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Design modifications will enable this device to be used as an implantable defibrillator with an external RF power source.
A multi-harmonic asymmetric cavity is predicted to obtain lower RF breakdown probability than a conventional pillbox cavity, when driven by two or more external RF harmonic sources.
After exposure to an external RF field, nonaggregated AuNPs absorbed and dissipated energy as heat, causing thermal damage to the targeted cancer cells.
The complete measurement set-up contains LNA with BIST circuit, external RF source, RF relays, 50 Ω load impedance, and a DC voltmeter.
We consider two models: an electrostatic (ES) model using an external rf voltage and an electromagnetic (EM) model using an external rf current.
We considered two different electrode configurations: an electrostatic (ES) model using an external rf voltage and an electromagnetic (EM) model using an external rf current.
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Sensitivity and resolution in NMR experiments are affected by magnetic field inhomogeneities (of both external and RF), errors in pulse calibration, and offset effects due to finite length of RF pulses.
The gate-width can be set to a preset value ranging from 200ps to 1000ps, (COMB modes) or can be controlled through external signals (RF or logical triggering).
The SMA-coil actuator itself forms a passive resonant circuit that functions as a wireless heat source activated using external radio-frequency (RF) electromagnetic fields for frequency-selective control of the actuation.
We investigated the external radio frequency (rf) electromagnetic field penetration into the magnetized collisionless plasma using one-dimensional particle-in-cell (PIC) code, which simulates the plasma and electromagnetic field evolution in a direction perpendicular to the background magnetic field.
Table 1 Four runs are performed, where the system lengths, L=2a, are 1000Δ and 767Δ for run1 and runs 2 4, respectively Method ω rf External field amplitude Run 1 ES 10 ω LH V rf /c B 0 L=1 Run 2 ES 0.5 ω LH V rf /c B 0 L=0.008 Run 3 EM 0.5 ω LH μ 0 j rf Δ/B 0=0.02 Run 4 EM 0.5 ω LH μ 0 j rf Δ/B 0=0.2.
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