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Analytical Approaches to Electroacoustic Music Improvisation

Published online by Cambridge University Press:  27 January 2022

Pierre Couprie*
Affiliation:
Centre for Cultural History of Contemporary Societies (CHCSC), Paris-Saclay University, France
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Abstract

This article introduces a framework for musical analysis applied to electroacoustic improvisation. After an introduction about the benefits of interdisciplinary research and research-creation practice there is a description of the different domains of the framework: acoustic analysis, music analysis itself and the design of graphic representations. The framework is based on the extraction of information from the audio signal (music information retrieval) to create data representations, some of which are very efficient for music analysis, such as the brightness standard deviation or the self-similarity matrix. The last part of the article demonstrates the use of the framework on extracts of electroacoustic improvisations performed by the Paris-based group Les Phonogénistes, of which the author is a member.

Information

Type
Article
Copyright
© The Author(s), 2022. Published by Cambridge University Press
Figure 0

Figure 1. The framework for the analysis of electroacoustic music.

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Figure 2. The principle of producing a BStD. Compared with other types of graphs, a flow curve such as BStD facilitates the interpretation and correlation between several descriptor data.

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Figure 3. The computation method of self-similarity matrix.

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Figure 4. Schematic diagram of the performance DMIs and devices of each musician (A, B and C).

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Figure 5. BStD (A, B and C) based on RMS amplitude, spectral variance, ZCR; waveform on the global mix (Sound Example 1).

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Figure 6. Logarithmic FFT representation of the global mix (Sound Example 2).

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Figure 7. A self-similarity matrix computed on the FFT and a formal segmentation (top) of the four parts of the improvised performance.

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Figure 8. Self-similarity matrix computed on RMS amplitude, spectral rolloff, spectral variance and ZCR with segmentation in five zones on top (Movie Example 1).

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Figure 9. Two self-similarity matrices calculated from the FFT (1 at top of figure) and from the RMS amplitude, spectral rolloff, spectral variance and ZCR (2 at centre of the figure), and the waveform (bottom) (Movie Example 2).

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Figure 10. Three self-similarity matrices calculated for each musician on the FFT (Movie example 3).