Abstract
Some quantum information protocols require delay or storage of quantum light states so that the timing of the transaction can be controlled. One potential method for the delay and storage of quantum light states is to engineer a coherent interaction with an atomic level scheme, such as electromagnetically induced transparency [1] or addressing of coherent spin states of atomic ensembles [2]. Before such experiments can be attempted, one requires a source of quantum light states at a compatible atomic wavelength.
© 2007 IEEE
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