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<math>A^2 _{total} = 2 A^2 (1 + \cos ( d _2 - d _1 ) ) </math>
 
<math>A^2 _{total} = 2 A^2 (1 + \cos ( d _2 - d _1 ) ) </math>
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Because the wave reflecting off the back of the diamond travels through the diamond twice, the term <math> d _2 - d _1 </math> is twice the thickness of the diamond, in seconds. Because this measurement is in unhelpful units, we can multiply it by the speed of light in a diamond and divide by two for the thickness.
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Because the wave reflecting off the back of the diamond travels through the diamond twice, the term <math> d _2 - d _1 </math> is twice the thickness of the diamond, in seconds. Because this measurement is in unhelpful units, we can multiply it by the speed of light in a diamond and divide by two for the thickness <math> \tau </math>.
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<math> ( d _2 - d _1 ) V / 2 = \tau </math>
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We can calculate A by returning the mirror, removing the diamond, and measuring the amplitude from the mirror alone.
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== Calculating the Shape ==
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Of course, thickness is not the only thing we need. We will also detect a third laser, which reflects off the mirror. We can calculate that the amplitude of this new combined wave will be
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<math>A^2 _{total} = A^2 + A^2 _t + 2 A A _t \cos ( d _t ) </math>
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Because we have values for A and <math> A _t </math>,
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<math> ( d _2 - d _1 ) V / 2 = /tau </math>
       
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