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Rodolfo  Cuerno

    Rodolfo Cuerno

    Low-pressure chemical vapor deposition LPCVD is one of the most frequently used techniques for thin-film production in several industrial applications. 1 Silicon dioxide films have been extensively used in very large scale integrated... more
    Low-pressure chemical vapor deposition LPCVD is one of the most frequently used techniques for thin-film production in several industrial applications. 1 Silicon dioxide films have been extensively used in very large scale integrated devices. Knowledge and eventual control of the morphology of silica films produced by CVD become very important as device dimensions are being continuously reduced. In particular, this control becomes critical when conformal growth ie, good step coverage is required.
    A new model is introduced for two-dimensional crystalline interfaces with negligible surface tension. The model is given by a discrete version of the linear molecular beam epitaxy (MBE) equation plus an additional term periodic in the... more
    A new model is introduced for two-dimensional crystalline interfaces with negligible surface tension. The model is given by a discrete version of the linear molecular beam epitaxy (MBE) equation plus an additional term periodic in the interface height variable. Langevin dynamics simulations and analytical arguments show that the model exhibits a roughening transition to the high temperature phase of the sine-Gordon model, whose initial stages are nevertheless described by the scaling of the linear MBE equation.
    During the last decade, there have been great theoretical and experimental efforts to understand surface growth. This is due to possible applications, eg, to the production of thin films and, from the basic point of view, to the... more
    During the last decade, there have been great theoretical and experimental efforts to understand surface growth. This is due to possible applications, eg, to the production of thin films and, from the basic point of view, to the interesting examples growing surfaces provide of nonequilibrium statistical systems 1, in some cases with strong relation to relevant equilibrium systems 2.
    The dynamics of growing surfaces 1, 2 has attracted great interest during the last decade. This is due both to the practical implications for the control of film quality in thin film production techniques, and to the fundamental questions... more
    The dynamics of growing surfaces 1, 2 has attracted great interest during the last decade. This is due both to the practical implications for the control of film quality in thin film production techniques, and to the fundamental questions it raises in areas of physics such as spatially extended systems in the presence of fluctuations 3, or scale invariance in nonequilibrium systems 4.
    We study the critical behavior of the Laplacian roughening model, which describes the growth of tensionless surfaces. This type of growth phenomena is very important, for instance, in biological membranes and in molecular beam epitaxy. We... more
    We study the critical behavior of the Laplacian roughening model, which describes the growth of tensionless surfaces. This type of growth phenomena is very important, for instance, in biological membranes and in molecular beam epitaxy. We summarize previous analytical and numerical results and point out their contradictions and differences, thus making clear the context of our work.
    A microscopic, driven lattice gas model is proposed for the dynamics and spatiotemporal fluctuations of the precursor film observed in spreading experiments. Matter is transported both by holes and particles, and the distribution of each... more
    A microscopic, driven lattice gas model is proposed for the dynamics and spatiotemporal fluctuations of the precursor film observed in spreading experiments. Matter is transported both by holes and particles, and the distribution of each can be described by driven diffusion with a moving boundary. This picture leads to a stochastic partial differential equation for the shape of the boundary. Explicit analytic results are obtained which agree with the simulations of the lattice gas.
    We report large scale Monte Carlo simulations of the equilibrium discrete Laplacian roughening dLr model, originally introduced as the simplest one accommodating the hexatic phase in two-dimensional melting. The dLr model is also relevant... more
    We report large scale Monte Carlo simulations of the equilibrium discrete Laplacian roughening dLr model, originally introduced as the simplest one accommodating the hexatic phase in two-dimensional melting. The dLr model is also relevant to surface roughening in molecular beam epitaxy MBE. Our data suggest a single phase transition, possibly of the Kosterlitz-Thouless type, between a flat low-temperature phase and a rough, tensionless, high-temperature phase.
    A lack of universality with respect to ion species has been recently established in nanostructuring of semiconductor surfaces by low-energy ion-beam bombardment. This variability affects basic properties of the pattern formation process,... more
    A lack of universality with respect to ion species has been recently established in nanostructuring of
    semiconductor surfaces by low-energy ion-beam bombardment. This variability affects basic properties of the
    pattern formation process, like the critical incidence angle for pattern formation, and has remained unaccounted
    for. Here, we show that nonuniform generation of stress across the damaged amorphous layer induced by
    the irradiation is a key factor behind the range of experimental observations, as the form of the stress field
    is controlled by the ion/target combination. This effect acts in synergy with the nontrivial evolution of the
    amorphous-crystalline interface. We reach these conclusions by contrasting a multiscale theoretical approach,
    which combines molecular dynamics and a continuum viscous flow model, with experiments using Xe + and Ar +
    ions on a Si(100) target. Our general approach can apply to a variety of semiconductor systems and conditions.
    Research Interests:
    We study kinetically rough surfaces which display anomalous scaling in local properties such as the rough- ness or the height-difference correlation function. By studying the power spectrum of the surface and its relation to the... more
