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Dynamics of Open Quantum Systems II, Markovian Approximation

Marco Merkli

2022Quantum28 citationsDOIOpen Access PDF

Abstract

A finite-dimensional quantum system is coupled to a bath of oscillators in thermal equilibrium at temperature<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>T</mml:mi><mml:mo>&amp;#x003E;</mml:mo><mml:mn>0</mml:mn></mml:math>. We show that for fixed, small values of the coupling constant<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>&amp;#x03BB;</mml:mi></mml:math>, the true reduced dynamics of the system is approximated by the completely positive, trace preserving Markovian semigroup generated by the Davies-Lindblad generator. The difference between the true and the Markovian dynamics is<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>O</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mrow class="MJX-TeXAtom-ORD"><mml:mo stretchy="false">|</mml:mo></mml:mrow><mml:mi>&amp;#x03BB;</mml:mi><mml:msup><mml:mrow class="MJX-TeXAtom-ORD"><mml:mo stretchy="false">|</mml:mo></mml:mrow><mml:mrow class="MJX-TeXAtom-ORD"><mml:mn>1</mml:mn><mml:mrow class="MJX-TeXAtom-ORD"><mml:mo>/</mml:mo></mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msup><mml:mo stretchy="false">)</mml:mo></mml:math>for all times, meaning that the solution of the Gorini-Kossakowski-Sudarshan-Lindblad master equation is approximating the true dynamics to accuracy<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>O</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mrow class="MJX-TeXAtom-ORD"><mml:mo stretchy="false">|</mml:mo></mml:mrow><mml:mi>&amp;#x03BB;</mml:mi><mml:msup><mml:mrow class="MJX-TeXAtom-ORD"><mml:mo stretchy="false">|</mml:mo></mml:mrow><mml:mrow class="MJX-TeXAtom-ORD"><mml:mn>1</mml:mn><mml:mrow class="MJX-TeXAtom-ORD"><mml:mo>/</mml:mo></mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msup><mml:mo stretchy="false">)</mml:mo></mml:math>for all times. Our method is based on a recently obtained expansion of the full system-bath propagator. It applies to reservoirs with correlation functions decaying in time as<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mn>1</mml:mn><mml:mrow class="MJX-TeXAtom-ORD"><mml:mo>/</mml:mo></mml:mrow><mml:msup><mml:mi>t</mml:mi><mml:mrow class="MJX-TeXAtom-ORD"><mml:mn>4</mml:mn></mml:mrow></mml:msup></mml:math>or faster, which is a significant improvement relative to the previously required exponential decay.

Topics & Concepts

SemigroupPropagatorMaster equationLindblad equationLambdaMarkov processQuantumThermal reservoirExponential decayGenerator (circuit theory)Exponential functionQuantum master equationMathematicsTrace distanceStatistical physicsCoupling (piping)PhysicsMathematical physicsQuantum mechanicsMathematical analysisQuantum stateHeat spreaderMechanical engineeringEngineeringPower (physics)Heat transferStatisticsAdvanced Thermodynamics and Statistical MechanicsQuantum Information and CryptographyQuantum Mechanics and Applications
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