By solving Maxwell's equations, we observed photon localization and strong electromagnetic field enhancement in laser-irradiated, one-dimensional random multilayer and twodimensional random media, with particle size around the laser wavelength. Higher refractive index contrast and degree of randomness result in stronger localization. The probability density and the location of enhanced fields are investigated as functions of refractive index and particle size distribution. For weakly dissipative media, local absorption enhancement is observed, and the expectation intensity distribution is obtained by averaging among many realizations. For comparison, the equation of radiative transfer (ERT) is also solved for random porous media, using the two-flux model. Since no interference effects are allowed, the classical diffusion, rather than localization, is predicted. Consequently, ERT can represent a good statistical average of the intensities only as absorption is dominant over localization. As expected, the particle treatment of ERT does not allow for predicting photon localization and field enhancement.Radiative transport in random porous media has long been an important problem in science and engineering [1][2][3]. As a laser beam is irradiated on a nonabsorbing random porous medium in which the particle size is much larger than the laser wavelength, the transmissivity reveals a diffusive behavior; i.e., decays inversely with the medium thickness [4]. Recently, however, it has been found that as the particle size decreases to the order of the laser wavelength, the diffusion breaks down and the transmission coefficient decays exponentially with the medium thickness, due to the constructive interference among the multiply scattered waves [5,6]. This phenomenon, termed "photon localization," is the counterpart of electron localization suggested by Anderson [7] and has been investigated theoretically and experimentally in one- [8-13], two-[14-20], and three-[21-24] dimensional structures. With the onset of localization, the electromagnetic (EM) waves may not propagate through, but are confined in a finite spatial region, forming a "random resonator." This property has initiated intense research interest in random lasers