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Recent Theoretical Advances in Nuclear ClusterPhysics

P. Schuck

IPN Orsay and LPMMC Grenoble

CONTENT

The situation of alpha cluster states in 12C

The situation in 16O and heavier

Monopole transitions and alpha clustering in 16O, etc.

Extension of THSR to include valence neutrons

Alpha condensation in infinite matter

Alpha decay of 212Po

Alpha-rings

Conclusions

Hoyle family

arXiv:1802.03523, to appearMaasaki KIMURA; Yasuro FUNAKI PRC 92,021302; C. Kurokawa, K. Kato: 3rd and 4th 0+ states, NPA 792, 87

Transition probabilities

Inelastic form factor to Hoyle state (Funaki et al.); very good agreementwith data with no adjustable parameter! THSR and GFMC; Los Alamos,Pieper et al.

0 1 2 3 410-4

10-3

10-2

10-1

k (fm-1)

f pt(

k)

VMC

GFMC

Experiment

0 0.2 0.40

1

2

3

4

5

6

k2 (fm-2)

6 Z

ftr

(k)

/ k2

(

fm2)

10−9

10−8

10−7

10−6

10−5

10−4

10−3

10−2

0 0.5 1 1.5 2 2.5 3 3.5

(dσ/d

Ω)/

(dσ/d

Ω) M

ott

q [fm−1]

THSR (01+ → 02

+)

Very sensitive to size of Hoyle state! VHoyle

Vg.s.∼ 4

Yasuro FUNAKI et al., Phys. Scripta 91, 123001 (2016)Kamimura, Uegaki, T. Neff et al.

Freer et al., also Cseh, but P. O. Hess: Pauli very important!!

AMD, from Kanada-En’yo:

y (f

m)

x (fm)

0

0.8

0.4

-4

-2

0

2

4

-4 -2 0 2 4

(fm )−2

T. Otsuka et al.: No core SM

also J. Draayer et al., K. Launey No inelastic form factor so far!

Radius of second 2+ state in 12C: Makoto ITO: to appear in PRC

Alpha condensation, 3-alpha decay out of Hoyle:S. Ishikawa

0

0.2

0.4

0.6

0.8

1.0

µλ

Ground state Hoyle state

S1 D1 G1 S2 D2 G2 S3 D3 G3 S1 D1 G1 S2 D2 G2 S3 D3 G3

S-wave dominance: 80 percent

Meissner et al., PRL 109, 252501 Lattice QMC; lattice spacing: 2fm

Yasuro FUNAKI: extended THSR for 4 alpha’s in 16O, PRC 97, 021304.experimental problem with 6-th +0 state around 15.1 MeV

|THSR− 16O〉 = α+α+α+α+|vacuum〉

Taiichi YAMADA: Monopole transitions in 16O:

Neutron separation of 8-11Be

PRC 93, 054308 (2017)

M. Kimura: 14, 16C, chain states

Alpha condensation in infinite matter, Sogo et al., PRC 81, 064310

Quantum Phase Transition in infinite matter and 16O

Lazauskas, Sogo et al., PRC 79, 051301

0

0.1

0.2

0.3

0.4

0 0.5 1 1.5 2 2.5

nk

k (fm-1

)

µ = −5.26 MeV

µ = −1.63 MeV

µ = 0.55 MeV

QPT in finite nucleiGogny force D1S, M. Girod; ’RMF’, JP. Ebran

Alpha pocket at the surface of 208PbChang Xu, G. Roepke et al., PRC 95; Double folding: Adamian et al.,PRC 94

Future challenge: alpha decay of deformed 226Ra

Alpha-ring: M. Girod et al., J.Phys. G 37, 064012 (2010)7-alpha ring measured?? Nature-article: Natowitz et al.

ConclusionsImmense activity in nuclear cluster physicsMostly for self-conjugate nuclei but also with valence neutrons (protons)Progress with Hoyle family of states in 12CSome progress with alpha gas states in 16O but experimental ambiguities withsixth zero plus state at about 15.1 MeVAlpha-condensation is a Quantum-Phase-transitionAlpha-decay 212PoAlpha rings

All started with this....THANK YOU!

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