Figure 1. Phase and group velocities in positive and negative index materials. a) A positive index material produces v ph = ω/k and v g = dω/dk in the same direction (both positive in this case). b) In contrast, a negative index material produces v ph and v g in opposite directions (negative v ph and positive v g in this case). c) Dispersion relation of positive-index materials showing that for positive v g (positive slope), v ph is also positive (k > 0, ω > 0). d) Dispersion relation for a negative-index material,showing that for a positive v g , a negative v ph (k < 0, ω > 0) is required. e) For positive-index, as the frequency increases, v g and v ph converge to zero. f) For negative-index, as the frequency increases, v ph < 0 diverges away from zero, while v g > 0 increases initially followed by a sharp drop toward zero close to the bandgap edge at ω 2 .