Direct Measurement of the Reaction Front in Chemically Amplified
Photoresists
The continual device performance
increases by the semiconductor industry has been largely driven by
the fabrication of smaller structures with lithography. As feature
sizes approach sub-100 nm, the photolithographic process must be controlled
with tolerances of (2 to 5) nm, dimensions comparable to the molecular
size of the polymer chains in the photoresist imaging material. New
experimental methods are needed to measure transport and materials
science phenomena over nanometer length scales to provide critically
needed data for the understanding, design, and control of new lithographic
materials and processes. In collaboration with IBM and the University
of Texas, we directly measured the spatial evolution of a reaction
front, within a photoresist, with nanometer resolution using neutron
and x-ray reflectometry and a deuterium-labeled photoresist polymer.
Figure 1. At left, SEM image of a lithographically fabricated
structure with a nominal critical dimension of 150 nm and 300 nm
pitch. At right, schematic illustration of patterning through a
mask to create the structure.
The semiconductor industry is rapidly approaching the need to fabricate
sub-100 nm structures to continue performance increases in integrated
circuits. Photolithography remains the enabling technology for the
fabrication of integrated circuit patterns. Although industry is
able to commercially produce 130 nm features, lithographic materials
and processes are not fully available for the production of sub-100
nm structures. New materials must be able to produce structures
with dimensional tolerances of (2 to 5) nm, dimensions near the
size of the polymer chain molecules in the imaging layer.
Current imaging layers, chemically amplified photoresists, are
multi-component materials consisting of a polymer resin initially
insoluble in an aqueous base developer solution, a photoacid generator
(PAG), and other additives. A schematic diagram of the fabrication
process and an example structure are shown in Figures 1 and 2. The
patterns are generated in the resist by exposure to UV radiation
through a mask. In the exposed areas, the PAG decomposes forming
an acid species. Upon baking, the acid diffuses and catalyzes a
deprotection reaction rendering the insoluble resist soluble in
a developer. The soluble regions are then removed with the aqueous
base developer. Control over this process is dominated by the events
in the transitional region between exposed and unexposed areas of
the photoresist.
Figure 2. Schematic diagram of the reaction-diffusion process
in chemically amplified photoresists. The transitional region between
exposed and unexposed regions is particularly important for critical
dimension and roughness control
The initial development of chemically amplified photoresists was
a key technological breakthrough furthering the continued use of
optical photolithography for the fabrication of sub?micrometer features.
The importance of chemically amplified photoresist concepts is illustrated
by the industry-wide use of these materials in the fabrication of
state-of-the-art devices today and into the foreseeable future.
With the imminent need for sub-100 nm feature sizes, nanometer level
control over the spatial evolution of the deprotection reaction
front and the subsequent development steps is needed. The current
level of understanding of the acid-catalyzed reaction-diffusion
process is not sufficiently detailed to achieve this goal.
Figure 3. General deprotection reaction in a chemically
amplified photoresist. Deuterated molecular parts with strong contrast
to neutrons are shown in red. PHOSt= polyhydroxystyrene, PBOCSt=
poly p-tert-butoxycarboxystyrene.
To meet the need for spatially detailed data, we have developed,
in collaboration with the IBM T. J. Watson Research Center and the
University of Texas at Austin, an experimental methodology to measure
directly the spatial evolution of the deprotection reaction front
through each processing step. By using model photoresist polymers
with a deuterated protection group, neutron and x?ray reflectivity
(NR, XR) measurements are able to follow the compositional and density
profiles of the reaction-diffusion process in an idealized transitional
region in a bilayer film stack. Neutron contrast with the reaction
is possible because the reaction products involving the deuterated
protection group are volatile as illustrated in Figure 3.
The NR and XR results from a series of bilayer samples are shown
in Figure 4. NR and XR measurements were taken after each processing
step from the spin-coating of each film layer through exposure and
bake to the dissolution of the upper layer and any deprotected polymer.
The data show that the deprotection reaction front broadens with
time within the photoresist. The initial interfacial width was approximately
4 nm wide whereas the reaction front was nearly 20 nm wide. Upon
development, the data show that the developed film remained sharply
defined with a surface roughness of approximately 4 nm as well.
Although the reaction front was much wider than the final interfacial
width, the selectivity of the dissolution process allows for the
fabrication of well-defined nanostructures with diffusive transport
mechanisms.
Figure 4. A) schematic diagram of the processing steps including
the application of each film layer, exposure to UV radiation, a
post-exposure bake (PEB) and development. B) and D) show the NR
data and compositional depth profile and C) and E) show the XR data
and density depth profiles from each step.
The spatial detail afforded by the developed methodology can play
an important role in not only the qualitative description of the
reaction-diffusion process, but also with the quantitative determination
of physical parameters and changes in any physical or chemical properties
over the nanometer length scales required for control over the fabrication
of sub-100 nm structures. In addition, the strategy developed here
is general and can be adapted for the study of candidate photoresist
materials being developed for future applications.
"[This work] opens a window of opportunity to construct
structure-property relationships between chemical transport mechanisms
and ultimate resist resolution. It may also lead to insights into
the ultimate, intrinsic resolution limits and critical dimension
control of polymer-based imaging materials."
E. Reichmanis and O. Nalamasu, Bell Labs, Lucent Technologies,
Science, 297, 349 (2002).
For more information on this topic:
E. K. Lin, C. L. Soles, R. L. Jones, J. L. Lenhart, W. L. Wu (Polymers
Division, NIST); S. K. Satija (NCNR, NIST).
E. K. Lin, C. L. Soles, D. L. Goldfarb, B. C. Trinque, S. D. Burns,
R. L. Jones, J. L. Lenhart, M. Angelopoulos, C. G. Willson, S. K.
Satija, and W. L Wu, "Direct Measurement of the Reaction Front
in Chemically Amplified Photoresists," Science, 297, 372 (2002).
NIST Material
Science & Engineering Laboratory - Polymers Division