Prevailing Triaxial Shapes in Heavy Nuclei Driven by \pi Meson

Virtually any object can rotate. While the rotation provides various intriguing physics cases, the primary picture for atomic nuclei was simple. Rotational bands have been observed for many nuclei, and their basic picture is considered to have been established in 1950s. We, however, show that this traditional picture is superseded with a novel picture arising from basic characteristics of the nuclear forces. In the traditional view, as stressed by Aage Bohr in his Nobel lecture, most of heavy nuclei are like axially-symmetric prolate ellipsoids (i.e., with two shorter axes of equal length), rotating about one of the short axes, like a rod. In the present picture, however, in many cases, the lengths of these three axes are all different, called triaxial. The triaxial shape yields more complex rotations, which actually reproduce experimental data as shown by state-of-the-art Configuration Interaction calculations, on supercomputers. The key to differentiate the two pictures is the nuclear tensor force, which is known to produce the shell evolution in exotic nuclei, a major agenda of Rare-Isotope physics. We now demonstrate that the same tensor force generates, in many nuclei, the triaxiality, fading the prolate-ellipsoid dominance away. The tensor force is a direct consequence of one $\pi$ meson exchange between nucleons, and the present finding is regarded as the first explicit or visible case that elementary particles directly affect nuclear shapes. The importance of the explicit tensor force is in the same line as Weinberg's modeling of nuclear forces. This feature makes the new picture robust, and may cast challenges for other many-body systems having spin-dependent forces. Substantial impacts on superheavy nuclei and fission are anticipated. This study sheds lights on the earlier suggestion of dominant triaxiality by Davydov, a Ukrainian physicist.