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The chosen design criteria were transformation of Iz→Ix over resonance offsets of ±20 kHz and RF variability of ±5%, with a pulse length of 2 ms.
Design criteria are unchanged: transformation of Iz → Ix over resonance offsets of ±20 kHz and RF variability of ±5%, with a peak RF amplitude equal to 17.5 kHz.
Design criteria were transformation of Iz→Ix over resonance offsets of ±20 kHz and RF variability of ±5%, with a pulse length of 500 μs and peak RF amplitude equal to 17.5 kHz.
Design criteria were transformation of Iz → Ix over resonance offsets of ±25 kHz for constant RF amplitude anywhere in the range 10 20 kHz, with a pulse length of 1 ms.
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Furthermore, the laser is represented by a delta-peak and locked to the cross-over resonance of the sodium D2-line.
For optimal optical rejection the laser is locked to the cross-over resonance, midway between the two (F=1) and (F=2) ground states of the D2-line (see Figure 1(d)).
Percussive melodic instruments include the bonang, the xylophone (gambang kayu), and various metallophones (instruments with a series of tuned metal plates, either suspended over a resonance trough or on resonance tubes).
In addition, we demonstrate that the ASSQ and PBDB-T show efficient exciton dissociation in the ternary blend over Förster resonance energy transfer (FRET).
Nearly ideal refocusing is possible over a resonance offset range of ± 170% relative to the nominal pulse B1 field, concurrent with tolerance to B1 inhomogeneity/miscalibration of ± 33%.
By comparing 22 to 10, it is possible to derive an expression for the average magnetic force experienced by the nanoresonator over the resonance relaxation time, which is given by F ̄ = μ 2 4 π ε 0 32 Φ c 3. (23..
The results reveal that an anti-symmetric nonlinear viscous damping can significantly reduce the transmissibility over all resonance regions for MDOF structures while it has almost no effect on the transmissibility over non-resonant and isolation regions.
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