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A concept of a density meter is discussed.
The distribution function of the level cuts of a density function is also introduced.
The peak energy increases with density, reaching 2.0 ± 0.1 GeV for npe = 6.6 × 1014 cm−3 in the presence of a density gradient, at which point the charge capture is much lower.
density current: descent to an ocean layer of equal densityDiagram showing the behaviour of a density current as it descends to a layer of water whose density equals that of the current.
This model leads to the appearance of a density ratio in the propagation term of the G equation.
The paper shows how to optimize the analogue and discrete filters applied in an electronic circuit of a density meter.
The combined result can detect deviant nodes in a scalable manner and can operate in the presence of a density of deviant nodes approaching 22%.
The specified inverse problem is solved within a smoothing spline framework which preserves the characteristic properties of a density function, namely its normalization and non-negativity.
The models are designed to agree as closely as possible with experimental diffraction data while simultaneously attaining a local energy minimum of a density functional Hamiltonian.
Within the limited statistics, we did not observe a clear sign of a density shift, in accordance with a theoretical estimate by Korenman.
The third example shows low-shear dayside magnetopause crossing without any indications of a density decrease in front of the magnetopause.
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