Glass films prepared by a process of physical vapour deposition have been shown to have thermodynamic and kinetic stability comparable to those of ordinary glasses aged for thousands of years. A central question in the study of vapour-deposited glasses, particularly in light of new knowledge regarding anisotropy in these materials, is whether the ultra-stable glassy films formed by vapour deposition are ever equivalent to those obtained by liquid cooling. Here we present a computational study of vapour deposition for a two-dimensional glass forming liquid using a methodology, which closely mimics experiment. We find that for the model considered here, structures that arise in vapour-deposited materials are statistically identical to those observed in ordinary glasses, provided the two are compared at the same inherent structure energy. We also find that newly deposited hot molecules produce cascades of hot particles that propagate far into the film, possibly influencing the relaxation of the material.
Glasses represent kinetically arrested states of matter, whose characteristics depend strongly on the process of formation1. They are generally prepared by gradual cooling of a liquid to temperatures below the glass transition, Tg, of the corresponding bulk material. The properties of liquid-cooled, ‘ordinary’ glasses depend on cooling rate and on the ‘age’ of the glass—the amount of time that the material is allowed to rest at a given temperature (below Tg). Lower cooling rates (or ageing) lead to materials that lie deeper in the underlying potential energy landscape. They tend to have a higher density2,3, greater mechanical strength4, lower enthalpy2 and higher onset temperature (the temperature at which the film transforms from a glass into a liquid upon heating)5, than those prepared by fast cooling. Higher stability is desirable in a wide range of applications, from organic electronics6 to drug delivery7.
Recent experimental work has shown that glasses prepared by a process of physical vapour deposition (PVD) can reach levels of stability that are equivalent to those of liquid-cooled glasses allowed to age for thousands of years3,8. These highly stable PVD glasses are formed by depositing the glass former onto a substrate whose temperature is somewhat lower than Tg. It has been proposed that newly deposited molecules can freely explore configurational space near the surface of the growing film9,10, leading to molecular arrangements that correspond to lower free energy states than those accessible by quenching a bulk liquid3.
The properties of three-dimensional (3D) PVD glasses have also been examined in computer simulations. On the one hand, results for a 3D model glass former consisting of a binary mixture of spherical particles indicate that vapour deposition leads to materials that exhibit higher kinetic stability, and whose structure is similar to that of their liquid-cooled counterparts11. On the other hand, simulations of model glasses consisting of anisotropic molecules suggest that a PVD process leads to materials that exhibit varying amounts of anisotropy12. Importantly, past simulations of vapour-deposited glasses have relied on a formation process that involves repeated minimizations of potential energy, which are introduced for computational reasons. As such, past studies have been unable to reveal the role that hot molecules impacting a surface can have on the relaxation of the underlying glassy film. A recent study investigated the formation of highly stable two-dimensional (2D) glasses prepared through a ‘pinning’ technique13. The authors formed equilibrium glasses by freezing in-place a small fraction of the particles in a glass-forming liquid, raising the glass transition temperature above the current temperature, and glassifying the system in an equilibrium configuration. As insightful as the results from the pinning strategy have been, however, such glasses do not incorporate the presence of an interface into the simulations.
Past studies of 2D systems have shed considerable light into the behaviour of glasses. A variety of colloidal particles, including polystyrene and latex, have been shown to assemble into monolayers exhibiting varying degrees of local and long-range order14,15. By virtue of being quasi-2D, such studies allow for the direct observation of glassy dynamics, including structural relaxation near the glass transition, thereby serving as a source of validation for theory and simulations16,17. Atomic 2D glasses have also been prepared, consisting of silica on a graphene substrate18,19. Such systems show a coexistence between crystalline and amorphous regions, which range in size from several unit cells to tens of nanometers across. Going beyond systems of spherical particles, 2D colloidal glasses have been formed using ellipsoids in order resist crystallization20.
In this work, we build upon these past studies by introducing a PVD formation approach that mimics closely that employed in experiments. Specifically, we avoid the artificial energy minimizations and temperature controls that were employed in past computational studies of 3D systems. Furthermore, by restricting our simulations to 2D systems, where configurations can be more easily visualized and inspected, we arrive at unambiguous correlations between local structure and energetic stability. Three important results emerge from our analysis. First, in contrast to previous reports, we find that vapour deposition leads to glasses whose energetic stability far exceeds that of samples prepared by liquid cooling. Second, it is shown that newly deposited particles generate cascades of hot particles that could serve to relax the interior of the film, and that help explain the advantages of PVD processes for preparation of new glasses. Third, we find that the structure of PVD glasses is isotropic and identical to that of liquid-cooled glasses, provided these two classes of materials are compared under preparation conditions for which their inherent structure energies are comparable.
