A close relationship between magnetic helicity injection and magnetic reconnection was observed during double-null formation of spherical tokamak (ST) plasmas. The magnetic reconnection of common flux into private flux causes concentration of current density along the current sheet, forming a high eigen-value area between the helicity source (coil flux) and the ST plasma. The formation of a plasmoid and its translation to core plasma indicate intermittent translation of the high eigen-value area, suggesting a mechanism for helicity injection. . Helicity injection is also observed around the connection region between poloidal coils and ST plasma during double-null merging (DNM) formation in the University of Tokyo Spherical Tokamak (UTST) plasmas. Magnetic helicity is considered to be injected from a helicity source with a high eigen-value into a helicity sink with a low eigen-value. However, helicity injection requires the helicity source, i.e. the coil flux, to be connected with the helicity sink through magnetic field lines. Thus, elucidation of how and why helicity injection is related reconnection processes is necessary. Reconnection generally produces a current sheet and plasmoids, which may directly influence helicity [5][6][7][8]. Few reports that measured the eigen value profiles of spheromaks and RFPs [9, 10] after their relaxation, but that of ST plasma and that during helicity injection are not yet measured. We measured for the first time 2-D eigenvalue profile of around the connecting region between the coil flux and the core plasma flux, and found that both the current sheet and the high eigenvalue plasmoids carry magnetic helicity from the coil region to the ST region.The UTST experiment has demonstrated DNM startup of ST plasmas using two pairs of poloidal field (PF) coils outside the vacuum vessel [11][12][13]. In the late phase of author's e-mail: watanabe@ts.t.u-tokyo.ac.jp DNM formation, a single ST is connected to the external poloidal coil flux. Merging of two ST plasmas through magnetic reconnection was successfully observed by twodimensional pickup coil arrays, which are located in the r-z plane of the vacuum vessel [14]. On the basis of the measured 2-D magnetic field profile, poloidal magnetic flux Ψ , toroidal current density j t and toroidal and poloidal eigen values λ t and λ p respectively are calculated as follows: Ψ = 2π B z R dR, λ t = j t /B t , λ p = j p /B p [15], and,Figure 1 (a) shows the experimental setup of the UTST device and the ST plasma produced in the late phase of DNM formation. Induction by the two pairs of PF coils initially ionizes the neutral gas around their double-null points and then injects toroidal plasma currents into the ST plasma. This process can increase the λ value of the PF coil flux region than that of the ST plasma. Figures 1 (b)-(d) show color contours of the poloidal magnetic flux with j t , λ t and λ p measured inside the dotted area of Fig. 1 (a) at 760 µs after PF coil discharge began. We observed for the first time in plasma experiments that a...