pions in nuclei and tensor force
DESCRIPTION
Pions in nuclei and tensor force. Hiroshi Toki (RCNP, Osaka) in collaboration with Yoko Ogawa (RCNP, Osaka) Jinniu Hu (RCNP, Osaka) Takayuki Myo (Osaka Inst. Tech.) Kiyomi Ikeda (RIKEN). Pion is important !! In Nuclear Physics. - PowerPoint PPT PresentationTRANSCRIPT
10.2.23 [email protected] 1
Pions in nuclei and tensor force
Hiroshi Toki (RCNP, Osaka)in collaboration with
Yoko Ogawa (RCNP, Osaka)Jinniu Hu (RCNP, Osaka)
Takayuki Myo (Osaka Inst. Tech.)Kiyomi Ikeda (RIKEN)
10.2.23 [email protected] 2
Pion is important !! In Nuclear Physics
Yukawa introduced pion as mediator of nuclear interaction for nuclei. (1934)
Nuclear Physics started by shell model with strong spin-orbit interaction.
(1949: Meyer-Jensen: Phenomenological)The pion had not played the central role in
nuclear physics until recent years.
10.2.23 [email protected] 3
Variational calculation of light nuclei with NN interaction
C. Pieper and R. B. Wiringa, Annu. Rev. Nucl. Part. Sci.51(2001)
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ΨVπ Ψ
Ψ VNN Ψ~ 80%
€
Ψ=φ(r12)φ(r23)...φ(rij )
VMC+GFMC
VNNN
Fujita-Miyazawa
Relativistic
Pion is a key elementWe want to calculate heavy nuclei!!
10.2.23 [email protected] 4
RCNP experiment (good resolution)
Y. Fujita et al.,E.Phys.J A13 (2002) 411
H. Fujita et al., PRC
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Ψf στ Ψ i
Not simpleGiant GT
10.2.23 [email protected] 5
The pion (tensor) is important.
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Deuteron (1+)QuickTime˛ Ç∆
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NN interaction S=1 and L=0 or 2
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π
10.2.23 [email protected] 6
Deuteron and tensor interaction
Central interaction has strong repulsion.Tensor interaction is strong in 3S1 channel.S-wave function has a dip.D-wave component is only 6%.Tensor attraction provides 80% of entire at
traction.D-wave is spatially shrank by a half.
€
rσ 1 ⋅
r q
r σ 2 ⋅
r q =
1
3q2S12( ˆ q ) +
1
3
r σ 1 ⋅
r σ 2q
2
€
S12( ˆ q ) = 24π Y2( ˆ q ) σ 1σ 2[ ]2[ ]0
Pion Tensor spin-spin
10.2.23 [email protected] 7
Chiral symmetry (Nambu:1960)
Chiral symmetry is the key symmetry to connect real world with QCD physics
Chiral model is very powerful in generating various hadronic states
Nucleon gets mass dynamicallyPion is the Nambu-Goldstone particle of the c
hiral symmetry breaking
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He was motivated by the BCS theory (1958) .
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E p = ±( p2 + m2)1/ 2
Nobel prize (2008)
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rσ ⋅
rp ψ R + mψ L = E pψ R
−r σ ⋅
r p ψ L + mψ R = E pψ L
€
Δ is the order parameter is the order parameter
€
m
Particle number Chiral symmetry€
εiψ i + Δψ i * = E iψ i
−ε iψ i * + Δ*ψ i = E iψ i
*
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E i = ±(ε i2 + Δ2)1/ 2
10.2.23 [email protected] 9
Nambu-Jona-Lasinio Lagrangian
Mean field approximation; Hartree approximation
Fermion gets mass.
The chiral symmetry is spontaneously broken.
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ψ ψ → ψ ψ cos(2α ) +ψ iγ 5ψsin(2α )
ψ iγ 5ψ →ψ iγ 5ψ cos(2α ) −ψ ψsin(2α )
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ψ → e iαγ 5ψChiral transformation
Pion appears as a Nambu-Goldstone boson.
10.2.23 [email protected] 10
Chiral sigma model
Chiral sigma model
Linear Sigma Model Lagrangian
Polar coordinate
Weinberg transformation
Y. Ogawa et al. PTP (2004)
Pion is the Nambu boson of chiral symmetry
10.2.23 [email protected] 11
Non-linear sigma modelNon-linear sigma model
Lagrangian = fπ + φ
whereM = gσfπ M* = M + gσ φ
mπ2 = 2 + fπ mσ
2 = 2 +3 fπ
m = gfπ m
= m + gφ
~ ~
Free parameters are and
€
mσ
€
gω (Two parameters)
N
10.2.23 [email protected] 12
€
Ψ=Ψ(σ ,ω)⊗Ψ(N)Mean field approximation for mesons.