The details of the vapour deposition simulations presented here are discussed in the Methods section. Here we point out that the model considered in this study consists of a binary mixture of spheres whose glass-forming behaviour in the bulk has been examined exhaustively, and that vapour-deposited samples are prepared by depositing groups of hot vapour particles onto a substrate held at a temperature Ts. Particles are deposited until a desired film thickness of ∼35 molecular diameters is reached. Liquid-cooled samples are prepared by heating vapour-deposited films above Tg, and then cooling them at a constant rate to a temperature near zero. A representative system is shown in Fig. 1, where the blue layer at the bottom represents the substrate, the white spheres are of type A, and the black spheres are of type B. Additional sample films are shown in Figs 1 and 2 of Supplementary Information. Vapour-deposited and liquid-cooled films are prepared using a wide range of deposition and cooling rates. The inherent structure energy EIS of a configuration, used to quantify its stability, is the potential energy of a configuration brought to its local energy minimum.
The 2D model considered here exhibits considerable local structure; to quantify this structure, we rely on two bond order parameters that assign values to each particle based on the configuration of its neighbours21. The first, denoted by q5, selects for local pentagonal order. The second, q8, selects for local rectangular order. The background colours in Fig. 1 correspond to the magnitude of such order parameters.
The energetic properties of PVD glasses are determined using only particles in the ‘bulk’ region of the films, which is highlighted in Fig. 2. It corresponds to a wide domain of constant density and composition. Fig. 2 shows results for a variety of PVD and liquid-cooled films. From Fig. 2, we point out two features that arise at the surface of these films: first, the density near the surface decreases gradually. This results from the surface being uneven, as density is simply taken as the number density at a horizontal cross section. Second, χA, the mole fraction of type A, rises near the surface of the films, as shown by previously Shi et al.22. More stable configurations maximize A–B interactions, as is larger than and . Type A particles, which are more abundant at χA=65%, segregate to the surface to maximize these interactions.
The inherent structure energy, EIS, is an effective measure of the position of a glass on the potential energy landscape23. Inherent structure energies of several liquid-cooled and PVD films are shown in panel (a) of Fig. 3. The deposition time for vapour-deposited films, tdep, corresponds to the interval between addition of new groups of particles to the growing film. During this time, newly deposited particles are allowed to cool down and become integrated into the growing film. The cooling time, tcool, is the time over which an ordinary film is cooled from T=5Tg to T=0.2Tg. Cooling and deposition times are expressed in units of the alpha relaxation time of this system, , which is calculated using the self-intermediate scattering function at T=1.10Tg (Supplementary Fig. 3). For all simulations, new, ‘hot’ particles are introduced into the system with an initial temperature of Ti=5.0Tg. The simulated bulk Tg for this material is ∼0.21 in Lennard-Jones units, as determined by taking the fictive temperature of a liquid-cooled film prepared with tcool=1.4 × 103.
Previous experimental work has shown that the optimal substrate temperature, Ts, for the formation of glasses via PVD lies in the vicinity of 0.85Tg (refs 3, 8, 24, 25). For the 2D model system considered here, we find that that the optimal substrate temperature (that leading to the lowest inherent structure energy) for a given deposition time decreases as deposition slows. PVD samples formed with tdep=1.4 × 100 show an optimal Ts of 0.87Tg, while samples formed with tdep=1.4 × 104 show an optimal Ts of 0.68Tg of Tg (Supplementary Table 1). Furthermore, PVD samples prepared at lower deposition rates exhibit significantly lower inherent-structure energies than those prepared at faster rates. As can be appreciated in Fig. 3, depositing with tdep=1.4 × 104 and Ts=0.68Tg gives EIS=−3.965 while tdep=1.4 × 100 and Ts=0.87Tg gives EIS=−3.918. Optimal temperatures are found by fitting a cubic spline to the values of EIS versus Ts in panel (a) Fig. 3 and taking the temperature at the minimum energy value.
We suggest that the ideal deposition temperature decreases with slower deposition rate due to a competition between thermodynamics and kinetics. As the substrate temperature decreases, lower energy states become more thermodynamically favourable, but the kinetics to reach such states become slower. As films are formed through more gradual deposition, atoms are allowed more time to approach equilibrium energy states. As originally proposed by Swallen et al.3, the ideal substrate temperature is where an ideal trade-off is found between which states the system is moving towards (thermodynamics) and how closely the system can approach those states (kinetics).
Panel (b) in Fig. 3 shows EIS of liquid-cooled films evaluated at T=0.25Tg as a function of cooling time (tcool). Previous work on 3D models suggests that EIS varies linearly with log(tcool)11,26. The 2D glass model considered here exhibits a nonlinear dependence. As shown in panel (b) of Fig. 3, a power-law fit of the form:
describes our results reasonably well. Equation 1 can be used to estimate how slowly a liquid should be cooled to form ordinary glass films having inherent structure energies comparable to those of PVD films. These estimated cooling rates are shown by crosses in panel (b) of Fig. 3, for tdep values ranging from 1.4 × 100 to 1.4 × 104, separated by order-of-magnitude intervals. On the basis of this simple extrapolation, one can anticipate the most stable PVD configuration prepared here to be equivalent to a liquid-cooled sample prepared with tcool=1.6 × 1010, which is 1.1 × 105 times longer than the time utilized for the slowest cooling rate that we could accomplish with our computational resources.
