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The distribution of Dn on the detonation wave in the stable mode was approximately formulated.
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Lateral resolution in the μ-ARPES measurement mode is approximately 5 μm, and for this reason some contribution from the HOPG substrate can be seen in the image.
In actual fact, it is found that flow measurement based on the fundamental mode is approximately free of errors while all other modes are characterized by the same (and, generally, non-vanishing) deviation of measurement.
For appropriate choice of system parameters, the natural frequency of the second mode is approximately three times that of the first mode for a range of mean flow velocity, activating a three-to-one internal resonance.
The obtained results indicate that the maximum load for the shear fracture mode is approximately three times larger than that for the tensile fracture mode and that the displacement in the shear fracture mode is also larger than that in the tensile fracture mode.
The test time required to evaluate an image with a pixel resolution of 1024 × 1024 pixel in GPU mode is approximately 0.04 s, which means the method based on a Faster R-CNN has the capacity of a quasi-real-time autonomous dispersion evaluation in GPU mode to replace a human-assisted microscopic dispersion evaluation in OP images.
The Cu-Mn distance in this mode is approximately in the range of 2.73 to 3.98 Å (Additional file 1: S1).
LEE for the TM mode is approximately ten times lower than that for the TE mode, which is attributed to the strong TIR effect for the TM mode.
As observed, the computational cost of the proposed system using the rhombus (2D) integration mode is approximately four times the computational cost needed when 1D modes are used.
The maximum power density at this condition in the fuel cell mode is about 0.84 W/cm2 and the minimum power density in the electrolyser mode is approximately − 1.18 W/cm2.
The computation time for uncompressed chorus burst mode is approximately 1.4 times that of the duration of a burst observation for electric and magnetic field waveforms (red and blue rectangles in Fig. 12a).
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