The critical dimension (CD) limits of conventional optical lithography foll
ow directly from the low-pass filter characteristics of the imaging optical
system (\k\less than or equal to 2 pi NA/lambda where lambda is the optica
l wavelength and NA the numerical aperture). In contrast, the linear system
s limits of optics extend to spatial frequencies of 4 pi/lambda (interferen
ce between counterpropagating beams at grazing incidence). Imaging interfer
ometric lithography is introduced as a technique to approach this linear sy
stems limit while retaining the arbitrary pattern capability of an imaging
optical system. Multiple, wavelength-division-multiplexed exposures are use
d, each exposure recording a different portion of frequency space. A conven
tional, coherent illumination exposure provides the low frequency informati
on, within the lens passband. Offset exposures provide the high spatial fre
quency information. Off-axis illumination shifts a portion of the high spat
ial frequency diffraction from the mask into the lens passband and interfer
ence with a reference beam resets the frequencies once they are transmitted
through the optical system. For a typical x-y geometry pattern, offset exp
osures in the x and y directions provide a sufficient coverage of frequency
space. Model calculations illustrate that the imaging capabilities of imag
ing interferometric lithography (ILL) for dense features extend to -lambda/
3 (130 nm at I line; 65 nm at an ArF exposure wavelength). Initial experime
nts are reported at I line with a modest (NA=0.04) optical system. The resu
lts are in good agreement with the model calculations. A resolution enhance
ment of similar to 3 X from dense 6 mu m CDs for a conventional, coherent i
llumination exposure to similar to dense 2 mu m CDs for an IIL exposure seq
uence is demonstrated. (C) 1998 American Vacuum Society.