The reference parameters P k,l are estimated first at the coder from isolated source signals.
This approach assumes that the reference parameters are exactly known at the coder step before the alteration of the signal.
The network throughput, energy consumption and success rate of transmission data were used as the reference parameters in the simulation analysis.
According to the desired target quality, the reference parameters are quantized and partials are constructed in order to compute the time-frequency mask of each source.
b The estimated time-dependent parameters of the non-stationary ETAS model, where the reference parameters are the MLE of the ETAS model.
The algorithm is derived by considering an extended dynamic system where the reference parameters and the transmitted symbols are system-state random processes.
This issue is solved using long-term sinusoidal modeling[31] of the reference parameters at the coder which allows to code the entire mask with a negligible bitrate, thanks to the informed estimation of sinusoidal parameters.
In the δf code using the reference parameters of the SSC (Superconducting Super Collider), beam blow-up near resonances and oscillations in the tune shift, Δv, far from resonances are observed.
The reference parameters adopted for the central element followed the proposed values by Zarnic and Gostic (1997c) and later modified by Dolsek and Fajfar (2008) which are based on recommendations from past researchers, experimental tests and are in accordance with the FEMA 356 (2000) recommendations, and the hysteretic curve of the central element is illustrated in Fig. 8a.
The stress path parameters describe the evolution of the Mohr circle and are defined by three terms, the stress arching parameter γ 3, the horizontal stress path parameter γ 1 and the deviatoric stress path parameter or stress anisotropy parameter K. Since only two of the three parameters are independent we choose γ 3 and K as the reference parameters (e.g., Segura et al. 2011).
Three samples with the CL layer grown at 2 ML s−1 were studied: the first one with the reference parameters for N and Sb sources (sample F1), the second one by raising the Sb effusion cell temperature to 345°C (sample F2), and the last one by increasing both the Sb cell temperature to 345°C and the RF plasma source power to 210 W (sample F3).
