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Spins, Moments and Charge Radii Beyond Spins, Moments and Charge Radii Beyond

Spins, Moments and Charge Radii Beyond - PowerPoint Presentation

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Spins, Moments and Charge Radii Beyond - PPT Presentation

48 Ca INTCP313 ML Bissell On behalf of COLLAPS Background     Program initiated with IS484 Groundstate properties of Kisotopes from laser and β NMR spectroscopy ID: 508136

stage shifts charge radii shifts stage radii charge theory moments ground detection state rilis oes ucx measurements yield shutdown

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Slide1

Spins, Moments and Charge Radii Beyond 48CaINTC-P-313

M.L. Bissell - On behalf of COLLAPS Slide2

Background

 

 

Program initiated with IS-484 -

Ground-state properties

of

K-isotopes from laser and

β

-NMR

spectroscopy

Extended with

I-117 -

“Moments, Spins and Charge Radii Beyond

48

Ca.”

Substantial theoretical interest and recent developments encourage us to bring forward part of this programSlide3

New magic numbers N = 32, 34

 

 

Whilst β-decay spectroscopy, deep inelastic scattering and Coulomb-excitation experiments have all provided evidence for a sub-shell closure at

N

=32, no direct experimental evidence exists for such a closure at

N

=34.

Maierbeck

et al., Phys.

Lett. B 675, 22 (2009)-> 55Ti has a 1/2− ground state. GXPF1A predicts this , KB3G predicts 5/2 −

A.Gade

, T.

Glasmacher

, Progress in Particle and Nuclear Physics 60, 161–224 (2008)

54

Ca

is “the key nucleus for a search for the new magic number

N=34.”Slide4

Ca: An ideal testing ground for theory

 

 

Gaute

Hagen (Oak Ridge) :

“ I

think it would really great idea for a proposal to measure the neutron rich

calciums

. We can within coupled-cluster theory compute radii, masses, spectra and moments of

39,40,41,47,48,49,51,50,52,53,54,55,59,60,61

Ca.

So basically its only a few calciums we cannot compute at the moment. To have experiments measure radii and moments of the n-Ca would be of really huge interest for the theory community and provide tests for ab-initio approaches. ”Slide5

Ca: An ideal testing ground for theory

 

 

Existing charge radii of Ca are probably the most theoretically investigated of any isotopic chain:

I.Talami

,

Nucl

. Phys. A 423, 189 (1984

)

->

Linear

+ Parabolic + OESEach of these terms related to particular components of the interaction used. Slide6

Charge radii beyond 48Ca

 

 

Fe

-> Normal OES

Mn

-> Downturn at

N

=31 but could be just OES.

IS-508 will extend this beyond

N

=32 K -> Preliminary results indicate a downturn at N=32. Statistics to be improved. Slide7

Only old SC yields available on the database:49Ca 2.5x105 /

uC

Old design

UCx49Ca 1.4x10

7 /uC Ta (Should be equivalent to new UCx)51Ca 1.0x104 /uC Ta powder (last yield measurements for

51

K claimed we had approximately equal amount of K and Ca)

52

Ca 1.0x10

2

/uC T. Stora- Yield will be 1 order of

magnitude higher than this. (All yield measurements at the PSB have been in the 1x103 range.)+ Possible factor of 10 from RILIS

YieldsSlide8

Stage 1 – Optical detection

Optical detection efficiency for K improved from

1 : 300 k

to

1 in 20 k+ low background .

η

(new)

dx

/ ∫η

(existing) dx ≈14For Cd we observed 1 in 6k -> 1 in 4k for CaSlide9

What is possible?

Strong ionic

J

=1/2 to

J=3/2 393.4 nm transition.4 shifts on 52Ca with 1k ions /μ

C

3 Such spectra required to reduce

systmatics

+ 5 shifts for

51Ca+ 1 shift for

49Ca+ 3 offline shifts directly prior to the run for stable measurements.Stage 1 total 18 online shifts + 3 offline.Slide10

Stage 2 – Radioactive detection

Radioactive

detection

of Optically pumped ions after state selective

Charge exchange (ROC)

The theoretical

possibilities:

1 ion/s of an even isotope over 5 shifts.

An additional

18 shifts

53,54

CaSlide11

Why is stage 2 stage 2?

ROC is not ideally suited to odd cases. We must introduce multiple pumping.

In the previous setup it was not possible to reliably focus both the ion and atom beam onto the detectors.

-> Shutdown will be an ideal time to develop this.Slide12

Summary of Request

Stage 1 – Investigation of

N

=32

18 shifts

with

UCx

and RILIS prior to shutdown

.

Stage

2 – Investigation of N=3418 shifts with UCx and RILIS after the shutdown .Slide13

Collaboration

M. L. Bissell,

1

K. Blaum,

2

I. Budincevic,

1

N.Frömmgen,

3

R.F. Garcia Ruiz,

1

Ch. Geppert,

3

M. Hammen,

3

M. Kowalska,

4

K. Kreim,

2

P. Lievens,

5

R. Neugart,

3

G. Neyens,

1

W. Nörtershäuser,

3

J. Papuga

1

, M.M. Rajabali

1

and D. T. Yordanov

4