Abstract

A new type of optical configuration—a solid immersion axicon (SIAX)—is proposed. Similar to a solid immersion lens for Gaussian beams, a SIAX increases the diffraction-limited resolution for propagating Bessel beams by a factor of the refractive index of the media. For incident radial polarization, the scheme generates the smallest focal spot available for nondiffracting beams. The configuration can be implemented with either refractive or diffractive axicons. The scheme may find use in microscopy, imaging, lithography and data storage, and other applications requiring nondiffracting beam characteristic features such as very large focal depth.

© 2007 Optical Society of America

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References

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2007 (3)

2006 (1)

2004 (3)

2003 (3)

U. T. Schwarz, J. Zeitler, J. Baier, M. Maier, and S. Sogomonian, J. Opt. Soc. Am. B 20, 1750 (2003).
[CrossRef]

T. Grosjean, D. Courjon, and D. Van Labeke, J. Microsc. 210, 319 (2003).
[CrossRef] [PubMed]

R. Dorn, S. Quabis, and G. Leuchs, Phys. Rev. Lett. 91, 233901 (2003).
[CrossRef] [PubMed]

2002 (2)

K. Cohn, D. Simanovskii, T. Smith, and D. Palanker, Appl. Phys. Lett. 81, 3678 (2002).
[CrossRef]

Z. Ding, H. Ren, Y. Zhao, J. S. Nelson, and Z. Chen, Opt. Lett. 27, 243 (2002).
[CrossRef]

2001 (2)

L. E. Helseth, Opt. Commun. 191, 161 (2001).
[CrossRef]

S. B. Ippolito, B. B. Goldberg, and M. S. Unlu, Appl. Phys. Lett. 78, 4071 (2001).
[CrossRef]

1998 (1)

1997 (1)

1995 (1)

1993 (2)

1992 (1)

1991 (1)

1990 (2)

I. Golub and R. Tremblay, J. Opt. Soc. Am. B 7, 1264 (1990).
[CrossRef]

S. M. Mansfield and G. S. Kino, Appl. Phys. Lett. 57, 2615 (1990).
[CrossRef]

1989 (1)

1988 (1)

1987 (1)

1980 (1)

1978 (1)

1960 (1)

J. H. McLeod, J. Opt. Soc. Am. 50, 592 (1960).
[CrossRef]

1954 (1)

Appl. Opt. (6)

Appl. Phys. Lett. (3)

S. M. Mansfield and G. S. Kino, Appl. Phys. Lett. 57, 2615 (1990).
[CrossRef]

S. B. Ippolito, B. B. Goldberg, and M. S. Unlu, Appl. Phys. Lett. 78, 4071 (2001).
[CrossRef]

K. Cohn, D. Simanovskii, T. Smith, and D. Palanker, Appl. Phys. Lett. 81, 3678 (2002).
[CrossRef]

J. Microsc. (1)

T. Grosjean, D. Courjon, and D. Van Labeke, J. Microsc. 210, 319 (2003).
[CrossRef] [PubMed]

J. Opt. Soc. Am. (3)

J. Opt. Soc. Am. A (3)

J. Opt. Soc. Am. B (2)

Opt. Commun. (2)

T. Grosjean and D. Courjon, Opt. Commun. 272, 314 (2007).
[CrossRef]

L. E. Helseth, Opt. Commun. 191, 161 (2001).
[CrossRef]

Opt. Lett. (8)

Phys. Rev. Lett. (2)

R. Dorn, S. Quabis, and G. Leuchs, Phys. Rev. Lett. 91, 233901 (2003).
[CrossRef] [PubMed]

T. Wulle and S. Herminghaus, Phys. Rev. Lett. 70, 1401 (1993).
[CrossRef] [PubMed]

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Figures (3)

Fig. 1
Fig. 1

(a) A SIL increases the NA of a focused Gaussian beam by a factor n. (b) A SIAX increases the NA of a propagating Bessel beam by a factor n. (c) Ray tracing for a SIAX with NA=0.9 (base angle β = 64.8 ° ) accommodating an incident Bessel beam with convergence angle θ = β .

Fig. 2
Fig. 2

Bessel beams generated by an axicon with an apex facing toward (a) the image and (b) the object while in contact with a medium with refractive index n.

Fig. 3
Fig. 3

Comparison of convergence angles for the schemes shown in Figs. 2a (solid curve, θ 1 ) and 2b (dashed curve, θ 2 ) as a function of the base angle of the axicon for n = 1.45 .

Equations (6)

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β = θ = arc sin ( n sin α ) α .
θ 1 = arc ( n sin α ) α ,
θ 2 = α arc sin ( sin α n ) .
E r cos θ J 1 ( k r sin θ ) ,
E z sin θ J 0 ( k r sin θ ) ,
D Bessel 0.36 λ NA ,

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