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Applied Physics Letters

Volumn 98, Issue 26, 2011, Pages

Superlensing effect of an anisotropic metamaterial slab with near-zero dynamic mass

(2) Zhou, Xiaoming a Hu, Gengkai a

a BEIJING UNIVERSITY OF POSTS AND TELECOMMUNICATIONS (China)

Author keywords

[No Author keywords available]

Indexed keywords

ANISOTROPIC METAMATERIALS; DIFFRACTION LIMITS; EVANESCENT WAVE; EXTRAORDINARY TRANSMISSION; MASS EFFECTS; MICROSTRUCTURE DESIGN; NUMERICAL MODELING; SUPERLENSES; SUPERLENSING; UNDERLYING MECHANISM;

ACOUSTIC IMAGING; METAMATERIALS; WAVE TRANSMISSION;

ANISOTROPY;

EID: 79960088050 PISSN: 00036951 EISSN: None Source Type: Journal
DOI: 10.1063/1.3607277 Document Type: Article

Times cited : (87)

References (13)

1
- 0003972070
- 7th ed. (Cambridge University Press, Cambridge, England).
- M. Born and E. Wolf, Principles of Optics, 7th ed. (Cambridge University Press, Cambridge, England, 1999).
- (1999) Principles of Optics
- Born, M.¹ Wolf, E.²

2
- 0034296247
- Negative refraction makes a perfect lens
- DOI 10.1103/PhysRevLett.85.3966
- J. B. Pendry, Phys. Rev. Lett. 85, 3966 (2000). 10.1103/PhysRevLett.85. 3966 (Pubitemid 32027228)
- (2000) Physical Review Letters , vol.85 , Issue.18 , pp. 3966-3969
- Pendry, J.B.¹

3
- 36049031273
- Acoustic metamaterials for sound focusing and confinement
- DOI 10.1088/1367-2630/9/11/399, PII S1367263007453058
- S. Guenneau, A. Movchan, G. Pétursson, and S. Ramakrishna, New J. Phys. 9, 399 (2007). 10.1088/1367-2630/9/11/399 (Pubitemid 350099180)
- (2007) New Journal of Physics , vol.9 , pp. 399
- Guenneau, S.¹ Movchan, A.² Petursson, G.³ Ramakrishna, S.A.⁴

4
- 65649131982
- 10.1103/PhysRevLett.102.194301
- S. Zhang, L. Yin, and N. Fang, Phys. Rev. Lett. 102, 194301 (2009). 10.1103/PhysRevLett.102.194301
- (2009) Phys. Rev. Lett. , vol.102 , pp. 194301
- Zhang, S.¹ Yin, L.² Fang, N.³

5
- 34347335747
- 10.1103/PhysRevB.75.195447
- M. Ambati, N. Fang, C. Sun, and X. Zhang, Phys. Rev. B 75, 195447 (2007). 10.1103/PhysRevB.75.195447
- (2007) Phys. Rev. B , vol.75 , pp. 195447
- Ambati, M.¹ Fang, N.² Sun, C.³ Zhang, X.⁴

6
- 67650251844
- 10.1063/1.3153976
- K. Deng, Y. Ding, Z. He, H. Zhao, J. Shi, and Z. Liu, J. Appl. Phys. 105, 124909 (2009). 10.1063/1.3153976
- (2009) J. Appl. Phys. , vol.105 , pp. 124909
- Deng, K.¹ Ding, Y.² He, Z.³ Zhao, H.⁴ Shi, J.⁵ Liu, Z.⁶

7
- 69449104453
- 10.1103/PhysRevE.80.026603
- F. Liu, F. Cai, S. Peng, R. Hao, M. Ke, and Z. Liu, Phys. Rev. E 80, 026603 (2009). 10.1103/PhysRevE.80.026603
- (2009) Phys. Rev. e , vol.80 , pp. 026603
- Liu, F.¹ Cai, F.² Peng, S.³ Hao, R.⁴ Ke, M.⁵ Liu, Z.⁶

8
- 78650573862
- 10.1038/nphys1804
- J. Zhu, J. Christensen, J. Jung, L. Martin-Moreno, X. Yin, L. Fok, X. Zhang, and F. J. Garcia-Vidal, Nat. Phys. 7, 52 (2010). 10.1038/nphys1804
- (2010) Nat. Phys. , vol.7 , pp. 52
- Zhu, J.¹ Christensen, J.² Jung, J.³ Martin-Moreno, L.⁴ Yin, X.⁵ Fok, L.⁶ Zhang, X.⁷ Garcia-Vidal, F.J.⁸

9
- 46349109609
- 10.1088/1367-2630/10/4/043020
- S. Yao, X. Zhou, and G. Hu, New. J. Phys. 10, 043020 (2008). 10.1088/1367-2630/10/4/043020
- (2008) New. J. Phys. , vol.10 , pp. 043020
- Yao, S.¹ Zhou, X.² Hu, G.³

10
- 33749649082
- Tunneling of electromagnetic energy through subwavelength channels and bends using ε-near-zero materials
- DOI 10.1103/PhysRevLett.97.157403
- M. Silveirinha and N. Engheta, Phys. Rev. Lett. 97, 157403 (2006). 10.1103/PhysRevLett.97.157403 (Pubitemid 44547767)
- (2006) Physical Review Letters , vol.97 , Issue.15 , pp. 157403
- Silveirinha, M.¹ Engheta, N.²

11
- 77958580696
- 10.1088/1367-2630/12/10/103025
- S. Yao, X. Zhou, and G. Hu, New. J. Phys. 12, 103025 (2010). 10.1088/1367-2630/12/10/103025
- (2010) New. J. Phys. , vol.12 , pp. 103025
- Yao, S.¹ Zhou, X.² Hu, G.³

12
- 79960079281
- See C. E. S. Selector 4.0 for information about the rubber material.
- See C. E. S. Selector 4.0 for information about the rubber material (http://www.grantadesign.com/products/ces/).

13
- 79960076908
- In the macro-cell unit (c é 0) of the slab lens normally incident by plane acoustic waves, effective bulk modulus and effective mass density are computed by = S ( ii / 3) dS / ( right udl - left udl) and = ( right pdl - left pdl) / ( 2 S udS), where ij is the stress tensor, u is the x-component of the displacement, is the pressure, the subscripts S', left', and right' represent, respectively, the integration over the surface, left and right boundaries of the unit.
- In the macro-cell unit (c = 0) of the slab lens normally incident by plane acoustic waves, effective bulk modulus and effective mass density are computed by = S ( ii / 3) dS / ( right udl- left udl) and = ( right pdl- left pdl) / ( 2 S udS), where ij is the stress tensor, u is the x-component of the displacement, p is the pressure, the subscripts S', left', and right' represent, respectively, the integration over the surface, left and right boundaries of the unit.

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