[1] [1] KRYLOV V V. Laminated plates of variable thickness as effective absbers f flexural vibrations[C]Proceedings of the 17th International Congress on Acoustics(ICA), Rome: The Acoustic Society of Italiy, 2001: 270−271.

[2] KRYLOV V V, TILMAN F J B S. Acoustic 'black holes' for flexural waves as effective vibration dampers[J]. Journal of Sound and Vibration, 274, 605-619(2004).

[3] KRYLOV V V. New type of vibration dampers utilising the effect of acoustic 'black holes'[J]. Acta Acustica United with Acustica, 90, 830-837(2004).

[4] KRYLOV V V, WINWARD R E T B. Experimental investigation of the acoustic black hole effect for flexural waves in tapered plates[J]. Journal of Sound and Vibration, 300, 43-49(2007).

[5] CONLON S C, FAHNLINE J B, SEMPERLOTTI F. Numerical analysis of the vibroacoustic properties of plates with embedded grids of acoustic black holes[J]. The Journal of the Acoustical Society of America, 137, 447-457(2015).

[6] [6] CONLON S C, FAHNLINE J B, SEMPERLOTTI F, et al. Enhancing the low frequency vibration reduction perfmance of plates with embedded acoustic black holes[C]INTERNOISE NOISECON Congress Conference Proceedings. Austin, TX: Applied Research Labaty (ARL), 2014.

[7] [7] CONLON S C, FAHNLINE J B, SHEPHERD M R, et al. Vibration control using grids of acoustic black holes: how many is enough[C]Proceedings of the 44th International Congress Exposition on Noise Control Engineering INTERNOISE 2015. San Francisco: [s. n.], 2015.

[9] ZHAO L X, CONLON S C, SEMPERLOTTI F. Broadband energy harvesting using acoustic black hole structural tailoring[J]. Smart Materials and Structures, 23, 065021(2014).

[12] MIRONOV M A. Propagation of a flexural wave in a plate whose thickness decreases smoothly to zero in a finite interval[J]. Soviet Physics-Acoustics, 34, 318-319(1988).

[13] [13] HELMAN G. On the effects of the addition of mass to vibrating systems: AFOSR TN 56387 [R]. [S.1: s.n], 1956.