2018
DOI: 10.1109/tap.2018.2854285
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Cold-Source Noise Measurement of a Differential Input Single-Ended Output Low-Noise Amplifier Connected to a Low-Frequency Radio Astronomy Antenna

Abstract: We present two methods for measuring the noise temperature of a differential input single-ended output (DISO) Low-Noise Amplifier (LNA) connected to an antenna. The first method is direct measurement of the DISO LNA and antenna in an anechoic chamber at ambient temperature. The second is a simple and low-cost noise parameter extraction of the DISO device using a coaxial long cable. The reconstruction of the DISO noise parameter from the noise wave measurements of the DISO LNA with one terminated input port is … Show more

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Cited by 14 publications
(17 citation statements)
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“…We then apply the various T rcv formulations presented in Sect. II using the measured noise parameters and S-parameters of the LNA previously measured in [9]. note that all three different methods presented converges for various pointing direction and array configurations (uniform and pseudo-random configuration) which indicated agreement in current literature of computing receiver noise temperature.…”
Section: Resultssupporting
confidence: 70%
See 1 more Smart Citation
“…We then apply the various T rcv formulations presented in Sect. II using the measured noise parameters and S-parameters of the LNA previously measured in [9]. note that all three different methods presented converges for various pointing direction and array configurations (uniform and pseudo-random configuration) which indicated agreement in current literature of computing receiver noise temperature.…”
Section: Resultssupporting
confidence: 70%
“…Following noise extraction of a low noise amplifier (LNA) as utilized by the Murchision Widefield Array (MWA) [7], [8] seen in [9], we now aim to compute the receiver noise temperature of MWA, which is a uniform array, and Engineering Development Array (EDA) [3], which is a pseudo-random array using existing formulations which accounts for mutual coupling.…”
Section: Introductionmentioning
confidence: 99%
“…The frequency of interest was 154.88 MHz, which corresponded to the channel number 121. To calculate the system temperature, we also used measured S-parameters and noise parameters of the LNA (Sutinjo et al 2018), as well as the Haslam 408 MHz all-sky map (Haslam et al 1982) scaled to 154.88 MHz using a spectral index of −2.55 (Mozdzen et al 2019). The Galactic contribution corresponded to the day and time of the observation.…”
Section: Simulation Predictions For the Mwamentioning
confidence: 99%
“…From this information, we obtain T sky ≈ 228 K (ν/150 MHz) −2.53 at the location of the CDFS. Following Wayth et al (2015), we set T rec = 50 K except at ν > 200 MHz, where we set T rec = 80 K; laboratory measurements by Sutinjo, Ung, & Juswardy (2018), indicate that T rec ≈ 80 K at ν > 200 MHz. We set B = 0.75 × 7.68 MHz given a 25% reduction in the bandwidth due to flagged edge channels.…”
Section: Estimating the Thermal Noisementioning
confidence: 99%