Changes

Light is a wave, and can be expressed as

Light is a wave, and can be expressed as

<math>\Psi = A _{laser} \sin ( \omega t + d ) </math>

<math>\Psi = A _{laser} \sin ( \omega t + d ) \,</math>

where <math> A _{laser} </math> is the amplitude of the initial laser beam, <math>\omega</math> is the frequency, t is time, d is the phase-shift, and C is a constant dependent on the reflectivity of all surfaces the laser intercepts.

where <math> A _{laser} </math> is the amplitude of the initial laser beam, <math>\omega</math> is the frequency, t is time, d is the phase-shift, and C is a constant dependent on the reflectivity of all surfaces the laser intercepts.

We have a sum of three waves, which can be expressed as

We have a sum of three waves, which can be expressed as

<math>\Psi _{Front Of Diamond} = \Psi _1 = C _1 A _{laser} \sin ( \omega t + d _1 ) </math>

<math>\Psi _{\mbox{Front Of Diamond}} = \Psi _1 = C _1 A _{laser} \sin ( \omega t + d _1 ) \,</math>

<math>\Psi _{Back Of Diamond} = \Psi _2 = C _2 A _{laser} \sin ( \omega t + d _2 ) </math>

<math>\Psi _{Back Of Diamond} = \Psi _2 = C _2 A _{laser} \sin ( \omega t + d _2 ) \,</math>

<math>\Psi _{Mirror} = \Psi _0 = C _0 A _{laser} \sin ( \omega t) </math>

<math>\Psi _{Mirror} = \Psi _0 = C _0 A _{laser} \sin ( \omega t) \,</math>

(For simplicity, we will say that the wave leaving the mirror has not been phase-shifted, as above.)

(For simplicity, we will say that the wave leaving the mirror has not been phase-shifted, as above.)