軽い重イオン散乱における 三体斥力の効果

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「少数系物理の現状と今後の展望」研究会 (Dec 23-25, 2008 at RCNP ). 軽い重イオン散乱における 三体斥力の効果. 古本 猛憲 ( 大阪市立大学・理学研究科). 共同研究者 櫻木 千典 ( 大阪市立大学・理学研究科) 山本 安夫 ( 都留文科大学 ). Contents. New complex G-matrix (CEG07) ・ modern NN interaction in free space “ ESC04 ” (Extended Soft-Core) - PowerPoint PPT Presentation

Transcript of 軽い重イオン散乱における 三体斥力の効果

Page 1: 軽い重イオン散乱における 三体斥力の効果

軽い重イオン散乱における三体斥力の効果

古本 猛憲( 大阪市立大学・理学研究科 )

「少数系物理の現状と今後の展望」研究会 (Dec 23-25, 2008 at RCNP)

共同研究者櫻木 千典 ( 大阪市立大学・理学研究科 )山本 安夫 ( 都留文科大学 )

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ContentsContents

1. New complex G-matrix (CEG07) ・ modern NN interaction in free space

“ESC04” (Extended Soft-Core)

・ includes the Three-Body Force (TBF) effects

・ satisfy the nuclear-matter saturation property

2. Application to N-A elastic scattering ・ Single-Folding model for p + 12C

3. Application to A-A elastic scattering ・ Double-Folding model for 16O + 16O & other systems

important role of three-body force (TBF)

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“ESC04” : the latest version of Extended Soft-Core force designed for NN, YN and YY systems

Th. Rijken, Y. Yamamoto, Phys.Rev.C 73 (2006) 044008

Complex G-matrix interaction ( CEG07 )

T.Furumoto, Y. Sakuragi and Y. Yamamoto, Phys.Rev.C 78 (2008) 044610

1. Three-body attraction (TBA) ・ Fujita-Miyazawa diagram ・ important at low density region

2. Three-body repulsion (TBR) ・ originated the triple-meson correlation ・ important at high-density region

density-dependent effective two-body force

In the ESC04 model

Page 4: 軽い重イオン散乱における 三体斥力の効果

Complex G-matrix interaction ( CEG07 )

includes the three-body force

switch off three-body force(two-body only)

derived from ESC04 NN force (Extended Soft-Core)

Decisive role to make the saturation curve realistic

Page 5: 軽い重イオン散乱における 三体斥力の効果

)()(

)exp(),;,(),(

),;,()()(

0

RR

rskrRrR

rrRrR

CC

FEX

FDC

iWV

diEkT

dEkTU

)(,

)(,,

imagEXD

realEXDEXD iTTT

Single folding Potential(Central part)

Proton

Target

R

rT(s)

Complex G-matrix interaction (CEG07)

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)()(

)exp()(),;,()(

)(),;,()()(

0)(*

)(*

RR

rskRSLrRr

rrSLrRrR

LSLS

iiF

LSEXi

iiF

LSDiLS

iWV

diEkT

dEkTU

),(,

),(,

)(,

imagLSEXD

realLSEXD

LSEXD iTTT

Single folding Potential(LS part)

Proton

Target

R

rT(LS)(s)

Complex G-matrix interaction (CEG07)

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LSWLS

CWCopt

WiNV

WiNVU

Renormalization of the imaginary potential strength

fix NW-value to be 0.65to reproduce the measuredtotal reaction cross sections

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p-12C elastic scattering

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Comparison of the folding potential at E = 122 MeV CEG07a(two body only) vs CEG07b(with TBF)

mainly seen in the real central part

TBF effect

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This difference appears in analyzing power

Comparison of the folding potential at E = 122 MeV CEG07a(two body only) vs CEG07b(with TBF)

TBF effect

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0

02

0

Nucleon-Nucleus(one nuclear matter)

Nucleus-Nucleus(two nuclear matters)

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Double folding Potential

R

r1

r2

vNN(s)

Projectile(1) Target(2)

)(,

)(,,

imagEXD

realEXDEXD iTTT

Complex G-matrix interaction (CEG07)

)()(

ddexp),;(),(),(

dd),;()()()(

21222111

212211

RR

rrsK

ssrrsrr

rrsrrR

DFMDFM

EX

D

iWV

MiET

ETU

Frozen-density app. (FDA)

21

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Double folding Potential

R

r1

r2

vNN(s)

Projectile(1) Target(2)

)()(

ddexp),;(),(),(

dd),;()()()(

21222111

212211

RR

rrsK

ssrrsrr

rrsrrR

DFMDFM

EX

D

iWV

MiET

ETU

Frozen-density app. (FDA)

21

DFMWDFMDFM WiNVU

Renormalization factor

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16O + 16O elastic scattering @ E/A = 70 MeV

DFMWDFMDFM WiNVU

T.Furumoto, Y. Sakuragi and Y. Yamamoto, (Phys.Rev.C rapid communications (2008) in press)

important effect of three-body force

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21222111

212211

ddexp),;(),(),(

dd),;()()()(

rrsK

ssrrsrr

rrsrrR

MiET

ETU

EX

D

Double folding Potential

R

r1

r2

vNN(s)

Projectile(1) Target(2)

)()()( RRR DFMDFMDFM iWVU

21 1.

)(5.0 2. 21

Local density approximation (LDA)

)(

)( 3.

00

021

FDA

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)(

)( 3.

)(5.0 2.

1.

00

021

21

21

局所密度近似 (LDA)

16O + 16O folding potentials with CEG07b (with TBF) @ E/A = 70 MeV

FDA

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)(

)( 3.

)(5.0 2.

1.

00

021

21

21

局所密度近似 (LDA)

16O + 16O elastic scattering with CEG07b (with TBF) @ E/A = 70 MeV

FDA

DFMWDFMDFM WiNVU

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DFMWDFMDFM WiNVU

16O + 12C, 12C + 12C elastic scattering                    @ E/A = 93.9, 135 MeV

important effect of three-body force

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SummarySummary

• We have proposed a new complex G-matrix (CEG07) - derived from modern NN interaction model; ESC04 (extended soft-core) - include Three-Body Force (TBF) effect to be consistent with saturation property

• CEG07 with TBF-effects is successful for both - proton-nucleus (N-A) and nucleus-nucleus (A-A) elastic scattering

•Decisive role of Three-Body Force (TBF) effect is found. - particularly TBR (Three-Body Repulsion) effect is essential, both for nuclear saturation & nucleus-nucleus scattering