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![Figure 2.Single-orbit ATI PADs computed without prefactors for hydrogencalculated for the field parameters ((a) and (b)], ((p(density plots have been represented in a linear scale and normalized to the highestand the numbers on the top left corners give the](https://thumb-ap.123doks.com/thumbv2/123dok/2962259.1356425/13.612.100.470.95.372/figure-computed-prefactors-hydrogencalculated-parameters-represented-normalized-highestand.webp)
![Figure 7. Fan-shaped holographic structures computed for Hydrogen using orbits1 and 2 and symmetrizing upon p∥ = 0 so that Re[t1−t2] is smaller than or at mostequal to half a field cycle](https://thumb-ap.123doks.com/thumbv2/123dok/2962259.1356425/21.612.99.467.93.243/figure-holographic-structures-computed-hydrogen-symmetrizing-smaller-mostequal.webp)
![Figure 10. Spider-like structures computed for Hydrogen in a field of intensitythe continuum propagation [panel (e); indicated by SFA] and the SFA-like partfor which the potential and momentum integrals in the have been neglected inof the action without res](https://thumb-ap.123doks.com/thumbv2/123dok/2962259.1356425/24.612.99.469.95.228/structures-hydrogen-intensitythe-continuum-propagation-indicated-integrals-neglected.webp)
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For low voltage distribution grids, where the impedance has often very low values, we suggest to perform network sensing by measuring the network impedance with either the PLM-ABB
In this section, we show the results of the measurement of the time evolution of the EGAM frequency. 5, we have shown that a quadratic scaling of the saturated electric field on
Real world e ffi ciencies (and also those in the simulation described later) will deviate from these calculated ones for several reasons: The performance when using a real
Usually for this equation the angle θ is defined as average around 24.5°. Direction cosine toward z axis is given from condition of continuously reflection of the sunlight off the
Comparisons of results of molecular dynamic simulations with the results of calculations based on the macroscopic diffusion model and experimental data allow to conclude that
The proposed device can operate as either a fine tuning element or an optical router and paves the way toward increased control of on-chip single photon devices using
Our estimates for the order of magnitude of the involved time scales indicate that socio-political instabilities may develop once the aggregate time scale for the evolution of
The hit function distribution, H ( z ), can be defined to be gauge invariant, although since the potential enters the path integral as a phase it now becomes complex val- ued.. We
