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The reported C piston-flow age is the age at the median probability (assuming that the age range is normally distributed about the radiocarbon age) of the distribution of the range of ages given in parentheses to the right of the piston-flow age (Table 1) (Stuiver and Reimer 1993).
(B,E) Distribution of the range residuals obtained with a 1-mm smoothing coefficient.
The results show that the derived analytical function can describe the probability density distribution of the range data obtained by laser radar with a constant threshold discriminator.
The symmetrical distribution of the range residuals around the 0 level (Figure 6A,D) gives a very low normal point RMS per pass: 0.06 mm for Ajisai and 0.09 mm for BLITS.
In the course of this process, fitting functions (orbital function or low degree polynomials) are used in order to remove the systematic trends from the distribution of the range residual data.
The probability density distribution of the range data is proportional to the probability density function of the noise and to the slope of the rising edge of the laser echo pulse.
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Figure 49 shows the distribution of the ranging arm temperature field without the water cooler under working conditions.
The probability density distributions of the range data obtained by laser radar with different pulse shapes, amplitudes, widths and thresholds are also presented.
The tuning scheme is obtained based on the distribution directives of the range sensors on the robot.
The distribution of the gasoline range hydrocarbons (C5 C10 non-aromatics and aromatics hydrocarbons) was also determined for the optimum conditions.
Finally, we show that the observed distribution of the covariance range has significantly longer tails than random, with clear geographic correspondences.
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