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In the other approaches the sampling offset can be taken into account at the receiver.
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If the tip approaches the sample, then an electrostatic force forms between the metal tip and the surface of the sample.
Buoyancy is observed to affect this mode of smolder at very low air velocities, or when the smolder front approaches the sample end.
For each tip-sample interaction circle, the AFM tip firstly approaches the sample surface at a discrete distance above the sample, and there is no interaction between the tip and the sample surface (Fig. 1a).
First, as with many qualitative approaches, the sample size was small.
In parallel approaches, the sample is usually illuminated with a single high NA beam, and angle is encoded in a specific domain.
In the Markov-based approach, the sampling resolution is chosen adaptively depending on the fitness of the last sample(s).
To facilitate the development of the LP approach, the sampling interval is properly chosen such that the discrete-time frequency is ω=π/2.
On the other hand, simulations at mixed/exchanged resolutions by parallel multi-scale approaches enrich the sampling of conformational space.
Thus, using this snowballing approach, the sample size continuously expanded, as compared with other sampling techniques.
Following this approach, the sample size increased like a rolling snowball.
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