why are we (in general) interested in q?

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First combined DSAM and Coulex experiment at REX-ISOLDE – measuring the sign of the spectroscopic quadrupole moment of the 2 1 + state in neutron-rich 140 Ba * 8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer Christopher Baue r 1 , Jörg Leske 1 , Thorsten Kröll 1 , Norbert Pietralla 1 , Vinzenz Bildstein 2 , Roman Gernhäuser 2 , Reiner Krücken 2 , Rudi Lutter 3 , Chavdar Stoyanov 4 , Dimitar Tarpanov 4 1 Institut fr Kernphysik, TU Darmstadt, 64289 Darmstadt 2 Physik-Department E12, TU Mnchen, 85748 Garching 3 Maier-Leibnitz-Laboratorium, LMU Mnchen, 85748 Garching 4 Institute for Nuclear Research and Nuclear Energy, 1784 Sofia, Bulgaria *supported by the BMBF (06 DA 9040 I) and HIC for FAIR

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First combined DSAM and Coulex experiment at REX-ISOLDE – measuring the sign of the spectroscopic quadrupole moment of the 2 1 + state in neutron-rich 140 Ba *. - PowerPoint PPT Presentation

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Page 1: Why are we (in general) interested in Q?

First combined DSAM and Coulex experiment at REX-ISOLDE – measuring the sign of the spectroscopic quadrupole moment of the 21

+ state in neutron-rich 140Ba *

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

Christopher Bauer1, Jörg Leske1, Thorsten Kröll1, Norbert Pietralla1, Vinzenz Bildstein2, Roman Gernhäuser2, Reiner Krücken2, Rudi Lutter3,

Chavdar Stoyanov4, Dimitar Tarpanov4

1Institut fur Kernphysik, TU Darmstadt, 64289 Darmstadt 2Physik-Department E12, TU Munchen, 85748 Garching 3Maier-Leibnitz-Laboratorium, LMU Munchen, 85748 Garching 4Institute for Nuclear Research and Nuclear Energy, 1784 Sofia, Bulgaria

*supported by theBMBF (06 DA 9040 I) and HIC for FAIR

Page 2: Why are we (in general) interested in Q?

Why are we (in general) interested in Q?

Q describes the deviation of the charge distribution from spherical symmetry in a nucleus

The intrinsic quadrupole moment Q0 (in the reference frame of the nucleus) is related to the deformation parameter β by

The observable is the spectroscopic quadrupole moment Q, which is related to Q0 in the case of the first 2+ state by

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

Page 3: Why are we (in general) interested in Q?

The diagonal matrix element

The matrix elements are evaluated from measured yields / cross-sections in comparison with Coulomb excitation calculations

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

2+

0+

M20

M22

Page 4: Why are we (in general) interested in Q?

The idea

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

With new lifetime informationthe situation changes dramatically

Page 5: Why are we (in general) interested in Q?

ExperimentMINIBALL at REX-ISOLDE (IS411)

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

CD detector

MINIBALL

γ

θγ

γ

θp

RIB140Ba

96Mo

Z=50

N=

82

Barium (Z=56)

140Ba

132Sn

Ebeam = 392 MeV

Target: 1mg/cm2 96Mo

Page 6: Why are we (in general) interested in Q?

DSAM analysis

Additional run

natCu target(thickness: 1mm)

140Ba is stopped

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

Time difference [µs]

Energy [keV]

raw spectrum

backgroundsubtracted

602 keV

602 keV

Page 7: Why are we (in general) interested in Q?

DSAM analysis: Fit

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

The DSAM fit was done by J. Leske.

= 12.5(6) ps

20 individual fits for each MB Ge core in this experiment

weighted average

Page 8: Why are we (in general) interested in Q?

Coulex cross-section

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

The cross-section is sensitive on the

quadrupole moment!

The cross-section is sensitive on the

quadrupole moment!

SensitivityS = (Q+-Q-)/Q0

Page 9: Why are we (in general) interested in Q?

Complete statistics

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

The new determined lifetime fixes the M20

matrix element.

The new determined lifetime fixes the M20

matrix element.

Old lifetime: 14(6) psNew Lifetime: 12.5(6) ps

Page 10: Why are we (in general) interested in Q?

Splitted statistics

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

Comparison to theory

QPM: Q = 0.1(M22 = 0.13)

The quadrupole moment must be

positive!-> OBLATE SHAPE

The quadrupole moment must be

positive!-> OBLATE SHAPE

Page 11: Why are we (in general) interested in Q?

e-

Recoil-in-vacuum

15.4.2010 | MINIBALL Workshop Leuven | IKP Darmstadt | Christopher Bauer

Ion beam

(140,142Ba)

96Mo

(0.9mg/cm2)

Ion beam

(140,142Ba)

natCu (892mg/cm2)

I

I

J

F

γ

γ

Page 12: Why are we (in general) interested in Q?

Angular Distributions

Thick target: natCu 142Ba, distribution for 360 keV line ( )

15.4.2010 | MINIBALL Workshop Leuven | IKP Darmstadt | Christopher Bauer

Page 13: Why are we (in general) interested in Q?

g factor

Limit for g ( ) in 140Ba is |g|≤0.38 RIV method is applicable But need appropriate calibration isotope(s)

8.12.2010 | ISOLDE workshop | TU Darmstadt | Christopher Bauer

Page 14: Why are we (in general) interested in Q?

Summary

Results

140Ba Coulex evaluation Lifetime:

= 14(6) ps 12.5(6) ps21(9) W.u. 18.8(9) W.u.

Qspec > 0 oblate shape

RIV method First time tested at REX-ISOLDE Limit for g( )-factor in 140Ba

|g|≤0.38

Conclusions

Both methods are complementary to standard MINIBALL experiments Need extra run with suitable

thicker target for DSAM

Need extra runs for distribution without deorientation and with calibration isotope(s)g factor

Be aware of contamination!

15.4.2010 | MINIBALL Workshop Leuven | IKP Darmstadt | Christopher Bauer

Thank you for your attention!

Thank you for your attention!