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DTSTART:20261101T010000
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DESCRIPTION:Effective JC and anti-JC Interactions via Strong Driving   \n\nThe Jaynes-Cummings Model (JCM) approximates the Quantum Rabi Model (QRM) in some regimes and is exactly solvable by only keeping the rotating or `energy-conserving’ terms and dropping the counter-rotating or `non-energy conserving’ terms. Since the proposal of the JCM\, questions on the effect and presence of counter-rotating terms popped up. Using strong driving\, one can induce the effects of the counter-rotating terms on a comparable timescale to the rotating terms. In such a scenario\, one can create a Schrödinger cat state in a resonant manner without the need for any type of Kerr nonlinearity. In this talk\, we review the QRM and its descendant\, the JCM. Then\, we discuss the realization of a Schrödinger cat state\, its challenges in practice and how to solve them.      \n\n
X-ALT-DESC;FMTTYPE=text/html:<strong>Effective JC and anti-JC Interactions via Strong Driving   </strong><br><br>The Jaynes-Cummings Model (JCM) approximates the Quantum Rabi Model (QRM) in some regimes and is exactly solvable by only keeping the rotating or `energy-conserving’ terms and dropping the counter-rotating or `non-energy conserving’ terms. Since the proposal of the JCM, questions on the effect and presence of counter-rotating terms popped up. Using strong driving, one can induce the effects of the counter-rotating terms on a comparable timescale to the rotating terms. In such a scenario, one can create a Schrödinger cat state in a resonant manner without the need for any type of Kerr nonlinearity. In this talk, we review the QRM and its descendant, the JCM. Then, we discuss the realization of a Schrödinger cat state, its challenges in practice and how to solve them.      <br><br>
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SUMMARY:IQC Student Seminar featuring Mohammad Ayyash
DTSTART;TZID=America/New_York:20220914T120000
DTEND;TZID=America/New_York:20220914T130000
DTSTAMP:20260408T061307Z
TRANSP:OPAQUE
STATUS:CONFIRMED
SEQUENCE:0
LOCATION:QNC 1201
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