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Shell model studies along the N~126 line Zsolt Podolyá

Shell model studies along the N~126 line

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Shell model studies along the N~126 line. Zsolt Podoly ák. Z. 70. 74. 78. 110. N. 122. H. Grawe, K. Langanke, G. Martinez-Pinedo, Rep.Progr.Phys.70 (2007)1525. Shape transition, triaxiality. “Shell-model” nuclei. L.M. Robledo et al., J. Phys. G. 36, 115104 (2009). - PowerPoint PPT Presentation

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Page 1: Shell model studies along the N~126 line

Shell model studies along the N~126 line

Zsolt Podolyák

Page 2: Shell model studies along the N~126 line

“Shell-model” nucleiShape transition, triaxiality

70 7874

122

110

N

Z

L.M. Robledo et al., J. Phys. G. 36, 115104 (2009).

H. G

raw

e, K

. Lan

gank

e, G

. Mar

tine

z-P

ined

o,

Rep

.Pro

gr.P

hys.

70 (

2007

)152

5.

Page 3: Shell model studies along the N~126 line

Isomeric states around 208Pb

208Hg,209TlN. Aldahan et al., PRC80, 061302(R) (2009).

Isomeric state

RISING: isomeric decays

S. Steer et al., Int. J. Mod. Phys. E18, 759 (2009) and to be published

*

A. Gottardo et al.

Page 4: Shell model studies along the N~126 line

In box: E(4+)/E(2+) ratio

Even-even nuclei around 208Pb

Page 5: Shell model studies along the N~126 line

π

ν

In the beta decay of the r-process path nuclei:The FF ν i13/2 -> πh11/2 dominates; also GT νh9/2 ->πh11/2

Page 6: Shell model studies along the N~126 line

Zs. Podolyák et al., Phys. Lett. B 672 (2009) 116.

Internal charged particle decay

Internal gamma decay

205Au: three proton-hole nucleus

Gammas following beta decay

AIDA will do much better with conversion electrons

Page 7: Shell model studies along the N~126 line

Shell-model calculations (M.Górska, H.Grawe, H. Maier, A.Brown)

(a)and (d):TBME from L.Rydstrom et al, NPA512(1990)217 (based on Kuo-Brown interaction)

(b) and (c): three TBMEs modified

Δ(d3/2 h11/2; d3/2 h11/2)7- = +135 keV

Δ(s1/2 d5/2; s1/2 d5/2)2+,3+ =+230 keV (monopole only)

Δ(d3/2 h11/2; s1/2 h11/2)6- changed to +0.160 MeV (fit for B(E2)

Good description of energies and B(EL)s

S.Steer et al., Phys. Rev C78 (2008) 061302(R)

Page 8: Shell model studies along the N~126 line

Variation of key non-diagonal TBME to fit E2 strengths. The effective proton charge used in the SM is 1.35 e which is smaller than the adopted value of 1.5 e. Note that the upper experimental limit for the 7- → 5- is increased by a factor of about five if the (unknown) transition energy is below the Pt M edge. The vertical dashed line represents the adopted TBME value, which is given in MeV.

Page 9: Shell model studies along the N~126 line

203Ir

b) modified; a) original

Page 10: Shell model studies along the N~126 line

Effective charges: 1.5e for E2 and 2.0e for E3 (to reproduce 206Hg)

Transition strengths in N=126 nuclei

Good description of N=126 nuclei after small modifications of TBMEs

203Ir B(E2:23/2+->19/2+) 0.02(1)b) 3.58 0.013

Page 11: Shell model studies along the N~126 line

N=125; Z=78 203Pt

Page 12: Shell model studies along the N~126 line

Structure:N=126 nuclei (205Au, 204Pt, 203Ir)

changes in TBME helps/neededN=128 nuclei (208Hg,209Tl)

agreement with shell modelN<126 nuclei (203Pt etc)

shell model has difficulties

Conclusions

Page 13: Shell model studies along the N~126 line

Approved experiment on the book205Au: beta decay from 205Pt => will fix the πs1/2 orbital203Ir: beta decay from 203Os (νg9/2) => will fix the πd3/2,πs1/2,πh11/2 202Os: isomeric decay I=(5),(7),(10)202Os: beta decay of 203Ir (νg9/2)

3/2+ 0

1/2+ 240

11/2- 921

0+ 0

2+ 1181

4+ 1555

7- 1893

5- 1932

10+ 26738- 2558

8+ 2685

205Au202Os

shel

l mod

el+fast-timing measurements:206Hg: 7- -> 5- ~1.2ns(1W.u.)…

Future