As PVD films are formed more slowly, the inherent structure energy apparently approaches that of the deepest minima in the amorphous region of the potential energy landscape. By setting the liquid cooling time equal to infinity in equation 1, one can estimate that these lowest energy states have inherent structure energies of −3.98. By this prediction, the most stable configurations produced here for tdep=1.4 × 104 with Ts=0.67Tg are only 0.013 above this value. We emphasize here that these estimates should be viewed with some skepticism, as the curve shown in the inset of Fig. 3 extends well beyond the data that can be generated with available computational resources. Also note that the more stable vapour-deposited films show a similar, slowing rate of change for inherent structure energy as a function of deposition time, which we believe supports the idea that these films are gradually approaching the bottom of the amorphous regions of the potential energy landscape.
While the overall composition of each film is fixed, the local composition of the bulk region cannot be controlled precisely. On average, type A particles are excluded from the bulk, and the degree of exclusion varies by film formation type and formation time. It has been shown that EIS for 3D Ni80P20 films depends linearly on composition over a small range26. That linear dependence is also observed in our 2D films. To account for the variation in EIS due to composition effects, we perform linear fits of EIS to χA for several cooling times. We find ∂EIS/∂χA=1.6 near χA=0.65 fits well across a wide range of film formation times during both liquid cooling and vapour deposition. The energy of all films is thus interpolated to χA=0.65 for all films, including those used in Fig. 3. The average χA values for PVD and liquid-cooled films in the bulk are 0.648 and 0.637, respectively.
While the aim of this work is to investigate how vapour deposition may influence the structure of glass films, it is worth pointing out that for situations where PVD films and liquid-cooled films exhibit comparable structures, vapour deposition provides an efficient computational method for generating low-energy glasses. For instance, forming a liquid-cooled film with tcool=1.4 × 105 requires 5.0 × 107 time units and 5.0 × 105 s on a particular machine. To form a vapour-deposited film of equal energy, one can deposit with tdep=1.4 × 102 and Ts=0.76Tg, which requires 5.12 × 106 time units and 4.1 × 104 s on the same machine, or approximately one order of magnitude less computational (central processing unit, or CPU) time. Using predicted equivalent cooling rates from Table 1 in the Supplementary Information, we anticipate that this difference becomes greater for more stable, lower-energy films. We estimate that our most stable PVD films, prepared with tdep=1.4 × 104, would require over three orders of magnitude more CPU time if prepared by liquid cooling.
The stability of the PVD films prepared here, based upon two measures, is comparable to that observed in experiment. First, we calculate the fictive temperature, Tf, of several liquid-cooled and PVD films. The fictive temperature is defined as the temperature at which the energy line extrapolated from the glass phase meets the energy line extrapolated from the equilibrium liquid phase, as shown in Fig. 4. In the experiments of Swallen et al.3, the fictive temperature of the glass former 1,3-bis-(1-naphthyl)-5-(2-naphthyl)benzene (Tg=347 K) was measured for three types of films: ordinary liquid-cooled films, aged liquid-cooled films, and PVD films. These authors found the Tf of these films to be 0.99Tg, 0.95Tg, and 0.91Tg, respectively. Later work in which PVD films were formed at slower deposition rates yielded 1,3-bis-(1-naphthyl)-5-(2-naphthyl)benzene films with Tf of 0.88Tg (ref. 27). Following their work, we calculate Tf for three types of films: films formed by liquid-cooling with tcool=1.4 × 101 , films formed by liquid-cooling with tcool=1.4 × 106 (analogous to an aged glass prepared by liquid cooling), and films formed by vapour deposition using our slowest deposition rate, tdep=1.4 × 104 . The results are shown in Fig. 4. We find Tf=1.05Tg, 0.94Tg and 0.89Tg for the three classes of films, respectively. To measure Tf, films were heated at a constant rate of 2 × 10−6 from well below Tg. The ordering and spread of the corresponding fictive temperatures from simulations are consistent with those found in experiment.
