To circumvent numerical instabil- ities, we write ln ( Z(q, l))) = ln PNb k=1 eq·ln[Pk(l)] and make use of ln X k exk ! = M + ln X k exk−M ! , (C2) with M = maxk(xk)

A partition function is calculated by summing the moments of these probabilities as Z(q, l) = NbX k=1 [Pk(l)]q, (C1) with −8 < q < 8

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Fibonacci Waveguide Quantum Electrodynamics

quant-ph · 2025-07-08 · unverdicted · novelty 7.0

Fibonacci-structured photonic waveguides enable atom-photon bound states and effective emitter Hamiltonians with Fibonacci or multifractal properties, providing a platform for coherent quantum interactions in aperiodic systems.

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Fibonacci Waveguide Quantum Electrodynamics quant-ph · 2025-07-08 · unverdicted · none · ref 5
Fibonacci-structured photonic waveguides enable atom-photon bound states and effective emitter Hamiltonians with Fibonacci or multifractal properties, providing a platform for coherent quantum interactions in aperiodic systems.

To circumvent numerical instabil- ities, we write ln ( Z(q, l))) = ln PNb k=1 eq·ln[Pk(l)] and make use of ln X k exk ! = M + ln X k exk−M ! , (C2) with M = maxk(xk)

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