modeling

A DISCRETE-TIME MODEL FOR CODED DENSE WDM NETWORKS EMPLOYING FABRY-PEROT FILTERS
Tri T. Ha and John P. Powers
Department of Electrical and Computer Engineering
Code EC/HA
Naval Postgraduate School
Monterey, CA 93943 USA

Abstract
We present a novel discrete-time model to evaluate the capacity, power penalty/coding gain and bit error probability of dense WDM networks employing OOK modulation with direct detection and Fabry-Perot filters as channel selector. Reed-Solomon error correcting codes and concatenated Reed-Solomon/Reed-Solomon codes are employed to pack the optical channels. The discrete-time model utilizes the trapezoidal expression together with signal samples obtained at the Nyquist rate equal to twice the Fabry-Perot spectral range.


COMPARISON OF LOWER BOUNDS IN DIRECTION OF ARRIVAL ESTIMATION
Hung Nguyen
Mountain Technology Inc.
5243 Braywood Drive
Centreville, VA 22020
E-Mail: [email protected]

Abstract
The performance of nonlinear estimators exhibits an SNR threshold behavior above which the estimator mean square error performance is small and can be closely characterized by the Cramer-Rao lower bound. Below the threshold SNR, the MSE performance is large and can exceed the CRLB by a large factor, implying that the CRLB is an overly optimistic lower bound to use. Thus, improved lower bounds can be used to analyze the performance of direction of arrival (DOA) estimators below the threshold SNR and to determine where the threshold occurs.

For a single signal, a numerical comparison of the CRLB, the single parameter Chazan-Ziv-Zakai lower bound (CZZLB) and the Weiss-Weinstein lower bound (WWLB) on DOA estimation MSE shows that the CZZLB is the tightest lower bound. Thus, various DOA estimation algorithms can be simulated and their performance compared to the CZZLB to select the best algorithm. Furthermore, the CZZLB accurately predict the threshold SNR which is a critical system design parameter. The analysis is extended to two signals. Here, the multiple parameter WWLB is applicable but appears to be a weak lower bound. Below the threshold SNR, a maximum likelihood DOA estimation procedure such as the Expectation Maximization (EM) algorithm seeded by the Alternating Projection Maximization (APM) algorithm should be used to provide the best DOA estimation performance. Above the threshold SNR, the use of the statistically efficient MUSIC algorithm is adequate.



THE ANALYSIS OF VARIOUS DIFFUSION THEORY MODELS AND SOLUTION STRATEGIES FOR HEXAGONAL PRODUCTION REACTORS
Thuy Trong Le
SuperComputer Group
Fujitsu America Incorporation
San Jose, CA 95134-2022 USA
E-Mail: [email protected]

Abstract
This paper describes our research to improve the speed and accuracy of the computer system used for reactor operation and design at Savannah River Laboratory (SRL). Since the old code system was written at a time when computer processing speed and memory storage capacity were very limited (1970s), re-investigating this code system for both computing speed and accuracy of the solution methods is necessary. The speed performance of the system can be improved by implementing the new code system to take advantage of the hardware improvement (vectorization, parallelization, and higher memory capacities) as well as the range of available computer (from workstations to supercomputers). For the accuracy of the computational system, several studies were performed to locate the least accurate source from the multi-step solution procedure. It was found that the least accurate part is from the reactor calculation step which does not reproduce in case of infinite lattice the lattice physics results as accurately as desired. Three investigated techniques were performed to located and improve the source of least accuracy. These are the improvement of spatial resolution, the implementation of response matrix method, and the correction from flux discontinuity factors. Our research results show that flux discontinuity factors, the technique widely used for the analysis of light water reactor is also the solution for the production reactor.