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This is the origin for Doppler-free EIT line shapes in thermal atoms, see, for example,.
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Typically mm =10 for η=0.1, increasing to mm =25 for η=0.5.
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For rubidium the dc polarizabilities of ground and excited states differ by about a factor of 2.7.
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For rubidium the dc polarizabilities of ground and excited states differ by about a factor of 2.7.
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