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Recent advancements in the semiconductor industry have resulted
in new problems involving the photoresist-liquid interface. For immersion
lithography, the water profile within a resist film impacts pattern
quality from changes in photoacid generator diffusion or optical transparency.
For the development step, where a latent image is realized into the
final structure, an improved understanding of photoresist swelling
and dissolution mechanisms is needed to address stringent line-edge
roughness requirements. Data from neutron reflectivity measurements
provide critical insight needed to understand and optimize next-generation
photoresists and process strategies. |
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Bryan D. Vogt and Vivek
M. Prabhu |
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Introduction
Polymer thin film photoresists comprise the materials foundation for
the production of semiconductor devices with nanoscale dimensions.
The extension of optical methods has been problematic due to challenges
arising from the implementation of shorter exposure wavelengths. The
past focus of the semiconductor industry has been the development
of sufficiently transparent photoresist materials for future exposure
sources. However, future progress requires depth profile information
at the photoresist-liquid interface, due to the emergence of immersion
lithography and the increased influence of the photoresist development
process on lithographic performance.
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Using neutron reflectivity (NR), NIST successfully quantified the
profile of water and aqueous base counterions in model photoresist
films. NR provides structural information regarding the composition
profile normal to the thin film surface with isotopic selectivity
between protons and deuterium. Selective deuteration of components
in the system allows for the quantification of water or counterion
distribution within photoresist films despite the negligible differences
in physical density. This data provide critical insight needed to
refine models for immersion lithography and polymer dissolution. |
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Immersion Lithography: Water Profile
Recently, immersion lithography has emerged as the key strategy to
extend existing optical tools. A liquid, such as water, is placed
between the lens and photoresis thin film to enhance resolution. The
industry anticipates using immersion lithography for production in
2007 at the 65 nm node. The role of liquids in contact with photoresist
films is important; not only for component leaching and contamination,
but also due to the detrimental influence of trace levels of water
on the reaction and diffusion of photoacid generators. Additionally,
a non-uniform water profile within thin films leads to incorrect assumptions
regarding the transmission and reflection at the photoresist-anti-reflective
coating interface. |
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Figure 1: Volume fraction of water distributed
near the PBOCSt/HMDS treated substrate during immersion, as determined
by neutron reflectivity. The excess of water at the substrate reaches
a maximum concentration of 17 % by volume. Inset. Dependence of initial
film thickness on the total film swelling for two model photoresists
in thin and ultrathin films. |
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Figure 1 shows the measured volume fraction profile of water versus
the distance from a trimethylsilane-primed silicon oxide interface.
Far from the substrate, the 248 nm photoresist, poly(4-tert-butoxycarbonlyoxystyrene)
(PBOCSt), shows bulk water absorption, near 2.5 %. However, significant
deviations occur near the interface. An excess of water, up to 17
%, extends 40 Å from the substrate. This enriched interfacial
water was previously unknown and unaccounted for. |
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In contrast, a depletion of water was observed for poly(4-hydroxystyrene)
(PHOSt), the developer soluble resist, even though the bulk of the
film absorbs 25 %. This depletion indicates the interface cannot accommodate
excess water. It appears that the relative hydrophobicity between
polymer and substrate controls the amount of interfacial water. |
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The total film swelling is also observed to be a function of the
initial thickness and interfacial water. For thinner resist films
the interfacial water dominates the swelling as shown in the inset
to Fig. 1 for PBOCSt and PHOSt. For these different resists, the swelling
becomes similar for ultrathin films with thickness less than 200 Å.
The data are consistent with an interfacial water thickness and content
for each film thickness. The interfacial concentration is strongly
dependent upon the surface chemistry, but relatively independent of
the photoresist material or film thickness. |
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Dissolution Effects: Aqueous Base Profile
The development step of a latent image in an aqueous base contributes
significantly to undesirable line-edge roughness (LER). There is a
strong need for improved dissolution models incorporating photoresist-developer
interactions. A key component is the depth profile of the aqueous
base counterion through a photoresist film because it controls the
dissolution mechanisms that lead to unacceptable LER. We provided
the first direct measurement of the aqueous base distribution (tetramethylammonium
hydroxide) (TMAH) within the film. These measurements quantify the
extent of developer penetration and the influence of ionization on
the response of the photoresist to the developer solution.
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We used a zero-average contrast (ZAC) experiment where the neutron
scattering length density of a thin film of poly(norbornene hexafluoroisopropanol)
(PNBHFA), a model 157 nm photoresist, is matched to the developer
solution with a D2O/H2O mixture. As shown in the schematic of Fig.
2, the contrast matched film and solvent (equal color) eliminates
neutron contrast at this interface. However, when base (d12-TMAH)
enters the film, the reflectivity contrast is enhanced. These changes
allow quantification of both film swelling and the base profile through
the film. |
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Figure 2: Schematic of the zero-average neutron reflectivity
experiment. The contrast between the film and solvent are equal, only
the enrichment of deuterated aqueous base within the film provided
the reflectivity enhancement. |
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The volume fraction of d12-TMA+ is plotted versus distance from
the substrate in Fig. 3 for four different equilibrating concentrations
of base. The change in the counterion profile illustrates the advancement
of the swollen solid front. A key finding was that the film expansion
proceeds via base transport throughout the entire film rather than
gradually through the film. In addition, a depletion of base was observed
at the substrate. The film-solution interfacial width increases with
higher base concentration. These measurements show that ionization
induced swelling occurs at the dissolution front. At even higher base
concentrations, the photoresist film dissolves quickly. Understanding
the transition from swelling to rapid dissolution with base concentration
will provide guidance into developer-induced roughness. |
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Figure 3: Volume fraction profiles of d12-TMA+ within
the PNBHFA film. The aqueous base profile illustrates the enhanced
swelling and content within the thin film with higher equilibrating
base concentration. |
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These base profilometry experiments were followed by a deswelling
step by rinsing with pure water. The rinse kinetically traps base
within the film where it could contaminate other processes during
device fabrication. |
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NR measurements provide new information about the liquid-photoresist
interface needed to improve current models of dissolution. In future
work, we will examine the effects of liquid-photoresist interactions
on surface roughness with atomic force microscopy measurements of
surface features. |
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For More Information on this Topic |
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C. Soles, M. Wang, C. Wang, R. Jones, W. Wu, E. Lin (Polymers Division,
NIST); S. Satija (NCNR, NIST); D. Goldfarb, M. Angelopoulos (IBM T.J.
Watson Research Center); H. Ito (IBM Almaden Research Center). |
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"Water immersion of model photoresists: Interfacial influences
on water concentration and surface morphology" B.D. Vogt, et
al., J. Microlithography, Microfabrication, and Microsystems, in press. |
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