Simple model for a heat engine. QH is input heat from a hot source to the engine, QC is the heat rejected to the colder environment (entropy sink) and W is the work output.

Simple model for a heat engine. QH is input heat from a hot source to the engine, QC is the heat rejected to the colder environment (entropy sink) and W is the work output.

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The advantages of quantum effects in several technologies, such as computation and communication, have already been well appreciated. Some devices, such as quantum computers and communication links, exhibiting superiority to their classical counterparts, have been demonstrated. The close relationship between information and energy motivates us to e...

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... Q H and Q C are the heat received and rejected in the engine operation and W is the work produced in the engine cycle, as illustrated in Figure 1. Simple model for a heat engine. ...
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... a strategy allows us to establish the efficiency of such information fueled engines compared to the Carnot bound. The basic idea is to consider the source and the sink in Figure 1 as information reservoirs and to use a quantum system as the engine's working substance. The work output of the cycle becomes then analog of a calculation or a computational process. ...
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... problem of thermalization of a composite system consisting of a target qubit (the system) that randomly and repeatedly interacts with a cluster of N identical spin-1/2 (qubit) particles is examined in Ref. [173,177]. The system is illustrated in Figure 10. The target qubit's evolution is found to be equivalent to the master equation of a coherently driven two-level atom in a squeezed thermal bath. ...
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... work output depends on the number of the atoms quadratically, due to the superradiance [184], where a cluster can radiate quadratically faster than a single atom. The model is illustrated in Figure 11. Superradiance (SR) is given as a cooperative emission of light from an ensemble of excited two-level atoms in a small volume relative to emission wavelength [184]. ...
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... is a critical size of the cluster for which quadratic enhancement in the work output can still be obtained even in the presence of a quadratic increase in the decoherence factor. We can represent coherences between N atomic energy levels as a complete graph as in Figure 12, which can Figure 11. A cavity field pumped by a beam of N -atom clusters in atomic coherent or Dicke states reaches a steady state, a coherent thermal state. ...
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... is a critical size of the cluster for which quadratic enhancement in the work output can still be obtained even in the presence of a quadratic increase in the decoherence factor. We can represent coherences between N atomic energy levels as a complete graph as in Figure 12, which can Figure 11. A cavity field pumped by a beam of N -atom clusters in atomic coherent or Dicke states reaches a steady state, a coherent thermal state. ...
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... to the result of Ref. [179], there is a critical size of such a quantum fuel molecule, after which further increase of the size would give negative yields, rapidly decreasing the efficiency and work output. Figure 12. Representation of coherences between N atomic energy levels in a multilevel atom or an atomic cluster as a complete graph. ...
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... can be compared to the microeconomical law of diminishing returns [194], plotted in Figure 13. ...
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... finite size systems with a varying number of particles are further examined in [174] from the perspective of their generation using thermal and nonthermal means. The system subject to thermal charging of coherences is illustrated in Figure 14a. A pair of two-level atoms is initially prepared in a state with an amount of heat exchange coherence C L . ...
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... role of dipolar interactions between the particles is shown to be not critical in thermal induction of coherence. The discharge of stored coherences Figure 13. Microeconomical law of diminishing returns. ...
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... heat is shown in Figure 14b, where a single two-level atom collides sequentially with a pair of atoms with coherence C H . Some amount of the energy cost to generate coherences in the initial state can be harvested back as heat. ...
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... the single-atom reaches a steady state that is a thermal state with an effective temperature of T eff . This temperature depends on the coherence C H of the subenvironment atomic pairs as illustrated in Figure 14c. [174])A pair of two-level atoms initially in a state with (lower) coherence CL can be transformed into another state with higher coherence CH > CL by collective interaction with a thermal bath. ...
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... N -element spin-star network, illustrated in Figure 15, has been proposed as a quantum fuel to power up a photonic Carnot engine [177]. Previously, it has been shown that using individual qubit in a pair yields different work output than using the pair as whole as quantum fuel [195]. ...
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... single-particle quantum thermalizing devices could be realized using superconducting circuit QED schemes [196]. Figure 15. A spin star system that consists of a central spin coupled to N surrounding spins. ...

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