ) 163×32 (for other hadrons except)
spatial volume: (2.9fm)3 (β=5.70) (2.7fm)3 (β=5.75) (1.8fm)3 (β=6.10)
Quenched lattice QCD
Parameters of lattice QCD
: lattice spacing (lattice cutoff)
(corresponding to gauge coupling)
![Page 14: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/14.jpg)
Scalar-quark meson mass M vs bare scalar-quark mass msq
(β=5.75, latt.size: 163×32)
3GeV
M(GeV) (scalar-quark meson mass)Mass generation of scalar quark by gluon
Scalar-quark meson φ†φ
Ψ : quark φ: scalar quark
msq(GeV)(bare scalar-quark mass)
Important result :At bare scalar-quark mass msq ~ 0,
scalar-quark meson mass M ~ 3.0GeV.⇒dynamically generated mass of scalar quark Msq is 1.5GeV!!Compared with constituent quark mass ( ~ 300MeV), this mass generation is very large.
Large mass generation by strong interaction (non chiral origin) occurs in the scalar-quarksystem!
![Page 15: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/15.jpg)
Scalar-quark baryon φφφM(GeV) (scalar-quark baryon mass)
scalar-quark baryon mass M vs bare scalar-quark mass msq (β=5.70, latt.size: 163×32)
msq(MeV)(bare scalar-quark mass)
Large mass generation of scalar quark is also seen
At bare scalar-quark mass msq ~ 0,
scalar-quark baryon mass M ~ 4.8GeV.⇒dynamically generated mass of scalar quark Msq is 1.5GeV.
Ψ : quarkφ: scalar quark
![Page 16: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/16.jpg)
Chimera meson φ†Ψ
chimera meson mass M vs quark mass mq and scalar-quark mass msq
(β=5.70, latt.size: 163×32)
mq(MeV) (bare quark mass)
M(GeV) (chimera meson mass)
msq=120MeV(bare scalar-quark mass)
msq=200MeV
msq=270MeV
Note:Ψ emerges in the following hadrons
Ψ : quarkφ: scalar quark
At bare scalar-quark mass msq ~ 0 and bare quark mass mq ~ 0,
chimera meson mass M ~ 1.9GeV. Msq + Mq ~ M is formed. (1.5 + 0.4 = 1.9)
dynamically generated mass of scalar quark Msq ~ 1.5GeV constituent quark mass Mq ~ 400MeV
![Page 17: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/17.jpg)
Chimera baryon φφΨ
mq(MeV)(bare quark mass)
M(GeV) (chimera baryon mass)
msq=120MeV(bare scalar-quark mass)
msq=200MeV
msq=270MeV
chimera baryon mass M vs quark mass mq and scalar-quark mass msq
(β=5.70, latt.size: 163×32)
At bare scalar-quark mass msq ~ 0 and bare quark mass mq ~ 0,
chimera baryon mass M ~ 3.7GeV. 2×Msq +Mq ~ M
dynamically generated mass of scalar quark Msq ~ 1.5GeVconstituent quark mass Mq ~ 400MeV
Ψ : quarkφ: scalar quark
![Page 18: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/18.jpg)
Chimera baryon ΨΨφ
mq(MeV) (bare quark mass)
M(GeV) (chimera baryon mass)
msq=120MeV(bare scalar-quark mass)
msq=200MeVmsq=270MeV
chimera baryon mass M vs quark mass mq and scalar-quark mass msq
(β=5.70, latt.size: 163×32)
At bare scalar-quark mass msq ~ 0 and bare quark mass mq ~ 0,
chimera baryon mass M ~ 2.4 GeV. Msq + 2×Mq ~ M
dynamically generated mass of scalar quark Msq ~ 1.5GeVconstituent quark mass Mq ~ 400MeV
Ψ : quarkφ: scalar quark
![Page 19: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/19.jpg)
⇒ Similar mq-dependence between and is observed.
★Similarity between φφΨ and φ†Ψ
mq(MeV)(bare quark mass)
msq=120MeV(bare scalar-quark mass)
msq=200MeV
msq=270MeV
mq(MeV)(bare quark mass)
M(GeV) (chimera meson mass)
Ψ : quarkφ: scalar quark
msq=120MeV(bare scalar-quark mass)
msq=200MeV
msq=270MeV
…Slopes (mq-dependence) are almost the same between and
M(GeV) (chimera baryon mass)
Figures of the mass of chimera hadrons
Chimera mesonChimera baryon
![Page 20: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/20.jpg)
Interpretation of the similarity between φ†Ψ and φφΨ
Chimera meson Chimera baryon
Due to the large constituent mass of scalar-quarkφ, the two particles (φφ) are close under Coulomb interaction.
V(r)
r
Energy level of φφ
Similarity of the system between and
Scalar quark φ is very heavy.So, the wave-function of light quark (Ψ) distributes around the scalar-quark φ.
wave functionsΨ : quarkφ: scalar quark
Chimera meson Chimera baryon
![Page 21: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/21.jpg)
Conclusion
Large mass generation occurs even in the scalar-quark system!(non-chiral origin)
msq ~ 0(bare scalar-quark mass)
Msq ≧ 1GeV(large mass generation of scalar quark) Dressed gluon effect
…
Dynamically generated mass of scalar quarks : about 1.5GeV Dressed gluon effect
QCD (gluon) effect(non-chiral origin)
![Page 22: Contents ・ Introduction ・ Formalism ・ Results ・ Conclusion The 17 th International Spin Physics Symposium (SPIN 2006) October 2-7, 2006 Kyoto University,](https://reader035.vdocuments.site/reader035/viewer/2022062805/5697bff21a28abf838cbbdd6/html5/thumbnails/22.jpg)
Summary and Concluding Remarks
Using Lattice QCD, we have performed the First Study of scalar-quark (colored-scalar) systems. We have found Large Mass Generation of scalar quarks. (This is Non-Chiral Origin) This Large Mass Generation can be explained by Dressed Gluon Effect.
Similarity between and systems emerges due to the large mass of scalar quark.
msq ~ 0 Msq ≧ 1GeV
colored-scalarDressed Gluon