Methyl radicals are trapped in the solid Kr film by simultaneous condensation of gaseous Kr and the products of the gas discharge in CH 4 doped Kr on the low temperature (4.2 K) substrate located at the center of the microwave cavity. The observed EPR spectrum is a superposition of broad-line and narrow-line series. At a low resonance microwave power, the latter one consists of four hyperfine components with nearly equal intensities, and shows small axial anisotropy of both g-and A-tensors. At a sufficiently large power, two central narrow lines split so that the narrow-line series takes an appearance recorded elsewhere for CH 3 in Ar at higher temperatures above 12 K. Simultaneously, the intensity of two central broad lines increases dramatically while the outer components become saturated. The possible explanation is discussed.PACS: 76.30.Rn Free radicals; 32.30.Rj X-ray spectra.Keywords: EPR, methyl radicals, matrix isolation, rotation.Methyl radical, CH 3 , is among the simplest polyatomic molecules which attract attention of both experimentalists and theoreticians in attempting to verify theoretical approaches used to analyze characteristics of a molecule in various substances. For example, a theory predicts a fairly large anisotropy of the proton hyperfine tensor for the free CH 3 molecule. While the anisotropy was actually observed with CH 3 radicals in CH 3 COONa×3D 2 O monocrystal [1], only symmetrical hyperfine lines were obtained in powder samples, which suggest practically isotropic interaction. This is closely related to the rotational motion of the CH 3 radical in such matrices as frozen gases which averages out the hyperfine components, A xx and A yy , yielding a spectrum of axial symmetry with the perpendicu- It is quite reasonable to attribute the difference in the DA signs for the free and trapped molecules to a different effect a matrix has on A^and A || parameters. The nonzero Dg is, probably, a fingerprint of the nonplanar structure of the trapped methyl radical [6]. It has been shown earlier [4] that DA < 0 for both Ar and Kr matrices while Dg is negative for Ar and positive for Kr. The whole set of experimental data was noncontradictory explained assuming fast rotation of the molecule around its C 3 axis in CO, Ar and Kr while the reorientation of this axis is suppressed in the matrix with orientation ordering, CO, and occurs through, possibly, tunneling motion in Ar and Kr. Very recently, high-resolution EPR measurements were carried out on CH 3 trapped in solid Ar [7]. With the linewidth of about 0.15 G, the authors were able to resolve a structure of the low field hyperfine component. The splitting of the line is owing to the hyperfine coupling and g-tensor anisotropy. In cases of the broader lines, the anisotropy reveals itself