    We study kinetically rough surfaces which display anomalous scaling in local properties such as the rough- ness or the height-difference correlation function. By studying the power spectrum of the surface and its relation to the height-difference correlation, we distinguish two independent causes for anomalous scaling. One is superroughening ~global roughness exponent larger than or equal to 1!, even if the
    A microscopic, driven lattice gas model is proposed for the dynamics and spatiotemporal fluctuations of the precursor film observed in spreading experiments. Matter is transported both by holes and particles, and the distribution of each... more
    A microscopic, driven lattice gas model is proposed for the dynamics and spatiotemporal fluctuations of the precursor film observed in spreading experiments. Matter is transported both by holes and particles, and the distribution of each can be described by driven diffusion with a moving boundary. This picture leads to a stochastic partial differential equation for the shape of the boundary.
    We study the dynamics of three-dimensional Fisher fronts in the presence of density fluctuations. To this end we simulate the Fisher equation subject to stochastic internal noise, and study how the front moves and roughens as a function... more
    We study the dynamics of three-dimensional Fisher fronts in the presence of density fluctuations. To this end we simulate the Fisher equation subject to stochastic internal noise, and study how the front moves and roughens as a function of the number of particles in the system, N. Our results suggest that the macroscopic behavior of the system is driven by the microscopic dynamics at its leading edge where number fluctuations are dominated by rare events. Contrary to naive expectations, the strength of front fluctuations decays extremely slowly as 1/logN, inducing large-scale fluctuations which we find belong to the one-dimensional Kardar-Parisi-Zhang universality class of kinetically rough interfaces. Hence, we find that there is no weak-noise regime for Fisher fronts, even for realistic numbers of particles in macroscopic systems.
    We study surface kinetic roughening of TiN films grown on Si100 substrates by dc reactive sputtering. The surface morphology of films deposited for different growth times under the same experimental conditions were analyzed by atomic... more
    We study surface kinetic roughening of TiN films grown on Si100 substrates by dc reactive sputtering. The surface morphology of films deposited for different growth times under the same experimental conditions were analyzed by atomic force microscopy. The TiN films exhibit intrinsic anomalous scaling and multiscaling. The film kinetic roughening is characterized by a set of local exponent values loc=
    A Comment on the Letter by T. C. Kim et al., Phys. Rev. Lett. 92, 246104 (2004). The authors of the Letter offer a Reply. ... (Some reference links may require a separate subscription.) ... T. C. Kim, et al., Phys. Rev. Lett. 92, 246104... more
    A Comment on the Letter by T. C. Kim et al., Phys. Rev. Lett. 92, 246104 (2004). The authors of the Letter offer a Reply. ... (Some reference links may require a separate subscription.) ... T. C. Kim, et al., Phys. Rev. Lett. 92, 246104 (2004). ... R. M. Bradley and J. M. E. Harper, ...
    We consider the Kardar-Parisi-Zhang equation for a circular interface in two dimensions, unconstrained by the standard small-slope and no-overhang approximations. Numerical simulations using an adaptive scheme allow us to elucidate the... more
    We consider the Kardar-Parisi-Zhang equation for a circular interface in two dimensions, unconstrained by the standard small-slope and no-overhang approximations. Numerical simulations using an adaptive scheme allow us to elucidate the complete time evolution as a crossover between a short-time regime with the interface fluctuations of a self-avoiding ring or two-dimensional vesicle, and a long-time regime governed by the Tracy-Widom distribution expected for this geometry. For small-noise amplitudes, scaling behavior is only of the latter type. Large noise is also seen to renormalize the bare physical parameters of the ring, akin to analogous parameter renormalization for equilibrium three-dimensional membranes. Our results bear particular importance on the relation between relevant universality classes of scale-invariant systems in two dimensions.
    ABSTRACT
    Interrupted coarsening (IC) has recently been identified as an important feature for the dynamics of the typical length-scale in pattern-forming systems on surfaces. In practice, it can be beneficial to improve pattern ordering since it... more
    Interrupted coarsening (IC) has recently been identified as an important feature for the dynamics of the typical length-scale in pattern-forming systems on surfaces. In practice, it can be beneficial to improve pattern ordering since it combines a certain degree of defect suppression with a limited increase in the typical pattern wavelength. However, little is known about its robustness with respect to changes in the preparation of the initial system for cases with potential applications. Working in the context of nano-scale pattern formation by ion-beam sputtering (IBS), we prove that IC properties do not depend on sample preparation. Specifically, interface dynamics under IBS is quantitatively compared on virgin amorphous and crystalline silicon surfaces, using 1 keV Ar(+) ions at normal incidence where nanodot pattern formation is triggered by concurrent co-deposition of Fe atoms during processing. Atomic force microscopy shows that dot patterns with similar spatial order and dynamics are obtained in both cases, underscoring the key dynamical role of the amorphous surface layer produced by irradiation. Both systems have been quantitatively described by an effective interface equation. We employ a new procedure based on the linear growth of the initial surface correlations to accurately estimate the equation coefficients. Such a method improves the predictive power of the interface equation with respect to previous studies and leads to a better description of the experimental pattern and its dynamical features.

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