Second, we calculate transformation times for both liquid-cooled and PVD films and compare them to experiment. The transformation time is defined as the time required for a material to melt after rapid heating to a temperature above Tg. Ultrastable PVD glasses have been shown to melt through a liquid front that originates at the surface of the film. Growth front velocities for ultrastable indomethacin (IMC) have been measured across a wide range of temperatures above Tg. These velocities have been found to be constant over a wide range of film thicknesses28. We measure film transformation times by rapidly heating films from below Tg to 1.1Tg, and determining the time required for the film to reach an equilibrium energy, as described in the Methods section. The results, normalized by at T=1.1Tg, are shown in Fig. 4 in the Supplementary Information. Energies used to calculate these transformation times are shown in Fig. 5 of the Supplementary Information. The experimental of IMC at T=1.1Tg is 1.3 × 10−4 s, while our 2D system shows a of 1.48 × 10−10 s assuming a Ni-P model. Our most stable PVD films show a transformation time of 158 , and are 8.93 nm thick, using a Ni-P model. Using data from the literature, we calculate that a 8.93 nm thick film of IMC would melt over 354 , where is measured at 1.1Tg for IMC28. By this comparison, our PVD films are just over half as stable as would be expected experimentally for films of this thickness. Note, however, that this comparison is highly speculative, given that both the materials and dimensionality of these two types of films are different. We suggest that the lower stability observed in simulations relative to experiment is expected, given that our slowest film growth rate (using a Ni-P model) is 48 μm per second. Experimental growth rates are typically a few nanometers per second, that is, several orders of magnitude slower. Additional details on the conversion to real units and film growth rates are given in the Methods.
Comparison with 3D films
Vapour deposition in two dimensions is more efficient than in three dimensions. Two-dimensional films exhibit surface regions which show higher mobility than 3D films assembled using comparable models. This trait allows 2D materials to explore configuration space more effectively, which we suggest leads to the lower inherent structure energy seen in 2D. To compare 2D and 3D films formed by PVD, we examine 3D films with the same interaction parameters as in 2D, but with χA=0.80, as in previous work11,26. We define the efficiency of vapour deposition as the ratio of a PVD film’s growth rate to the film’s equivalent liquid cooling rate. In 2D, equivalent tcool values are found using the power law shown in equation 1. In 3D, EIS is linearly fit to log(tcool) for accessible cooling rates. By combining results from 3D films generated using constant N, V and E deposition (Supplementary Fig. 6) with the 2D data presented here, we estimate that vapour deposition in 2D is between 6 × 101 and 6 × 102 times more efficient than in 3D for the films with the lowest inherent structure energies.
Molecules near the surface of a glassy film are more mobile than those in the bulk29. Highly mobile molecules can explore configurations more rapidly, thereby allowing films prepared by vapour deposition to reach lower energies than those without mobile surface regions. Consistent with this understanding of surface mobility and our estimated efficiencies, we find that molecules near the surface of 2D films are both more mobile and encompass a thicker region than in 3D. To quantify these observations, we calculate 〈Δr2〉 of 2D and 3D films for a range of temperatures and film stabilities. For 2D and 3D samples held at T=0.75Tg, we find that molecules in the surface region are, on average, 70% more mobile than those in the bulk. The high-mobility region extends nearly twice as far into the film than in 3D, as shown in Fig. 5. Surface mobilities do not depend strongly on film stability (Supplementary Fig. 7), though mobilities do depend on film temperature (Supplementary Fig. 8) and particle type (Supplementary Figs 9 and 10). Mechanistically, we suggest that the thicker and more mobile surface layer in 2D allows atoms to sample more configurations before being frozen into their glassy states, thereby enabling exploration of lower energy basins along the free energy landscape.
Heat transfer through films
As hot vapour particles impact the surface of growing films, energy is transferred from the vapour into the film. In this material, heat transfers along tightly coupled strings of particles. Correlated strings of particles in glasses have been reported before30. Note, however, that the strings discussed here are inherently different as they correspond to events initiated by newly deposited hot surface particles that introduce a disturbance. Several representative configurations of long strings are shown in Fig. 6. Particles in these thin strings reach kinetic energies near that of the vapour particle at impact. While 75% of these strings penetrate <4 atom diameters into the film, occasionally, such strings can be significantly longer. In 3% of the cases, strings penetrate over seven atom diameters into the film, thereby providing a highly focused energy transfer process down to a relatively large depth.
Heat transferred along strings enters the film much more rapidly than would be expected from a diffusive mechanism. To illustrate the difference, one can rely on a simple one-dimensional continuum model where heat only transfers by diffusion. The continuum model’s surface is initialized at a high temperature, such that the total amount of heat added to the continuum and molecular dynamics models are the same. Parameters for the continuum model, such as heat capacity and thermal diffusivity, are determined from molecular dynamics simulations as described in the Methods section. One can then generate temperature profiles with respect to distance from the film’s surface of these two models as they evolve in time. Figure 7 shows the temperature profile of the PVD films shown in Fig. 6 as compared with the continuum model at 1.1 × 10−2 after impact or initialization. If one looks at heat transfer averaged over many films, the continuum results are recovered (Supplementary Fig. 11). However, in the case of long strings, heat transfer is much faster and energy is much more localized than in the continuum case, as shown in Fig. 7.
