We discuss the effect of a strong magnetic field on the chemical freezeout points in the ultrarelativistic heavy-ion collision. As a result of the inverse magnetic catalysis or the magnetic inhibition, the crossover onset to hot and dense matter out of quarks and gluons should be shifted to a lower temperature. To quantify this shift we employ the hadron resonance gas model and an empirical condition for the chemical freezeout. We point out that the charged particle abundances are significantly affected by the magnetic field so that the electric charge fluctuation is largely enhanced especially at high baryon density. The charge conservation partially cancels the enhancement but our calculation shows that the electric charge fluctuation and the charge chemical potential could serve as a magnetometer. We find that the fluctuation exhibits a crossover behavior rapidly increased for eB (0.4 GeV) 2 , while the charge chemical potential has better sensitivity to the magnetic field. Introduction: Magnetic fields provide us with a useful probe to reveal non-trivial topological contents of the ground state of matter or the vacuum in quantum field theories. Dynamics of quarks, gluons, and composites is also significantly affected by an external magnetic field if its strength is comparable to the typical scale in quantum chromodynamics (QCD); i.e. Λ QCD ∼ 0.2 GeV. There are many works dedicated to strong magnetic field effects in the condensed matter and the neutron star environment [1, 2], in the early universe [3], and recently, more and more theoretical and experimental studies have been inspired by a possibility of gigantic magnetic fields created in the ultra-relativistic heavy-ion collision [4]. There are transport model simulations [5] that have verified an order estimate by simple classical modeling, leading to a compact formula [6,7]: eB(t) = eB 0 [1+(t/t 0 ) 2 ] −3/2 with eB 0 (0.05GeV) 2 (1fm/b) 2 Z sinh Y where the atomic number is Z = 79 in the Au-Au collision and the beam rapidity can be approximated as sinh Y √ s N N /(2m N )