A famous and long-standing problem so-called the “mysterious” 0+ state in 16O is discussed with a single scheme, a 12C plus four-nucleon five-body model. The wave function is expressed in terms of explicitly correlated Gaussian functions. Preliminary results show that the energy levels are in good agreement with experiment. A welldeveloped 12C+α cluster structure appears in the first excited 0+ state, whereas the ground state has shell model like structure
Gas-like α cluster states are investigated in 16O with the use of 4α OCM (orthogonality condition mo...
The 4α condensate state for 16O is discussed with the Tohsaki-Horiuchi-Schuck-Röpke (THSR) wave func...
We introduce the so-called Tohsaki-Horiuchi-Schuck-Röpke (THSR) wave function to describe various nu...
A famous and long-standing problem so-called the “mysterious” 0+ state in 16O is discussed with a si...
We calculate the low-lying spectrum of the $^{16}$O nucleus using an α-cluster model which includes ...
We report converged results for the ground and excited states and matter density of 16-O using reali...
The 16O spectrum is investigated microscopically in a multiconfiguration generator-coordinate basis,...
In order to explore the 4α-particle condensate state in 16O, we solve a full four-body equation of m...
In many previous calculations within microscopic models, the binding energy differ-ence between 12C ...
We use the Generator Coordinate Method to investigate some nuclei between A = 12 and A = 16 in a mul...
The O+ levels in 16O are considered in terms of the nuclear shell model, with zero range nuclear for...
α + 12C clustering in 16O has been vigorously studied. In the 2000s, a new picture was proposed that...
The 13C(α,n)16O reaction is studied in a microscopic multicluster model, where the 13C and 16O nucle...
12C and 16O nuclei are investigated within nonmicroscopic and microscopic theoretical frameworks, re...
We develop an approach for a unified description of bound and unbound states in the framework of the...
Gas-like α cluster states are investigated in 16O with the use of 4α OCM (orthogonality condition mo...
The 4α condensate state for 16O is discussed with the Tohsaki-Horiuchi-Schuck-Röpke (THSR) wave func...
We introduce the so-called Tohsaki-Horiuchi-Schuck-Röpke (THSR) wave function to describe various nu...
A famous and long-standing problem so-called the “mysterious” 0+ state in 16O is discussed with a si...
We calculate the low-lying spectrum of the $^{16}$O nucleus using an α-cluster model which includes ...
We report converged results for the ground and excited states and matter density of 16-O using reali...
The 16O spectrum is investigated microscopically in a multiconfiguration generator-coordinate basis,...
In order to explore the 4α-particle condensate state in 16O, we solve a full four-body equation of m...
In many previous calculations within microscopic models, the binding energy differ-ence between 12C ...
We use the Generator Coordinate Method to investigate some nuclei between A = 12 and A = 16 in a mul...
The O+ levels in 16O are considered in terms of the nuclear shell model, with zero range nuclear for...
α + 12C clustering in 16O has been vigorously studied. In the 2000s, a new picture was proposed that...
The 13C(α,n)16O reaction is studied in a microscopic multicluster model, where the 13C and 16O nucle...
12C and 16O nuclei are investigated within nonmicroscopic and microscopic theoretical frameworks, re...
We develop an approach for a unified description of bound and unbound states in the framework of the...
Gas-like α cluster states are investigated in 16O with the use of 4α OCM (orthogonality condition mo...
The 4α condensate state for 16O is discussed with the Tohsaki-Horiuchi-Schuck-Röpke (THSR) wave func...
We introduce the so-called Tohsaki-Horiuchi-Schuck-Röpke (THSR) wave function to describe various nu...
DOI
Add to ORKG