The 2D films considered here exhibit considerable local pentagonal and rectangular order. Figs 1 and 10 show representative configurations of the system. The q5 and q8 order parameters (which select for local pentagonal and rectangular order, respectively), are used here to analyse the structure of the films21. Additional details on the order parameters’ selectivity for different geometries are given in Figs 12–14 of the Supplementary Information. The ql order parameter, which is calculated for each particle based on the arrangement of its neighbours, is defined in equation 2, where a is a particle, N is the set of a’s neighbours, and Ylm is the spherical harmonic for the specified l and m:
High q5 pentagons tend to form mostly as five white type A particles surrounding a single black type B particle. For this reason, q5 is calculated only for type B particles. The q8 parameter is calculated for all atoms. The nearest four neighbours of atoms in high q8 rectangular structures tend to be of different type, thereby maximizing the A–B interaction. Figure 1 shows a contour map of and values calculated for a liquid-cooled film with a cooling time of tcool=1.4 × 101. Here denotes a time averaged ql parameter averages over in-cage vibrations, as defined in equation 5 in Methods. It can be seen that high-q8 clusters are of medium size, while locally ordered q5 clusters, which cannot tessellate, appear to be pentagonal. A similar coexistence of medium-range ordered clusters and locally ordered structures was reported in a simulated atomic glass system in which particles’ anisotropy frustrated crystallization31.
To assess the extent of order in these films, particle groups are classified as highly ordered or not using a simple cutoff scheme described in Methods. High-order cutoff values are chosen to be ϕ5=0.55 and ϕ8=22.0, or 78 and 34% of their values relative to perfectly pentagonal or square configurations (which yield the maximum values for these order parameters). All results can be reproduced using different cutoffs as shown in Figs 15–20 of Supplementary Information.
We define the degree of order, Dl, as the fraction of particles involved in high-l ordered groups. We plot the Dl for all PVD and liquid-cooled films in Fig. 8. We find that as the films become more stable, the q8 character decreases, while the q5 character increases. This can be appreciated by visually comparing Figs 3, 4, 5, 6, 7, 8, and by comparing the relatively unstable film in Fig. 1 to the relatively stable films in Fig. 10. Given the direct relationship between these parameters and EIS, we conclude that the structure and stability of these films are well captured by the q5 and q8 parameters.
Figure 9 shows the degree of q5 and q8 order versus EIS for all liquid-cooled and PVD films. Only data from films well in the glassy state, T<0.2, are included. The q5 and q8 trends with temperature are similar and independent of the process of formation. These results can in fact be used to estimate inherent structure energy from degree of order since both D5 and D8 behave monotonically with EIS. The degree of q8 order for PVD films on average lies slightly below that of liquid-cooled films. We attribute this slight difference to the differences in composition between PVD and liquid-cooled films: on average, their bulk compositions are =0.648, 0.637, respectively.
Note, however, that more subtle differences could in principle exist between PVD and liquid-cooled samples. Figure 10 compares vapour-deposited and liquid samples with EIS≈−3.95. The contour map shows no systematic differences in high-order cluster size, location or shape. We find that the size of high-order clusters dependly only on EIS as well, not formation method (Supplementary Fig. 21). Radial distribution functions and structure factors are also calculated for liquid-cooled and PVD films of equal energy, and we find no systemic differences between the two (Supplementary Figs 22–29). Comparing the film in Fig. 1 to the more stable films in Fig. 10, one can appreciate the increase in q5 and the corresponding decrease in q8 character that comes with increasing stability.
To conclude, a new method was introduced to prepare glasses in silico through a process of vapour deposition. The method was applied to investigate a model 2D glass forming liquid. After comparing the structure and energy of the resulting materials to that of ordinary liquid-cooled glassy films, it was found that in-silico PVD greatly expands the range of film properties and structures that can be accessed as compared with traditional liquid cooling. In the 2D materials studied here, the range of structures includes pentagonal clusters and square-grid ordered regions of varying size. Under appropriate conditions, forming films by PVD creates extremely low energy films, equivalent to liquid-cooled films cooled five orders of magnitude slower than possible on available computers. By varying the rate of vapour deposition, it is found that the ideal substrate temperature decreases with slowing deposition rate. In 2D, the surface layer of glassy films is thicker than it is in 3D, leading to a more effective PVD formation mechanism. Upon impacting a growing PVD film, newly deposited molecules form strings of hot particles that can reach well into the interior of the film, possibly providing an additional relaxation mechanism that helps the system explore its energy free landscape. An analysis using bond order parameters that select for square and pentagonal order revealed that films transition from a high square-grid character structure to a locally ordered pentagonal structure as films stabilize. By examining the change in D5 and D8 in films formed using both methods, it was possible to establish that the degree of order does not depend on the formation type. More generally, the results presented in this work serve to demonstrate that, for the simple, isotropic model considered here, the glassy materials prepared by PVD are the same as those prepared by gradual cooling from the liquid phase, and that PVD glasses correspond to liquid-cooled glasses prepared at extremely slow cooling rates.
