1979
DOI: 10.1109/proc.1979.11277
|View full text |Cite
|
Sign up to set email alerts
|

Holography and its application to acoustic imaging

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
4
0

Year Published

1980
1980
2022
2022

Publication Types

Select...
5
2

Relationship

0
7

Authors

Journals

citations
Cited by 25 publications
(4 citation statements)
references
References 45 publications
0
4
0
Order By: Relevance
“…cf. also the Ultrasonic Testing Documentation of the BAM [4] and the following publications [880,937,1649,1075,1360,1363,58 (containing many earlier references), 60, 1364, 881,…”
Section: Linear Holography; Holosafi' Methodsmentioning
confidence: 99%
“…cf. also the Ultrasonic Testing Documentation of the BAM [4] and the following publications [880,937,1649,1075,1360,1363,58 (containing many earlier references), 60, 1364, 881,…”
Section: Linear Holography; Holosafi' Methodsmentioning
confidence: 99%
“…Acoustic holography [1,2] is an essential tool for controlling sound waves, generating highly complex and customizable sound fields, and enabling the visualization of sound fields. Due to its powerful and flexible capability of arbitrary sound beam shaping and predesigned sound field reconstruction, acoustic holography has recently received increased attention in many interdisciplinary fields related to acoustics, including medicine [3][4][5][6], engineering [7,8], and biology [9][10][11], in addition to the pure acoustic field.…”
Section: Introductionmentioning
confidence: 99%
“…The set of acquired microphone signals are then processed in order to extract the relevant information. Several methods can then be used to recover sound sources: holography [1], beamforming [2,3], and time reversal [4][5][6] among others.…”
Section: Introductionmentioning
confidence: 99%
“…= Vector of 3D-coordinates x = (x, y, z) s i = Signal of source i, kg/s 2 p m , p = Pressure at microphone m, Pa g i,m , g i = Green's function between source i and microphone m g = Concatenation of all the Green's functions g 1 , · · · , g N S for a given microphone m S = Training set S = Validation set A (q) i = Active set at iteration q relative to source i A (q) = Global active set at iteration q * = Convolution product * Ph.D. candidate, ONERA DAAA -Aerodynamics Aeroelasticity Acoustics, sofiane.bousabaa@onera.fr † Research Engineer, ONERA DAAA -Aerodynamics Aeroelasticity Acoustics, jean.bulte@onera.fr ‡ Research Engineer, ONERA DAAA -Aerodynamics Aeroelasticity Acoustics, daniel-ciprian.mincu@onera.fr § Professor, Institut Jean Le Rond d'Alembert, UPMC -Paris 6, regis.marchiano@upmc.fr ¶ Assistant Professor, Institut Jean Le Rond d'Alembert, UPMC -Paris 6, francois.ollivier@upmc.fr ⊗ = Cross-correlation product j l , y l = Spherical Bessel functions of order l h (1) l , h (…”
mentioning
confidence: 99%