Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T....

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Λ spin-orbit splitting deduced from DWIA analysis of the 89Y+,K+) Λ89Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy (Moscow State U.) Y. Yamamoto (Tsuru U.)
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Transcript of Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T....

Page 1: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

Λ spin-orbit splitting deduced from DWIA analysis of

the 89Y(π+,K+) Λ89Y reaction

T. Motoba (Osaka E-C U.)

D.J. Millener (Brookhaven N.L.)

D. Lanskoy (Moscow State U.)

Y. Yamamoto (Tsuru U.)  

Page 2: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

(π+,K+) reaction characteristics

Page 3: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

T.Motoba, H. Bando, R. Wunsch, J.Zofka, Phys. Rev.C38 (1988)

Page 4: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

H. Hotchi et al,

Phys. Rev. C64

044302 (2001).

Great achievement

good resolution

Γ=1.65 MeV

Ls splitting (ΔE):

(f )=1.70 MeV

(d)=1.63

(p)= 1.37

Page 5: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

High resolution γ-ray

mesurements

Page 6: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

How to understand “large” splitting of subpeaks observed in heavy systems  

Page 7: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

ΔE is not proportional to (2l+1)

Page 8: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.
Page 9: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

XS ratio is determined as  

Page 10: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

EXP vs. DWIA CAL(WS, VLS=4.3MeV)

Page 11: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

Take core-excited states seriously : up to the level of p-shell

hypernuclei

Page 12: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.
Page 13: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.
Page 14: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.
Page 15: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.
Page 16: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.
Page 17: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.
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CONCLUSION (1)Reproduce cross section ratios among a series of pronounced peaks and sub-peaks.

Page 20: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

CONCLUSION(2) Observed energy sp

acing between doublet like sub-peaks

(3L-3R) are reproduced with δ(f)=0.20 MeV,

which leads to δ(d)=0.15 MeV and δ(p)=0.09 MeV.

(cf. Λ 13 C:δ(p)=0.152+-0.07 MeV)

Page 21: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.

CONCLUSION

(3) even the GS peak should consists of two components. (See the exp. GS peak The present analysis leads to the prediction that.)

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CONCLUSION (4)  Right partner(s) contain parity-mixing

contributions :example for 3R: [1p1/2f7/2hole] Λ ( d3/2 )

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New insight into (π+,K+) spectra for other medium-heavy hypernuclei

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END

Page 27: Λ spin-orbit splitting deduced from DWIA analysis of the 89 Y (π +,K + ) Λ 89 Y reaction T. Motoba (Osaka E-C U.) D.J. Millener (Brookhaven N.L.) D. Lanskoy.
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