We have analyzed the notions of group velocity V-g and energy velocity V-E for light pulses propagating inside one-dimensional photonic band gap structures of finite length. We find that the two velocities are related through the transmission coefficient t as V-E = \t\V-2(g). It follows that V-E = V-g only when the transmittance is unity (\t\(2) = 1). This is due to the effective dispersive properties of finite layered structures, and it allows us to better understand a wide range of phenomena, such as superluminal pulse propagation. In fact, placing the requirement that the energy velocity should remain subluminal leads directly to the condition V-g less than or equal to c/\t\(2). This condition places a large upper limit on the allowed group velocity of the tunneling pulse at frequencies of vanishingly small transmission.
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