Takuma Matsumoto (Kyushu Univ.)
description
Transcript of Takuma Matsumoto (Kyushu Univ.)
Takuma Matsumoto(Kyushu Univ.)
Analyses of breakup, one- and two-neutron removal reactions for three-body projectile
Contents
• Introduction
• Breakup of Borromean Nuclei
• Breakup of Samba Nuclei
• Summary
Introduction
Nuclear and Coulomb
Target
Unstable Nuclei
The unstable nuclear structure can be efficiently
investigated via the breakup reactions. Inelastic cross section
Breakup cross section
Momentum distribution of emitted particles
An accurate method of treating breakup processes
is needed.
Structure information
n + n + Core System Borromean nuclei
No bound sub-system (n + core) Two-neutron halo or skin structure 6He, 11Li, 14Be Breakup
n + n + core three-body channel
Samba nuclei Existence of bound sub-system (n + core) One-neutron halo structure (n + core sub-system) 12Be, 16C, 20C Breakup
n + n + core three-boy channel n + n-core two-body channel
CDCC
Breakup = Coupling to Continuumnuclear or/and Coulomb
Four-Body Breakup Reaction
CDCC method• Developed by Kyushu Univ. group• Fully quantum method• Treats breakup states explicitly
Essence of CDCC• Breakup continuum states are described by a finite number of discretized continuum states
• A set of eigenstates forms a complete set within a finite model space that is important for breakup processes
M. Yahiro, K. Ogata, T.M., K. Minomo, PTEP 2012(1), 01A206.
Channel 1 Channel 2 Channel 3
n n n nn
n
4He 4He 4He
Ground and Breakup States of 6He 6He : n + n + 4He (three-body model) Gaussian Expansion Method : E. Hiyama et al., Prog. Part. Nucl. Phys. 51, 223
An accurate method of solving few-body problems. A variational method with Gaussian basis functions Take all the sets of Jacobi coordinates
Ip=0+ Ip=1- Ip=2+
Exc
itatio
n en
ergy
of 6 H
e [M
eV]
ELASTIC SCATTERING OF 6HE
4He
n
n
6He12C
6He (n+n+4He) + 12C elastic scattering
initial final
0+ 2+1-
Double-folding model
vNN:DDM3Y → no imaginary part
Transition density
R
srTrp
ground state density
Coupling Potential (Double Folding)
Elastic Cross Section of 6He + 12C T.M. Hiyama, Ogata, Iseri, Kamimura, Chiba, and Yahiro, Phys. Rev. C70, 061601 (2004).
4He
n
n
6He209Bi
6He (n+n+4He) + 209Bi scattering
4He
n
n
initial final
Cluster folding model
VnBiVnBi
VaBi
Optical potentials are folded with the transition densities of 6He.
No free parameter
VaBi includes the Coulomb interaction
Coupling Potential (Cluster Folding)
Other calculationsM. Rodríguez-Gallardo, J. M. Arias, J. Gómez-Camacho, R. C. Johnson, A. M. Moro, J. Thompson, and J. A. Tostevin, PRC 77, 064609 (2008)
Elastic Cross Section 6He + 209Bi T.M. Egami, Ogata, Iseri, Kamimura, and Yahiro, Phys. Rev. C73, 051602 (2006).
BREAKUP CROSS SECTION OF 6HE
Breakup Cross SectionBreakup cross sections calculated by CDCC are discrete in the internal energy of the projectile.
PRC59, 1252(1999), T. Aumann et al.
E* (MeV)
s (m
b)
6He+12C scattering at 240 MeV/nucl.4-body CDCC calc.
How to calculate the continuum breakup cross section
New description of continuum breakup cross section with Complex-scaling method (CSM).
T.M., K. Kato, and M. Yahiro, PRC82, 051602 (2010).
The Cauchy integral contour for the completeness relation
Complex-scaling operator:
Coordinate:
Momentum:
k Im[k]
Re[k]
}Bound states
Resonance
Continuum
Useful for searching many-body resonances
Complex Scaling Method (CSM)
Green’s function with Complex-Scaling Method (CDCS Green’s function)
Asymptotic form of the outgoing wave
S. Aoyama, T. Myo, K. Kato, and K. Ikeda,Prog. Theor. Phys. 116, 1 (2006)
New Smoothing Procedure with CSM
Final state of the projectileResponse function
T-matrix calculated by CDCC
Green’s function with Complex-Scaling Method (CDCS Green’s function)
T.M., K. Kato, and M. Yahiro, PRC82, 051602 (2010).
