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	<title>The PT Symmeter &#187; X.-Y. Lü</title>
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		<title>PT-Symmetric Optomechanically-Induced Transparency</title>
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		<pubDate>Wed, 26 Nov 2014 07:55:53 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Henan Normal University]]></category>
		<category><![CDATA[Huazhong University of Science and Technology]]></category>
		<category><![CDATA[RIKEN]]></category>
		<category><![CDATA[Tsinghua University]]></category>
		<category><![CDATA[University of Michigan]]></category>
		<category><![CDATA[Washington University in St Louis]]></category>
		<category><![CDATA[B. Peng]]></category>
		<category><![CDATA[F. Nori]]></category>
		<category><![CDATA[H. Jing]]></category>
		<category><![CDATA[J. Zhang]]></category>
		<category><![CDATA[L. Yang]]></category>
		<category><![CDATA[S. K. Ozdemir]]></category>
		<category><![CDATA[X.-Y. Lü]]></category>
		<category><![CDATA[Z. Geng]]></category>

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		<description><![CDATA[H. Jing, Z. Geng, S. K. Özdemir, J. Zhang, X.-Y. Lü, B. Peng, L. Yang, F. Nori Optomechanically-induced transparency (OMIT) and the associated slow-light propagation provide the basis for storing photons in nanofabricated phononic devices. Here we study OMIT in parity-time (PT)-symmetric microresonators with a tunable gain-to-loss ratio. This system features a reversed, non-amplifying transparency:&#8230;]]></description>
			<content:encoded><![CDATA[<p><span style="background-color: transparent;">H. Jing, Z. Geng, S. K. Özdemir, J. Zhang, X.-Y. Lü, B. Peng, L. Yang, F. Nori</span></p>
<p><span style="background-color: transparent;">Optomechanically-induced transparency (OMIT) and the associated slow-light propagation provide the basis for storing photons in nanofabricated phononic devices. Here we study OMIT in parity-time (PT)-symmetric microresonators with a tunable gain-to-loss ratio. This system features a reversed, non-amplifying transparency: inverted-OMIT. When the gain-to-loss ratio is steered, the system exhibits a transition from the PT-symmetric phase to the broken-PT-symmetric phase. We show that by tuning the pump power at fixed gain-to-loss ratio or the gain-to-loss ratio at fixed pump power, one can switch from slow to fast light and vice versa. Moreover, the presence of PT-phase transition results in the reversal of the pump and gain dependence of transmission rates. These features provide new tools for controlling light propagation using optomechanical devices.</span></p>
<p><span style="background-color: transparent;"><a href="http://arxiv.org/abs/1411.7115" target="_blank">http://arxiv.org/abs/1411.7115</a><br />
Quantum Physics (quant-ph); Optics (physics.optics)</span></p>
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