We present here the Ðrst light curves of the peculiar Algol binary system R Canis Majoris obtained in the near-infrared photometric bands J and K. The light curves are Ðtted for a semidetached model with the Wilson-Devinney light-curve synthesis program. The parameters of the system are derived. Published light curves in the optical photometric bands (U, B, V , and of Guinan, V light U n , B n , V n , Hb w , Hb n curve of Sato, and and light curves of Edalati, Khalesse, & Riazi) are reanalyzed and the Ha w Ha n results are compared. The temperature of the secondary component derived from the light-curve T 2 analysis shows an increase toward the near-IR wavelengths, achieving maximum in the K band. The secondary minima are deeper by 0.03 and 0.07 mag and the primary minima are shallower by 0.02 and 0.03 mag in the J and K bands, respectively, than what is expected in these bands from the secondary temperature and primary radius derived from the V band. In the case of the Ha and Hb light curves, the narrowband light curves yielded higher than the broadband light curves. The values of derived T 2 T 2 from these bands are found to be higher than those derived from the light curves observed in the neighboring wavelengths. We consider the possibility of the di †erence in the strength of photospheric absorption of Ha and Hb lines in the primary and the secondary as a reason for the high values of derived T 2 from these light curves.Five epochs of primary minima and four epochs of secondary minima are obtained in the present study. The increased depth of the secondary minima in the near-IR bands compared with the optical bands enabled us to determine the moments of secondary minima with nearly the same accuracy as those of primary minima. All the secondary minima appear at phase 0.5, and the durations are equal for the primary and the secondary eclipses. The epochs of primary minima follow the nearly sinusoidal O[C curve that has been observed for this star in previous studies. The values of O[C for the secondary minima were in the same range as those of the primary minima observed by us. We conclude that the system is in a circular orbit. Our observed epochs of primary minima support the presence of a third component in the system, as proposed by Radhakrishnan, Sarma, & Abhyankar. The e †ect of the presence of a third, noneclipsing, light source would be to suppress the observed depths of both the eclipses, whereas in this system we Ðnd that the secondary eclipse depth is being enhanced and the primary eclipse depth is being suppressed compared with expectations. So we have not Ðtted for a third light in our light-curve analysis, leaving the nature of the third body, if present, undetermined from our present light-curve analysis.The J-band light curve of R CMa Ðtted well with a bolometric albedo of the secondary star A 2 \ 0.5, as expected for a star with a convective atmosphere. But the K-band light curve showed a value of is also found to be higher in the broadband light curves than in the narrowband light A ...