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Published byBlake McGinnis Modified over 11 years ago
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Wavetrains and Coherency
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© 2006 Walter Fendt Beats Animation http://www.walter-fendt.de/ph11e/beats.htm
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y(x) = Sin x © SPK
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y(x) = [Sin x + Sin (1.08 x)]/2 © SPK
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y(x) = [Sin x + Sin(1.04 x) + Sin (1.08 x)]/3 © SPK 0 < x < 200
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y(x) = [Sin x + Sin(1.02 x) + Sin (1.04 x) + Sin(1.06 x) + Sin (1.08 x)]/5 © SPK 0 < x < 400
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y(x) = [Sin x + Sin(1.01 x) + Sin (1.02 x) + Sin(1.03 x) + Sin (1.04 x) + Sin (1.05 x) + Sin (1.06 x) + Sin (1.07 x) + Sin (1.08 x)]/9 © SPK 0 < x < 400
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y(x) = [Sin x + Sin(1.01 x) + Sin (1.02 x) + Sin(1.03 x) + Sin (1.04 x) + Sin (1.05 x) + Sin (1.06 x) + Sin (1.07 x) + Sin (1.08 x)]/9 © SPK
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Solitary pulse
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For -L +L E0E0
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Fourier integral
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k p =2
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Wave packet or Wave group for k p =k
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Frequency Bandwidth Range of frequency k (or ) in wavetrain ( k) (or
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Temporal coherence: Coherence time: Coherence length: © SPK
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Spectral lines from helium gas tube
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A characteristic Spectral line
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Spectral line broadening 1.Natural linewidth 2.Doppler broadening 3.Collision broadening 4.Pressure broadening
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Red Cadmium= 6438 Å = 10 10 Hz, 30 cm Yellow Sodium = 10 9 3 cm = 5893 Å He-Ne Laser 6328 Å 300 m = 10 6 Hz, © SPK
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Kr discharge lamp has roughly the following intensity distribution at various wavlengths, (in nm), Estimate the coherence length of the Kr source.
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Coherence time Coherence length
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