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Figure 5 The absorption spectrum of signal laser as a function of the detuning between signal laser and exciton for four difference coupling of peptide QD-DNA.
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Figure 2 Scaled absorption spectrum of the signal current as a function of the detuning Δ s and energy level diagram of thecoupled system.
(a) Scaled absorption spectrum of the signal currentas a function of the detuning Δ s without landing anymasses on the NR.
(b) Energies of the first singlet and the first triplet excitation (normalized by the ground state energy), as a function of the detuning.
Figure 2a illustrates the absorption ofthe signal current as a function of the detuning Δ s (Δ s = ω s -ω q ).
In Figure 2(a), we plot the overlap of the ground state of 16 ions with the ground state manifold of the Majumdar-Ghosh model, and the Haldane-Shastry model as a function of the detuning.
(a) Overlap of the ground state of N = 16 ions with the ground state manifold of the Majumdar-Ghosh model, and the Haldane-Shastry model as a function of the detuning.
The phase quadrature (equation (7)) can been seen to consist of components that are quantum fluctuations (first two terms) and a component that is a function of the detuning parameter (last term).
The phase transition temperature of the NV-resonator hybrid system as a function of the scaled detuning (delta/omega_{r}).
Figure 3 The optical Kerr coefficient as a function of the probe detuning Δ pr for η =0.
Figure 2 plots the optical Kerr coefficient R e(χ(3)) as a function of the probe detuning Δpr.
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