The films in this work consist of a binary mixture of Lennard-Jones particles with a third particle type acting as the substrate. The interaction potential is given by equation 4, where r is the distance between two particles, rc is the distance beyond which interactions are not considered, and and σ change the strength and range of the interactions.
These simulations use the values rc=2.5, =1.0, =1.5, =0.5, σAA=1.0, σAB=0.8, σBB=0.88. Values of and σ for the A and B particles acting on the substrate are 1.0 and 0.75, respectively. The masses of all particles are set to 1.0. The simulation box uses periodic boundary conditions in the x dimension and finite in y. The x dimension is parallel to the substrate while the y dimension is perpendicular. The simulations box is 30σAA wide and the height is set so that the boundary is 10σAA above the surface of the film as it grows. A timestep of Δt=0.005 is used for all simulations. A Nosé-Hoover thermostat is used to maintain the temperature of all canonical (constant N, V, and T) ensembles32.
Inherent structural energies were calculated by minimizing configurations using the FIRE algorithm with energy and force tolerances of 1 × 10−10 (ref. 33). All simulations were performed using LAMMPS34 and all figures were generated using Matplotlib35.
Formation of PVD Films
Vapour-deposited films are formed by initializing a substrate, then adding groups of atoms to the simulation box and allowing them to settle and cool on the growing film. The substrate is formed such that it does not impose any strong ordering the on film. First, substrate particles are randomly placed in a small rectangular area near the bottom of the simulation box. The rectangle spans the width of the box and is 3σAA tall. The atoms are tethered to their original positions using harmonic springs with a spring constant k=5. The substrate is then minimized using the FIRE algorithm. The substrate atoms are then re-tethered to their minimized positions using harmonic springs with k=1,000. The initial weak spring ensures that the substrate thickness stays roughly constant during the minimization. Throughout the simulation the temperature of the substrate is held constant using a Nosé-Hoover thermostat in an NVT ensemble as described above. A wall with a harmonic repulsive potential is placed 10σAA above the substrate. The wall is moved as the film grows to keep the distance between the film and the wall constant.
The film is grown using the following method: ten particles are initialized in a region 3–5σAA above the growing film. The particle types are chosen to keep the film configuration as close to χa=0.65 as possible. The particles are initialized with random velocities at T=1.0, as in previous work11,26. The new particles and the growing film are then simulated as an NVE ensemble for tdep. The new particles cool by natural heat transfer through the growing film to the substrate. This process is repeated until the films have a height of ∼35σAA. Our method differs from previous work, where the film and vapour atoms are explicitly thermostatted. We find that this method produces lower energies than that employed in previous work (Supplementary Fig. 30) and that film temperature is well thermostatted by the substate (Supplementary Fig. 31).
In all but films formed with tdep=1.4 × 100, the film temperature was tightly distributed around Ts. Film temperatures for those formed with tdep=1.4 × 100 were deposited quickly enough that Tfilm was roughly 0.1Tg higher than Ts. In these cases, the actual temperature of the film was used in data.
Formation of liquid cooled films
Liquid-cooled films are generated by heating vapour-deposited films to T=1.0, then recooling linearly over the time tcool. The wall and substrate spring parameters are not changed during this process. To ensure the independence of each liquid-cooled film, the heated configurations are equilibrated for a random time ranging from 100 to 10,000 time units while at T=1.0. The films are cooled to T=0.05, at which point the inherent structural energy has essentially stopped decreasing.
Transformation time measurements
Transformation times are measured by heating a film to T=1.1Tg over 100 time units, then setting the thermostat to T=1.1Tg and measuring the potential energy of the film as it melts. When a film’s potential energy is 90% of the way from its initial energy to its final energy, it is said to be transformed. We find that if the films are instantaneously heated from very low temperatures (T=0.25Tg) to above Tg, the films expand extremely quickly, push off the static substrate, effectively ‘jump’. For this reason, we introduce the initial heating step.
Thermal conductivity measurements
Parameters for the one-dimensional continuum heat transfer were taken from molecular dynamics simulations. In the model, the equation cv=q=κ∇T is iterated, where T is temperature, t is time, cv is heat capacity, and κ is thermal conductivity. cv is determined by heating the systems around in the temperature of interest, and measuring the energy required. Thermal diffusivity is measured using the Green–Kubo relation which relates the auto-correlation of heat flux to thermal diffusivity.
