Electromagnetically Induced Transparency (Experimental)

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$Measurement of refractive index using a Michelson interferometer$

‣Intensity depends on the laser current and not the power. ‣Rabi frequency depends on the intensity and the coupling strength.
• The beams orthogonally polarized to each other. • That is how then they are separated out the detector. • Scattering can also cause polarization to change. • That is why we have also added another polarizer before the detector to block out the scattered light from the strong coupling beam.
Page 2 and 3: Golden Words The purpose of educati
Page 4 and 5: What is Transparency? • It is a r
Page 6 and 7: At the micro-scale, an electromagne
Page 8 and 9: 6 May 2011
Page 11: EIT Configurations Ladder V-type La
Page 14: 23 September 2011
Page 17 and 18: Lasers to be Used Considerations:-
Page 19 and 20: ‣ Spectral Width:- Spectral width
Page 21 and 22: Diagrams Spectral Width Full Width
Page 23 and 24: Distributed Feedback Diode Lasers
Page 25 and 26: The Diffraction Grating is outside
Page 27 and 28: Construction of ECDLs
Page 30 and 31: • Wavelength • Intensity • Po
Page 32 and 33: We need at least 20mW of power of t
Page 36 and 37: Beam Shape and Size • Diode laser
Page 40 and 41: ALL OPTICAL QUANTUM NANO SWITCHES (

Electromagnetically Induced Transparency (Experimental)

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