1995
DOI: 10.1049/ip-vis:19951559
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Modelling of acoustic transfer functions for echo cancellers

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Cited by 6 publications
(4 citation statements)
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“…Then, the (MoorePenrose) pseudoinverse [33] of is given by where the map is defined by Proof: From a property of pseudoinverses, we have (22) Now, for all and , hence (23) and the result follows by putting (23) and Lemma 1 into (22). Below, we use Lemma 3 to prove (9), (10), and (11).…”
Section: Appendix Proofsmentioning
confidence: 99%
See 2 more Smart Citations
“…Then, the (MoorePenrose) pseudoinverse [33] of is given by where the map is defined by Proof: From a property of pseudoinverses, we have (22) Now, for all and , hence (23) and the result follows by putting (23) and Lemma 1 into (22). Below, we use Lemma 3 to prove (9), (10), and (11).…”
Section: Appendix Proofsmentioning
confidence: 99%
“…Proof of (11): Let be the subspace of subband models whose support is defined by the matrices and , and let be the projection onto . Consider the map defined by .…”
Section: Appendix Proofsmentioning
confidence: 99%
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“…Typical all-pole model orders required for approximating RTFs are in the range 50 ≤ P ≤ 500 [32]. Mourjopoulos and Paraskevas [32] state that all-pole model orders are typically a factor of 40 lower than all-zero model orders, while several studies [33,34] state that the gain achieved using pole-zero over all-zero modelling of reverberant environments is not as high as generally thought throughout the literature. A significant advantage of the all-pole model over other LTI models is its lower sensitivity to changes in source and observer positions.…”
Section: A All-pole Model For Room Acousticsmentioning
confidence: 99%