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Physical limits to broadening compensation in linear slow light systems

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Fig.  2.  Pulse  broadening  as  a  function  of  the  frequency  separation  between  the  two  loss  resonances
Fig.  3.  Transmission  of  a  “101”  sequence  in  the    slow  light  medium  described  above  for  the  cases  of  loss  resonances  separation  of  400  MHz  (grey  curve)  and  130  MHz  (red  curve)

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