| 1. | Figure 3 shows the propagation of light through a polarization independent isolator.
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| 2. | For example, the propagation of light through a spectra that appear as rainbows.
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| 3. | This led to considerable theoretical work to explain the propagation of light without an aether.
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| 4. | Here the bulk plasmon resonance is induced or suppressed to manipulate the propagation of light.
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| 5. | The Huygens Fresnel principle provides a good basis for understanding and predicting the wave propagation of light.
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| 6. | In this case the propagation of light cannot simply be described by refractive indices except for polarizations along principal axes.
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| 7. | They can maintain the propagation of light in exclusively the clockwise or counterclockwise direction as long as they remain powered.
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| 8. | The propagation of light can be considered in terms of rays and wavefronts in ordinary physical three-dimensional space.
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| 9. | In order to find such a function, we turn to the wave equation, which governs the propagation of light.
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| 10. | Like Poincar? Cohn defined local time as the time, which is based on the assumption of isotropic propagation of light.
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