2011
DOI: 10.1111/j.1365-2478.2011.01006.x
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Comparison of pseudo‐random binary sequence and square‐wave transient controlled‐source electromagnetic data over the Peon gas discovery, Norway

Abstract: A B S T R A C TWe discuss the problem of source control in controlled-source electromagnetic (CSEM) surveying and compare and contrast equal energy transient square-wave and transient pseudo-random binary sequence source signatures for the same towedstreamer electromagnetic survey line over the Peon gasfield in the Norwegian sector of the North Sea. The received response of the transient square-wave data was 11 dB greater than that of the pseudo-random binary sequence data, due to diffusive attenuation of high… Show more

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Cited by 48 publications
(10 citation statements)
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“…Therefore, the detection accuracy for the targets at different depths could be optimized (Li, Xue, Zhao, Zhong, & Muhammad Younis, ; Li, Xue, & Zhong, ). Furthermore, the deconvolution of a PRBS signal increases the signal‐to‐noise ratio in the time domain by compressing the signal energy to a shorter time (Ziolkowski, Wright, & Mattsson, ). The autocorrelation properties of PRBS signals allow the deconvolution of the measured responses to be conducted in the time domain.…”
Section: Principles Of the Mtem Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…Therefore, the detection accuracy for the targets at different depths could be optimized (Li, Xue, Zhao, Zhong, & Muhammad Younis, ; Li, Xue, & Zhong, ). Furthermore, the deconvolution of a PRBS signal increases the signal‐to‐noise ratio in the time domain by compressing the signal energy to a shorter time (Ziolkowski, Wright, & Mattsson, ). The autocorrelation properties of PRBS signals allow the deconvolution of the measured responses to be conducted in the time domain.…”
Section: Principles Of the Mtem Methodsmentioning
confidence: 99%
“…It is crucial that the uncorrelated noise is eliminated during this process. Then, Equation could be written in matrix form as follows (Ziolkowski et al, ): []Rss()0Rss()1Rss()NRss()1Rss()0Rss()N1Rss()NRss()N1Rss()0[]g()0g()1g()N=[]Rvs()0Rvs()1Rvs()N. The coefficient matrix in Equation is a Toeplitz matrix, which can be solved efficiently using a Levinson recursion.…”
Section: Principles Of the Mtem Methodsmentioning
confidence: 99%
“…, ). A towed source and receiver system in water column was also used by Ziolkowski, Wright and Mattsson () in time‐domain CSEM measurements. For the discussion of topography effects, a towed system is also taken into account.…”
Section: Introductionmentioning
confidence: 99%
“…The Federal Institute for Geosciences and Natural Resources in Germany (BGR) used a bottom towed system mainly for the exploration of gas hydrate (one T x and 4 R x s with fixed offsets), while the cable length between T x and R x s are fixed (Schwalenberg et al 2010(Schwalenberg et al , 2017. A towed source and receiver system in water column was also used by Ziolkowski, Wright and Mattsson (2011) in time-domain CSEM measurements. For the discussion of topography effects, a towed system is also taken into account.…”
Section: Introductionmentioning
confidence: 99%
“…This led to an amplitude 'split' (i.e., the deviation between the anomaly site and reference sites), which was larger than that can be generated by reasonable variations in the overburden resistivity. The towed electromagnetic (EM) system of Petroleum Geo-Services (PGS) (Ziolkowski, Wright, and Mattsson 2011;Linfoot, Mattsson, and Price 2011) uses a moving source and the spread of inline E-field receivers, which are mounted on a streamer, where both the source and the receiver are towed by the same vessel. Kasaya and Goto (2009) developed a small ocean bottom electro magnetometer (OBEM) and ocean bottom electrometer (OBE) system equipped with a fluxgate magnetic sensor and arm-folding mechanism, where all of the electronic components are inside a single 17-inch (432-mm) glass sphere.…”
Section: Introductionmentioning
confidence: 99%