2013
DOI: 10.1016/j.jastp.2012.11.017
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Radar interferometer calibration of the EISCAT Svalbard Radar and a additional receiver station

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Cited by 4 publications
(3 citation statements)
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“…At high latitudes, satellites transiting the radar beam provide strong backscattering targets which make it possible to estimate the receiver phase offsets and the antenna baselines. Here, we have used the method by Schlatter et al (2013) to self-consistently solve for the baseline geometry and the phase offsets have been derived accordingly from satellite backscatter.…”
Section: Methodsmentioning
confidence: 99%
“…At high latitudes, satellites transiting the radar beam provide strong backscattering targets which make it possible to estimate the receiver phase offsets and the antenna baselines. Here, we have used the method by Schlatter et al (2013) to self-consistently solve for the baseline geometry and the phase offsets have been derived accordingly from satellite backscatter.…”
Section: Methodsmentioning
confidence: 99%
“…The aperture synthesis imaging technique is already being used at the EISCAT Svalbard Radar, employing a small number of additional low-gain arrays distributed around the main radar site, an example of which is shown in Fig. 33 (see, for example, Schlatter et al 2013). The existence of a distributed receiving array, as planned for EISCAT_3D, with receiving elements located up to 2 km from the array centre, allows the reconstruction of ionospheric targets down to tens of metre scales, significantly smaller than the beam widths of the current generation of incoherent scatter radars (La Hoz and Belyey 2011).…”
Section: Observing Techniques and Measurement Philosophiesmentioning
confidence: 99%
“…A phase imbalance between receiving channels refers to as phase offset, or systematic phase error, or initial system phase bias. Much work has been performed to estimate the phase offset using different methods, e.g., generating a common signal that simultaneously fed each of two receivers and measuring the phase offset between them (Aso et al 1979;Vandepeer and Reid 1995;Valentic et al 1997), calculating the trajectory of an airplane flying routinely in the vicinity of the radar and comparing the observed phase differences of the radar echoes between difference receiving channels with the optical-recorded ones (Robertson et al 1953;Chen et al 2002), utilizing single or a set of artificial radio beacons placed at known locations in the far-field of the radar array and measuring the phase present at each channel (Glanz 1971;Valentic et al 1997;Chau et al 2008), receiving beacon signals transmitted by satellites and radio stars which transit across receiving arrays, then calculating their trajectories and comparing the phase differences of the beacon signals between difference channels with the theoretical ones (Glanz 1971;Clark 1978;Palmer et al 1996;Sullivan et al 2006;Chau et al 2008Chau et al , 2014Schlatter et al 2013), using meteor-head or -trail echoes collected during routine observations to do the self-survey phase calibration (Valentic et al 1997;Holdsworth et al 2004;Chau et al 2008), or comparing the distribution of sporadic E echoes with the expected echoing region which is determined in accordance with the International Geomagnetic Reference Field (IGRF) model (Wang 1999;Wang and Chu 2001;Kuong et al 2003).…”
Section: Introductionmentioning
confidence: 99%