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If, however, they are not undermined, the two are alike insofar as the accomplishment of the two accumulations and the attainment of the two awakened bodies (kāyas), and so forth, are concerned.
The Raman spectra were acquired using a confocal microprobe Raman system (in Via-Reflex, Renishaw, UK) with an excitation laser wavelength of 532 nm, power of 2 mW, and the acquisition time was 10 s with two accumulations.
Since this relation continues as a means to avoid falling into extremes, and also to accomplish the two accumulations and attain the two awakened bodies (kāyas), it is imperative, says Jamyang Shepai Dorje, that the two truths be understood as mutually interrelated.
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The accumulation moments are computed in parallel according to two accumulation grids.
In this section, several techniques are used as examples to validate the performance of the new method such as the including FFT, EEMD-based one accumulation (OA) method, EEMD-based two accumulation (TA) method, EEMD-based four accumulation (FA) method, and EEMD-based six accumulation (SA) method.
If we consider two accumulation grids, the first computes the accumulation moments on the odd lines of the image and the second on the even lines.
The measurements were spanned with 150 to 1,500/cm of four accumulations, and the exposure time was 30 s.
Integration times of 30 s were employed and three accumulations were averaged for each spectrum to obtain an adequate signal-to-noise ratio.
Each data point was an average of three accumulations.
Each spectrum represents an average of ten accumulations.
Three accumulations, each with an exposure time of 10 seconds, were collected using a laser power of about 1 mW.
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