Sentence examples for projection of the coefficient from inspiring English sources

Exact(1)

Bottom: normalized projection of the coefficient vectors (tilde {z}_{n}^{m}) on the first four eigen modes ({mathcal {Z}}_{1}) to ({mathcal {Z}}_{4}), which represent 70.6% (top left), 9.4% (top right), 5.2% (bottom left), and 4.5% (bottom right) of the (tilde {z}_{n}^{m}) variances.

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This is achieved by estimating the completely bounded norm of the projections on the coefficients of irreducible representations of their compact duals.

Figure 10 Projection of the coefficients z( t ) on the first eigen modes, and comparison with the K p index.

The angles of arrival in elevation and azimuth are obtained as the maximizers of the sum of the magnitude squares of the projection of the signal coefficients on the column space of the array manifold.

As the projection of the multivariate coefficients is performed through the use of the spatial filters and the leadfield matrices, it is important to mention how the inverse solution affects the projection.

We show that the PDC reconstructed from the source projection of the MAR model coefficients, is very similar to the PDC, extracted from the simulated source signals directly.

We first demonstrate the theoretical feasibility of estimating source level causal interactions after projection of the sensor-level model coefficients onto the locations of the neural sources.

For the high and low energy X-ray spectra S H (E) and S L (E), the measured projections g H and g L are [ 4] (2) g H ln ⁡ I H I 0 = ln ⁡ ∫ 0 E m H S H E exp ⁡ − B 1 μ 1 E − B 2 μ 2 E d E, g L ln ⁡ I L I 0 = ln ⁡ ∫ 0 E m L S L E exp ⁡ − B 1 μ 1 E − B 2 μ 2 E d E, where B i is the projection of basis material coefficient b i and is represented by (3) B i = ∫ l b i x, y d l, i = 1,2.

The image of the particles on the camera corresponds to the projection of the field section, with a sin coefficient.

Finally, we present the main conclusions of this article in Section 5. First, as we mentioned, the sparsity is a property which can be described either directly for the signal itself or after some transformation, for example on the derivative of the signal, or in more general on the coefficients of the projection of the signal on any basis or any set of functions.

2 essentially summarizes the role played by the zonal coefficient of degree 3. We present in Figure 10 the projection of the (tilde {z}_{n}^{m}) coefficients onto the first four eigen modes.

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