New description of differential breakup cross section
Differential Breakup Cross Section
6He+12C scattering @ 240 MeV/nucl.
Exp. data from PRC59, 1252 (1999), T. Aumann et al.
Underestimation → Inelastic breakup effect ~ 20%
Nuclear Breakup is dominant
6He+208Pb scattering @ 240 MeV/nucl.
Exp. data from PRC59, 1252 (1999), T. Aumann et al.
Underestimation → Inelastic breakup effect
Overestimation ???
Coulomb Breakup is dominant
ONE- AND TWO-NEUTRON REMOVAL REACTION OF 6HE
Breakdown for Coulomb breakup!
Reaction theories
Glauber model
Eikonal approximation + adiabatic approximation
A new theory to treat the inclusive reactions accurately was proposed.
Eikonal reaction theory (ERT)→ one- and two-neutron stripping and removal cross
sections
○Exclusive reaction ○Inclusive reaction
M. Yahiro, K. Ogata, K. Minomo, PTP126, 167 (2011).
M. Yahiro, K. Ogata, T.M., K. Minomo, PTEP 2012(1), 01A206.
The method of Continuum-Discretized Coupled Channels (CDCC)
○Exclusive reaction ×Inclusive reaction
Two-neutron removal from 6He
Good agreement!
2n removalT. Aumann, et al. PRC59, 1252 (1999).
SAMBA NUCLEI
Samba nuclei
• Sub-bound state• core + n (bound)• n-n (unbound)
• Breakup channel• Core + n + n (Three-body breakup channel)• (Core + n)bound + n (Two-body breakup channel)
n
n
10Be
12Be
Because of existence of two breakup channels, we have to distinguish two-body breakup from three-body breakup channels.
Breakup of 12Be
target
(10Be + n + n)
(11Be + n)
Complete BU
Incomplete BU
11Be
10Be
n
n
10Be
12Be
In principle, this breakup process can be analyzed by four-body CDCC framework.
Discretized continuum of 12BeModel Hamiltonian of n + n + 10Be n-10Be interaciton
Phys. Rev. C62 034305, Aoyama n-n interaction
Phys. Lett. B32 591, Gogny et al. Phenomenological 3-body force and OCM
n + n + 10Be
n + 11Be
Discretized states include two components, complete BU and incomplete BU states.
BU cross section calculated by CDCC includes two components.
How to distinguish incomplete BU from complete BU
Probability of 11Be in 12BeWave functions of 12Be
Probability of 11Be ground state component in 12Be
Ground state Pi ~ 0.89 (89 %) Breakup cross sections for n + 11Be channel and n + n + 10Be
σ 𝐵𝑈 (𝑖𝑛𝑐𝑜𝑚𝑝𝑙𝑒𝑡𝑒 )=∑𝑖𝑃 𝑖𝜎 𝑖 ,𝜎𝐵𝑈 (𝑐𝑜𝑚𝑝𝑙𝑒𝑡𝑒 )=∑
𝑖(1−𝑃 𝑖 )𝜎 𝑖
12Be + Si @ 50 MeV/A
Pi=0.61 (61%)
Pi=0.57 (57%)
Pi=0.05 (5%)
Pi=0.03(3%)
Pi=0.89 (61%)
Calculation (preliminary)
BU(complete) : 54 mbBU(incomplete) : 20 mb
𝜎 (𝑐𝑜𝑚𝑝𝑙𝑒𝑡𝑒 )>𝜎 (𝑖𝑛𝑐𝑜𝑚𝑝𝑙𝑒𝑡𝑒)
Phys. Rev. C64, 044601Experiment
𝜎 ¿140 mb 100 mb
11Be is a halo nucleus
Continuum Breakup Cross Section
n + n + 10Be Breakup
?
n + 11Be Breakup
?
Summary We propose a new smoothing method with the complex scaling method to obtain continuous breakup cross sections.
The new smoothing method is applied to analyses for 6He breakup reactions on 12C and 208Pb at 240 MeV/A.
Inclusive cross sections of three-body projectile are calculated by Eikonal reaction theory.
For breakup of Samba nuclei, we have to consider two breakup channels, complete and incomplete breakup.
Prog. in part. and nucl. Phys. 67, 9390994 (2012)