The Mermin-Ho and Anderson-Toulouse coreless non-singular vortices are demonstrated to be thermodynamically stable in ferromagnetic spinor Bose-Einstein condensates with the hyperfine state F = 1. The phase diagram is established in a plane of the rotation drive vs the total magnetization by comparing the energies for other competing non-axis-symmetric or singular vortices. Their stability is also checked by evaluating collective modes.PACS numbers: 03.75. Fi, 67.57.Fg, 05.30.Jp Topological structure plays an important and decisive role in various research fields, ranging from condensed matter physics to high energy physics. They provide a common framework to connect diverse fields, enhancing mutual understanding [1].Recent advance of experimental techniques on BoseEinstein condensation (BEC) prompts us to closely and seriously look into theoretical possibilities which were mere imagination for theoreticians in this field. This is particularly true for spinor BEC where all hyperfine states of an atom Bose-condensed simultaneously, keeping these "spin" states degenerate and active. Recently, Barrett at al [3] have succeeded in cooling 87 Rb with the hyperfine state F = 1 by all optical methods without resorting to a usual magnetic trap in which the internal degrees of freedom is frozen. Since the spin interaction of the 87 Rb atomic system is ferromagnetic, based on the refined calculation of the atomic interaction parameters by Klausen at al[4], we now obtain concrete examples of the three component spinor BEC (F = 1, m F = 1, 0, −1) for both antiferromagnetic ( 23 Na) [5] and ferromagnetic interaction cases. In the present spinor BEC the degenerate internal degrees of freedom play an essential role to determine the fundamental physical properties. There is a rich variety of topological defect structures, which are already predicted in the earlier studies [6,7] on the spinor BEC. These are followed by others [8,9,10,11,12,13,14,15,16] who examine these topological structures more closely, such as skyrmion, monopole, meron or axis-symmetric or non axis-symmetric vortices both for antiferromagnetic and ferromagnetic cases.Superfluid 3 He is analogous to the spinor BEC where the neutral Cooper pair possesses the orbital and spin degrees of freedom, thus the order parameter is a multi-component [17]. Among various topological structures, the Mermin-Ho (MH) [18] and Anderson-Toulouse (AT) [19] vortices of a coreless and non-singular l-vector texture are proposed in 3 He-A phase. These are an extremely interesting object to study if they exist. The MH vortex is expected to spontaneously appear in a cylindrical vessel without any external rotation as an equilibrium state because the rigid wall boundary imposes the l-vector perpendicular to the vessel wall. The MH vortex is stable also under slow rotation because of their non-singular coreless structures [20].A similar topological structure, called skyrmion in general is proposed in the spinor BEC. Khawaja and Stoof[10] study a skyrmion in the ferromagnetic BEC with ...