Traditional photolithography has a resolution at wavelength scale due to optical diffraction. In this paper, a high-density direct photolithography method beyond diffraction limit by utilizing surface plasmons (SPs) was developed on virtually any substrate. Simulation results by Finite Different Time Domain (FDTD) method have shown that surface plasmon excited on both the mask and the substrate helps to confine the light behind the apertures of the mask. Numerical simulations have demonstrated that very high density sub-wavelength patterns can be transferred using this method. In experiments, a polarized laser beam of 355nm wavelength was used as a light source to photo-initiate a 80nm-thick photoresist on a silicon substrate with 50nm Ti coating. 100nm line aperture patterns were made on gold film on quartz substrate as mask. Experimental results showed that illumination intensity control is crucial to the lithography results. The feature size using such method could be further scaled down, limited theoretically by the validity of dielectric function of the material, and practically by the fabrication of mask.

1.
Okazaki
S.
, “
Resolution limits of optical lithography
,”
Journal of Vacuum Science and Technology
, B
9
,
2829
2833
(
1991
).
2.
Kunz
R.
,
Rothschild
M.
and
Yeung
M. S.
, “
Large-area patterning of 50 nm structures on flexible substrates using near-field 193 nm radiation
,”
Journal of Vacuum Science and Technology
,
B 21
,
78
78
(
2003
).
3.
Goodberlet
J. G.
and
Kavak
H.
, “
Patterning Sub-50 nm features with near-field embedded-amplitude masks
,”
Applied Physics Letters
,
81
,
1315
1315
(
2002
).
4.
Schmid
H.
,
Biebuyck
H.
,
Michel
B.
and
Martin
O. J. F.
, “
Light-coupling masks for lensless, sub-wavelength optical lithography
,”
Applied Physics Letters
,
72
,
2379
2379
(
1998
).
5.
H. Raether, “Surface Plasmons on Smooth and Rough Surfaces and on Gratings,” Berlin, 1988.
6.
Ebbesen
T. W.
,
Lezec
H. J.
,
Ghaemi
H. F.
,
Thio
T.
, and
Wolff
P. A.
, “
Extraordinary optical transmission through subwavelength hole arrays
,”
Nature (London)
391
,
667
669
(
1999
).
7.
Pendry
J.
, “
Playing Tricks with Light
,”
Science
285
,
1687
1688
(
2002
).
8.
Popov
E.
,
Neviere
M.
,
Enoch
S.
, and
Reinisch
R.
, “
Theory of light transmission through subwavelength periodic hole arrays
,”
Physical Review B
.
62
16100
16100
(
2000
).
9.
Srituravanich
W.
,
Fang
N.
,
Sun
C.
,
Luo
Q.
, and
Zhang
X.
, “
Surface Plasmonic Lithography
,”
Nano Letter
,
4
,
1085
1085
(
2004
).
10.
Luo
X.
,
Ishihara
T.
, “
Surface plasmon resonant interference nanolithography technique
,”
Applied Physics Letters
84
,
4780
4780
(
2004
).
11.
Yee
K. S.
, “
Numerical solution of initial boundary value problems involving Maxwell’s equations in isotropic media
,”
IEEE Transactions on Antennas and Propagation
, vol.
14
, pp.
302
307
, May
1966
.
12.
Krug
J. T.
,
Sa’nchez
E. J.
, and
Xie
X. S.
, “
Design of Near-field Optical Probes with Optimal Field Enhancement by Finite Difference Time Domain Electromagnetic Simulation
,”
Journal of Chemical Physics
,
116
,
10895
10895
(
2002
).
13.
Berenger
J. P.
, “
A Perfectly Matched Layer for the Absorption of Electromagnetic Waves
,”
Journal of Computational Physics
,
114
,
185
185
(
1994
).
14.
Gray
S. K.
and
Kupka
T.
, “
Propagation of light in metallic nanowire arrays: Finite-difference time-domain studies of silver cylinders
,”
Physical Review B
,
68
,
045415
045415
(
2003
).
15.
E. D. Palik, “Handbook of optical constants of solids,” Academic Press, Orlando, 1985.
16.
P. W. Barber, S. C. Hill, “Light Scattering by Particles: Computational Methods,” World Scientific, Singapore, 1990.
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