Electromagnetically induced transparency

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$Measurement of refractive index using a Michelson interferometer$

Rubidium 85 First excited state:Possible states Second excited state:possible states
Rubidium 85 Hyper fine splitting: This is interaction of nuclearspin (I) with the electron angular momentum (J). HF splitting of ground state is, HF splitting of the 1 st and 2 nd excited states is,
Page 1 and 2: ELECTROMAGNETICALLYINDUCED TRANSPAR
Page 3 and 4: Stimulated absorption Stimulated Ab
Page 5: Stimulated emission Stimulated emis
Page 10 and 11: Energy level diagram of 85 Rb
Page 12 and 13: Ladder type system The initial stat
Page 14 and 15: Hamiltonian Perturbed part: When an
Page 16 and 17: Time evolution of the density matri
Page 26 and 27: Complex susceptibility Doppler broa
Page 28 and 29: Complex susceptibility Ignoring two
Page 30 and 31: Complex susceptibility Including tw
Page 32 and 33: Complex susceptibilitythe constants
Page 34 and 35: Results
Page 36: Applications of EIT Fundamental and

Electromagnetically induced transparency

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