We assess the order of the systems using a simple high-order cutoff. High-order cutoff values are chosen to be ϕ5=0.55 and ϕ8=22.0, or 78 and 34% of their values relative to perfectly pentagonal or square configurations. These cutoff values are chosen in order to discriminate between ordered and non-ordered configurations. Note, however, that the conclusions can be reproduced using other cutoffs (Supplementary Figs 15–20). To create an order metric independent of in-cage vibrations, we average the order parameter ql defined in equation 5 over Here is taken to be 10 Lennard-Jones time units from the time at which the the self intermediate scattering function at T=0.8Tg has decayed to its in-cage plateau (Supplementary Fig. 32). This means that we are time averaging over the positions sampled within each atom’s glassy cage.
Particles are then classified as transiently high-order if the parameter is above the cutoff value as shown in equation 6.
Finally, we label the particle as high-order if more than half of the transient high-order values in the averaging window of are 1. Since the q8 metric is intended to select for larger-scale crystallinity, we mark high q8 particles that appear in small clusters and thin strands as not highly ordered.
When selecting highly ordered q8 clusters, two techniques are used to refine groupings. First, any cluster that is of five or fewer atoms is ignored. Second, we note that multiple q8 clusters are occasionally connected by single-atom-wide chains of q8-ordered atoms. For the purposes of counting cluster size, we would like to separate these clusters, as they are structurally distinct (but still connected). To do this, we remove particles from q8 clusters using the following method: First, we count how many of a given atom’s neighbours (within a radius of 1.2) are in a q8 ordered group. Then we look at those ordered neighbour particles and perform the same count. If the sum of all of these ordered neighbours is <5, we remove the particle from its ordered group, as the atom is likely part of some thin protrusion or connection. A neighbour cutoff of 1.2 was used for equation 3. This value represents the first minimum in the radial distribution function and gave good contrast for bond order parameter values.
Conversion to real units
In order to facilitate comparison to experiment, the Lennard-Jones units used in this work are converted to real units. We cast type A particles into nickel and type B particles into phosphorus. The simulated atom of nickel (type A) has mass and Lennard-Jones parameters of unity; to convert into real units, one only needs the energy, length, and mass by which those parameters were normalized. Dimensional analysis shows that the time unit in simulation is given by , with Lennard-Jones parameters for nickel as =5.65 kcal mol−1=23,640 J mol−1, σ=2.552 × 10−10 m, and the mass is 58.69 × 10−3 kg mol−1 (ref. 36). Dividing the and mass by Avogadro’s number, we find that the real time unit is 4.021 × 10−13 s. Our longest PVD simulations lasted 9.2 × 1010 simulation timesteps with dt=0.005 Lennard-Jones time units, which translates into a real time of 1.85 × 10−4 s. Films are roughly 35σ, or 8.93 × 10−9 meters thick, giving a growth rate of 48 μm per second.
Data and analysis code are available from the authors upon request.
How to cite this article: Reid, D.R. et al. Age and structure of a model vapour-deposited glass. Nat. Commun. 7, 13062 doi: 10.1038/ncomms13062 (2016).
Angell, C. A. Formation of glasses from liquids and biopolymers. Science 267, 1924–1935 (1995).
Simon, S. L., Sobieski, J. W. & Plazek, D. J. Volume and enthalpy recovery of polystyrene. Polymer 42, 2555–2567 (2001).
Swallen, S. F. et al. Organic glasses with exceptional thermodynamic and kinetic stability. Science 315, 353–356 (2007).
Olsen, N. B., Dyre, J. C. & Christensen, T. Structural relaxation monitored by instantaneous shear modulus. Phys. Rev. Lett. 81, 1031 (1998).
Wang, J. Q., Shen, Y., Perepezko, J. H. & Ediger, M. D. Increasing the kinetic stability of bulk metallic glasses. Acta Mater 103, 25–32 (2016).
Zallen, R. The Physics of Amorphous Solids. (Wiley, New York, 1983).
Yu, L. Amorphous pharmaceutical solids: preparation, characterization and stabilization. Adv. Drug Deliv. Rev. 48, 27–42 (2001).
Kearns, K. L., Swallen, S. F., Ediger, M. D., Wu, T. & Yu, L. Influence of substrate temperature on the stability of glasses prepared by vapor deposition. J. Chem. Phys. 127, 154702 (2007).
Yang, Z., Fujii, Y., Lee, F. K., Lam, C. H. & Tsui, O. K. C. Glass transition dynamics and surface layer mobility in unentangled polystyrene films. Science 328, 1676–1679 (2010).
Zhu, L. et al. Surface self-diffusion of an organic glass. Phys. Rev. Lett. 328, 256103 (2011).
Singh, S., Ediger, M. D. & de Pablo, J. J. Ultrastable glasses from in silico vapour deposition. Nat Mater. 12, 139–144 (2013).
Dalal, S. S., Walters, D. M., Lyubimov, I., de Pablo, J. J. & Ediger, M. D. Tunable molecular orientation and elevated thermal stability of vapor-deposited organic semiconductors. Proc. Natl Acad. Sci. USA 112, 4227–4232 (2015).
