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(a) The numerically simulated population of |1 after the triangular flux pulse is plotted as a function of the width and amplitude of the triangular flux bias.
In Fig. 3c, we plot the energy of the resonance peak E as a function of the width W for two different grooves.
In particular, reconstructed signal as a function of the width of the detector ring, its angular coverage and energy resolution were studied.
In Particular, we have found that the transmission, conductance and magnetoresistance oscillate as a function of the width of barriers.
(a) The population of |1 measured immediately (a few ns) after the triangular flux pulse is plotted as a function of the width and amplitude of the triangular flux bias waveform.
As in the simulations of the groove, we position the electron probe in the centre of the MIM waveguide and calculate the resonance energy of the MIM aGSP mode as a function of the width of the insulating layer.
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In Fig. 4d, the black line displays the calculated resonance energy as a function of the groove width.
Uncertainty was also investigated as a function of the plume width relative to well spacing.
The maximum of value downdraft was also parameterized as a function of the building width to building height ratio.
In order to better understand the origin of the 'hot spots', we also plot the probabilities of LZ transition as a function of the pulse width at fixed amplitude ΦLZS=10mΦ0 (Fig. 3c).
d Chirality parameter at zero ellipticity |κ η=0| as a function of the gap width.
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