€
Ψ(N) = C0 RMF + Ci
i
∑ 2p − 2hi
Nucleons are moving in the mean field and occasionally broughtup to high momentum states
due to pion exchange interaction
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σ
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σ
h h
p p
Bruekner argument
Relativistic Chiral Mean Field ModelWave function for mesons and nucleons
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Relativistic Brueckner-Hartree-Fock theory
Brockmann-Machleidt (1990)
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G = V + VQ
eG
Us~ -400MeVUv~ 350MeV
€
π
€
πrelativity
RBHF theory provides a theoretical foundation of RMF model.
RBHF
Non-RBHF
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Density dependent RMF model
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Brockmann Toki PRL(1992)
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Why 2p-2h states are necessary for the tensorinteraction?
G.S.
Spin-saturated
The spin flipped states are alreadyoccupied by other nucleons.
Pauli forbidden
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σ1σ 2[ ]2⋅Y2(r)
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Energy minimization with respect tomeson and nucleon fields
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δΨ H Ψ
Ψ Ψ= 0
€
δE
δσ= 0
δE
δω= 0
(Mean field equation)
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δE
δψ i(x)= 0
δE
δCi
= 0
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Energy
Energy minimization
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RCMF equation
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10.2.23 [email protected] 19
Energy minimization with respect tomeson and nucleon fields
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δΨ H Ψ
Ψ Ψ= 0
€
δE
δσ= 0
δE
δω= 0
(Mean field equation)
€
δE
δψ i(x)= 0
δE
δCi
= 0
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δE
δbi
= 0 (Corrrelation function)
10.2.23 [email protected] 20
Unitary Correlation Operator Method
H. Feldmeier, T. Neff, R. Roth, J. Schnack, NPA632(1998)61
corr. uncorr. SM, HF, FMDCΨ = ⋅Φ ←
{ }12exp( ), ( ) ( )ij r r
i j
C i g g p s r s r p<
= − = +∑
short-range correlator † 1 (Unitary trans.)C C−=
rp p pΩ= +r r r
Bare Hamiltonian
† : Hermitian generatorg g=
Shift operator depending on the relative distance r
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C+HCΦ = EΦ
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HΨ = EΨ
(UCOM)
10.2.23 [email protected] 21
Short-range correlator : C
† 1 1
( ) ( )r rC p C p
R r R r+ +
=′ ′
†C lC l=r r
† ( )C r C R r+= †12 12C S C S=†C sC s=r r
Hamiltonian in UCOM
2-body approximation in the cluster expansion of operator€
H = T + V = Ti
i
∑ − TC .M + V (rij
i< j
∑ )
€
C+HC = ˜ T + ˜ V
€
˜ T = T + ΔT
€
ΔT = uij
i< j
∑
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˜ V = V (R+
i< j
∑ (rij ))
( ( ))( )
( )
s R rR r
s r+
+′ =
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Numerical results (1)
4He12C16O
Ogawa TokiNP 2009
Adjust binding energyand size.
10.2.23 [email protected] 23
Numerical results 2
The difference between 12C and 16O is 3MeV/N.
The difference comes from low pion spin states (J<3).This is the Pauli blocking effect.
P3/2
P1/2
C
O
S1/2
Pion energy Pion tensor provides large attraction to 12C
10.2.23 [email protected] 24
Chiral symmetry
Nucleon mass is reducedby 20% due to sigma.
We want to work out heavier nuclei for magic number.Spin-orbit splitting should be worked out systematically.
Ogawa TokiNP(2009)
Not 45%
N
10.2.23 [email protected] 25
Nuclear matter
Hu Ogawa TokiPhys. Rev. 2009
€
ψ ψ
E/A
Total
Pion
€
Σ ~ 50MeV
10.2.23 [email protected] 26
Deeply bound pionic atom
Toki Yamazaki, PL(1988)
Predicted to exist
Found by (d,3He) @ GSIItahashi, Hayano, Yamazaki..Z. Phys.(1996), PRL(2004)
Findings: isovector s-wave
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b1
b1(ρ )=1− 0.37
ρ
ρ 0
€
fπ2mπ
2 = −2mq ψ ψ
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ψ ψ
ψ ψ=1− 0.37
ρ
ρ 0
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b1 ∝1
fπ2
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Halo structure in 11LiQuickTime˛ Ç∆
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Deuteron-like state ismade by 2p-2h states in shell model.
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Deuteron wave function
Myo Kato Toki Ikeda PRC(2008)
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Tensor interaction needs2p-2h excitation of pnpair.
P1/2 orbit is used for thisExcitation.
This orbit is blocked When we want to put two neutrons.
S1/2 orbit is free of this.
Tensor interaction
10.2.23 [email protected] 29
ConclusionPion (tensor) is treated within relativistic chi
ral mean field model.We extended RBHF theory for finite nuclei.Nucleon mass is reduced by 20%Chiral condensate is similar to the model in
dependent value. (Sigma term~50MeV)Deeply bound pionic atom seems to verify p
artial recovery of chiral symmetry.