The full width at half maximum of an atomic absorption line at 589 nm is 100 MHz. A beam of light passes through a gas with an atomic density of 10^17/m3 . Calculate: (1) The peak absorption coefficient due to this absorption line. You can assume that the index of refraction is close to 1 in for this dilute gas. (2) The frequency at which the resonant contribution to the refractive index is at a maximum. (3) The peak value of this resonant contribution to the index of refraction.
The full width at half maximum of an atomic absorption line at 589 nm is 100 MHz. A beam of light passes through a gas with an atomic density of 10^17/m3 . Calculate: (1) The peak absorption coefficient due to this absorption line. You can assume that the index of refraction is close to 1 in for this dilute gas. (2) The frequency at which the resonant contribution to the refractive index is at a maximum. (3) The peak value of this resonant contribution to the index of refraction.
Chemistry
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ISBN:9781305957404
Author:Steven S. Zumdahl, Susan A. Zumdahl, Donald J. DeCoste
Publisher:Steven S. Zumdahl, Susan A. Zumdahl, Donald J. DeCoste
Chapter1: Chemical Foundations
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Problem 1RQ: Define and explain the differences between the following terms. a. law and theory b. theory and...
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The full width at half maximum of an atomic absorption line at 589 nm is 100 MHz. A beam of light passes through a gas with an atomic density of 10^17/m3 . Calculate: (1) The peak absorption coefficient due to this absorption line. You can assume that the index of refraction is close to 1 in for this dilute gas. (2) The frequency at which the resonant contribution to the refractive index is at a maximum. (3) The peak value of this resonant contribution to the index of refraction.
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