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<!DOCTYPE article SYSTEM "http://www.adv-radio-sci.net/inc/ars/copernicus.dtd">
<article language="en">
	<journal>
		<journal_title>Advances in Radio Science</journal_title>
		<journal_url>www.adv-radio-sci.net</journal_url>
		<issn>1684-9965</issn>
		<eissn>1684-9973</eissn>
		<volume_number>2</volume_number>
		<volume_title>Kleinheubacher Berichte 2003</volume_title>
		<publication_year>2004</publication_year>
	</journal>
	<doi>10.5194/ars-2-19-2004</doi>
	<article_url>http://www.adv-radio-sci.net/2/19/2004/</article_url>
	<abstract_html>http://www.adv-radio-sci.net/2/19/2004/ars-2-19-2004.html</abstract_html>
	<fulltext_pdf>http://www.adv-radio-sci.net/2/19/2004/ars-2-19-2004.pdf</fulltext_pdf>
	<start_page>19</start_page>
	<end_page>25</end_page>
	<publication_date>2005-05-27</publication_date>
	<article_title content_type="html">Calibration methods for microwave free space measurements</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>I. Rolfes</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>B. Schiek</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Institut für Hochfrequenztechnik, Ruhr-Universität Bochum, Universitätsstraße 150, 44801 Bochum, Germany</affiliation>
	</affiliations>
	<abstract content_type="html">In this article calibration methods for the precise,
contact-less measurement of the permittivity, permeability or
humidity of materials are presented. The free space measurement
system principally consists of a pair of focusing
horn-lens antennas connected to the ports of a vector network
analyzer. Based on the measured scattering parameters, the
dielectric material parameters are calculable. Due to systematic
errors as e.g. transmission losses of the cables or mismatches
of the antennas, a calibration of the measurement
setup is necessary. For this purpose calibration methods with
calibration standards of equal mechanical lengths are presented.
They have the advantage, that the measurement setup
can be kept in a fixed position, for example no displacement
of the antennas is needed. The presented self-calibration
methods have in common that the calibration structures consist
of a so-called obstacle network which can be partly unknown.
The obstacle can either be realized as a transmissive
or a reflective network depending on the chosen method. An
increase of the frequency bandwidth is achievable with the
reflective realization. The theory of the calibration methods
and some experimental results will be presented.</abstract>
	<references>
	</references>
</article>