Hocky, G. M., Berthier, L. & Reichman, D. R. Equilibrium ultrastable glasses produced by random pinning. J. Chem. Phys. 141, 224503 (2014).
Pieranski, P. Two-dimensional interfacial colloidal crystals. Phys. Rev. Lett. 45, 569 (1980).
Denkov, N. et al. Mechanism of formation of two-dimensional crystals from latex particles on substrates. Langmuir 8, 3183–3190 (1992).
Weeks, E., Crocker, J. C., Levitt, A., Schofield, A. & Weitz, D. A. Three-dimensional direct imaging of structural relaxation near the colloidal glass transition. Science 287, 627–631 (2000).
Ebert, F., Keim, P. & Maret, G. Local crystalline order in a 2D colloidal glass former. Eur. Phys. J E Soft Matter 26, 161–168 (2008).
Lichtenstein, L. et al. The atomic structure of a metal-supported vitreous thin silica film. Angew. Chem. Int. Ed. 51, 404–407 (2012).
Huang, P. Y. et al. Direct imaging of a two-dimensional silica glass on graphene. Nano Lett. 26, 1081–1086 (2012).
Zheng, Z., Wang, F. & Han, Y. Glass transitions in quasi-two-dimensional suspensions of colloidal ellipsoids. Phys. Rev. Lett. 107, 065702 (2011).
Steinhardt, P. J., Nelson, D. R. & Ronchetti, M. Bond-orientational order in liquids and glasses. Phys. Rev. B. 28, 784 (1983).
Shi, Z., Debenedetti, P. G. & Stillinger, F. H. Properties of model atomic free-standing thin films. J. Chem. Phys. 134, 114524 (2011).
Debenedetti, P. G. & Stillinger, F. H. Supercooled liquids and the glass transition. Nature 410, 259–267 (2001).
Kearns, K. L., Swallen, S. F. & Ediger, M. D. Hiking down the energy landscape: progress toward the kauzmann temperature via vapor deposition. J. Phys. Chem. B 112, 4934–4942 (2008).
Yu, H.-B., Luo, Y. & Samwer, K. Ultrastable metallic glass. Adv. Mater. 25, 5904–5908 (2013).
Lyubimov, I., Ediger, M. D. & de Pablo, J. J. Model vapor-deposited glasses: growth front and composition effects. J. Chem. Phys. 139, 144505 (2013).
Dawson, K. et al. Highly stable vapor-deposited glasses of four tris-naphthylbenzene isomers. J. Phys. Chem. Lett. 2, 2683–2687 (2011).
Rodríguez-Tinoco, C. et al. Evaluation of growth front velocity in ultrastable glasses of indomethacin over a wide temperature interval. J. Phys. Chem. B 118, 10795–10801 (2014).
Brian, C. W. & Yu, L. Surface self-diffusion of organic glasses. J. Phys. Chem. A 117, 13303–13309 (2013).
Donati, C. et al. Stringlike cooperative motion in a supercooled liquid. Phys. Rev. Lett. 80, 2338 (1998).
Shintani, H. & Tanaka, H. Frustration on the way to crystallization in glass. Nat. Phys. 2, 200–206 (2006).
Martyna, G. J., Klein, M. L. & Tuckerman, M. Nosé-hoover chains: the canonical ensemble via continuous dynamics. J. Chem. Phys. 97, 2635–2643 (1992).
Bitzek, E., Koskinen, P., Gähler, F., Moseler, M. & Gumbsch, P. Structural relaxation made simple. Phys. Rev. Lett. 97, 170201 (2006).
Plimpton, S. Fast parallel algorithms for short-range molecular dynamics. J. Comput. Phys. 117, 1–19 (1995).
Hunter, J. D. Matplotlib: a 2d graphics environment. Comput. Sci. Eng. 9, 90–95 (2007).
Heinz, H., Vaia, R. A., Farmer, B. L. & Naik, R. R. Accurate simulation of surfaces and interfaces of face-centered cubic metals using 12- 6 and 9- 6 Lennard-Jones potentials. J. Phys. Chem. C 112, 17281–17290 (2008).
We would like to thank David Rodney for many useful conversations. This work was supported by a DMREF grant NSF-DMR-1234320. Fast GPU-accelerated codes for simulation of glassy materials were developed with support from DOE, Basic Energy Sciences, Materials Research Division, under MICCoM (Midwest Integrated Center for Computational Materials).
The authors declare no competing financial interests.
About this article
Cite this article
Reid, D., Lyubimov, I., Ediger, M. et al. Age and structure of a model vapour-deposited glass. Nat Commun 7, 13062 (2016). https://doi.org/10.1038/ncomms13062
This article is cited by
La Rivista del Nuovo Cimento (2022)
npj Computational Materials (2021)
Communications Materials (2021)
npj Computational Materials (2019)
Nature Communications (2018)