“…Recently, imaging systems for positron annihilation gamma rays, such as positron emission tomography and planar positron imaging systems (PPIS), have been vigorously applied to plant research. [1][2][3] Although positron imaging experiments have the advantage of visualizing the dynamics of nutrient and toxic elements by using positron-emitting radioisotopes such as 11 C (T 1/2 : 20.36 min), 4-7) 1 3 N (9.97 min), [8][9][10] 64 Cu (12.70 h), 11) 74 As (17.77 d) 12) and 107 Cd (6.50 h) [13][14][15][16][17][18][19][20][21] produced by using cyclotrons, they have the disadvantage of not being able to visualize commercially or non-commercially available radioisotopes emitting single gamma rays such as 42 K (T 1/2 : 12,36 d, main gamma-ray energy: 1525 keV, main gamma-ray intensity: 18.1%) 43 K (22.30 d, 373 keV, 86.8%), 54 Mn (312.05 d, 835 keV, 100%), 59 Fe (44.50 d, 1099 keV, 56.5%), and 137 Cs (30.08 y, 662 keV, 85.1%). This disadvantage causes a limitation in facilitating the research on elemental dynamics in plants.…”