@InProceedings{GrecoRoYaScBaSi:2020:1DSiMi,
author = "Greco, Ana Fl{\'a}via Guedes and Rossi, Jos{\'e} Osvaldo and
Yamasaki, Fernanda Sayuri and Schamiloglu, Edl and Barroso,
Joaquim Jos{\'e} and Silva Neto, Lauro Paulo da",
affiliation = "{Instituto Nacional de Pesquisas Espaciais (INPE)} and {Instituto
Nacional de Pesquisas Espaciais (INPE)} and {Instituto Nacional de
Pesquisas Espaciais (INPE)} and {University of New Mexico} and
{Instituto Tecnol{\'o}gico de Aeron{\'a}utica (ITA)} and
{Universidade Federal de S{\~a}o Paulo (UNIFESP)}",
title = "1D-FDTD simulation of microwave generation using ferrite
electromagnetic shock lines",
booktitle = "Proceedings...",
year = "2020",
organization = "IEEE Electrical Insulation Conference",
publisher = "IEEE",
keywords = "gyromagnetic nonlinear transmission lines, RF generation,
numerical simulation.",
abstract = "Ferrite-charged nonlinear transmission lines (NLTLs) have been
used as electromagnetic shock lines in applications that require
pulses with extremely fast rise times. Subject to an intense
external magnetic field (20-40 kA/m), these lines can generate
microwave radiation generally in L-band (1-2 GHz) and are known in
this case as nonlinear gyromagnetic lines. Due to its wide
applicability in the RF area, such as electronic warfare (in
defense) or high power beam modulators (in industry), there is
growing interest in the study of these lines, especially using
finite difference time domain (FDTD) simulations to predict some
important line parameters, such as the rise time of the output
pulse and the frequency generated. The FDTD method is based on the
nonlinear behavior of the magnetic material that fills the line as
the current pulse propagates, inducing RF oscillations due to the
precession of the ferrite's magnetic moments, described
mathematically by the Landau-Lifshitz-Gilbert equation (LLG).
Thus, this work presents a one-dimensional numerical modeling and
simulation (1D) study to describe the behavior of these lines,
which operate in the TEM mode. The numerical simulations were
obtained using the joint solution of the transmission line
equations and the gyromagnetic LLG equation in the publicly
available software OCTAVE.",
conference-location = "Knoxville, United States",
conference-year = "22 june - 03 july",
doi = "10.1109/EIC47619.2020.9158728",
url = "http://dx.doi.org/10.1109/EIC47619.2020.9158728",
isbn = "978-172815485-5",
language = "en",
targetfile = "greco-1d.pdf",
urlaccessdate = "01 jun. 2024"
}