pith. sign in

arxiv: 2606.24657 · v1 · pith:M5VNMRE6new · submitted 2026-06-23 · ❄️ cond-mat.soft · cond-mat.mtrl-sci

Limited surface mobility inhibits stable glass formation for 2-ethyl-1-hexanol

Pith reviewed 2026-06-25 21:50 UTC · model grok-4.3

classification ❄️ cond-mat.soft cond-mat.mtrl-sci
keywords vapor depositionstable glassessurface mobilitykinetic stability2-ethyl-1-hexanolorganic glassesglass transition
0
0 comments X

The pith

Limited surface mobility prevents 2-ethyl-1-hexanol from forming highly stable vapor-deposited glasses.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper examines why 2-ethyl-1-hexanol fails to produce highly stable glasses under standard vapor deposition conditions that work for many other organic molecules. Experiments show that lowering the deposition rate from 0.2 nm/s to 0.005 nm/s at a substrate temperature of 0.90 Tg raises the kinetic stability, measured by isothermal transformation times, by three orders of magnitude. Vapor-deposited samples also reach much higher stability than liquid-cooled glasses aged for the same total time. Comparison to ethylcyclohexane, which forms stable glasses readily, leads to the estimate that 2-ethyl-1-hexanol surface mobility is more than four orders of magnitude lower at 0.85 Tg. These findings support the claim that limited surface mobility is what blocks stable glass formation for this molecule.

Core claim

The kinetic stability of 2-ethyl-1-hexanol glasses increases by three orders of magnitude when the deposition rate is lowered at 0.90 Tg, and a vapor-deposited glass is far more stable than an aged liquid-cooled glass prepared in the same time; direct comparison shows the surface mobility of 2-ethyl-1-hexanol is more than four orders of magnitude lower than that of ethylcyclohexane at 0.85 Tg, supporting the hypothesis that limited surface mobility inhibits formation of highly stable glasses.

What carries the argument

Deposition-rate dependence of isothermal transformation times, used to quantify and compare surface mobility against ethylcyclohexane.

Load-bearing premise

That differences in stable glass formation between 2-ethyl-1-hexanol and ethylcyclohexane arise solely from their difference in surface mobility rather than from other molecular-structure or bulk-property distinctions.

What would settle it

A direct measurement of surface diffusion coefficients for both molecules at 0.85 Tg that finds the mobility ratio is not larger than four orders of magnitude.

Figures

Figures reproduced from arXiv: 2606.24657 by C. Schick, M. D. Ediger, M. S. Beasley, M. Tylinski, Y. Z. Chua.

Figure 1
Figure 1. Figure 1: Reversing heat capacity data from 20 Hz AC nanocalorimetry experiments on 2-ethyl-1-hexanol glasses, obtained during heating at 5 K/min. Panel a: Glasses deposited at Tsubstrate = 0.95 Tg. Panel b: Glasses deposited at Tsubstrate = 0.90 Tg. Panel c: Glasses deposited at Tsubstrate = 0.85 Tg. The black dashed lines in panel c demonstrate how the onset temperature (Tonset) for the transformation of the as￾de… view at source ↗
Figure 2
Figure 2. Figure 2: Characteristics of vapor-deposited glasses of 2-ethyl-1-hexanol, as a function of deposition rate, from the temperature ramping experiments shown in [PITH_FULL_IMAGE:figures/full_fig_p008_2.png] view at source ↗
Figure 5
Figure 5. Figure 5: Aging experiments on a liquid-cooled glass of 2-ethyl-1-hexanol. Panel a: Heat capacity decrease during aging at 0.95 Tg. The total aging time is equal to the time required for the longest deposition utilized to prepare the samples in [PITH_FULL_IMAGE:figures/full_fig_p013_5.png] view at source ↗
Figure 7
Figure 7. Figure 7: Relaxation times  and surface for 2-ethyl-1-hexanol and ethylcyclohexane. The surface values are obtained by fitting the data shown in [PITH_FULL_IMAGE:figures/full_fig_p020_7.png] view at source ↗
read the original abstract

Previous work has shown that vapor-deposition can prepare organic glasses with extremely high kinetic stabilities and other properties that would be expected from liquid-cooled glasses only after aging for thousands of years or more. However, recent reports have shown that some molecules form vapor-deposited glasses with only limited kinetic stability when prepared using conditions expected to yield a stable glass. In this work, we vapor deposit glasses of 2-ethyl-1-hexanol over a wide range of deposition rates and test several hypotheses for why this molecule does not form highly stable glasses under normal deposition conditions. The kinetic stability of 2-ethyl-1-hexanol glasses is found to be highly dependent on the deposition rate. For deposition at Tsubstrate = 0.90 Tg, the kinetic stability increases by 3 orders of magnitude (as measured by isothermal transformation times) when the deposition rate is decreased from 0.2 nm/s to 0.005 nm/s. We also find that, for the same preparation time, a vapor-deposited glass has much more kinetic stability than an aged liquid-cooled glass. Our results support the hypothesis that the formation of highly stable 2-ethyl-1-hexanol glasses is inhibited by limited surface mobility. We compare our deposition rate experiments to similar ones performed with ethylcyclohexane (which readily forms glasses of high kinetic stability); we estimate that the surface mobility of 2-ethyl-1-hexanol is more than 4 orders of magnitude less than that of ethylcyclohexane at 0.85 Tg.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. The manuscript reports vapor-deposition experiments on 2-ethyl-1-hexanol, demonstrating that the kinetic stability of the resulting glasses (quantified via isothermal transformation times) increases by three orders of magnitude when the deposition rate is lowered from 0.2 nm/s to 0.005 nm/s at T_substrate = 0.90 T_g. The authors test multiple hypotheses for the limited stability observed under standard conditions and conclude that limited surface mobility is the inhibiting factor. This conclusion rests on a direct comparison to ethylcyclohexane (which forms highly stable glasses), from which they estimate that the surface mobility of 2-ethyl-1-hexanol is more than four orders of magnitude lower at 0.85 T_g. They additionally show that, for equivalent preparation times, vapor-deposited glasses exhibit greater kinetic stability than aged liquid-cooled glasses.

Significance. If the central claim holds, the work identifies surface mobility as a key constraint on stable glass formation for hydrogen-bonding molecules and provides a concrete experimental example where rate-dependent deposition fails to produce high-stability glasses. The clear demonstration of strong rate dependence and the explicit comparison to a contrasting molecule constitute strengths; the manuscript also supplies falsifiable predictions about mobility differences that can be tested with independent diffusion measurements.

major comments (1)
  1. [abstract, final paragraph] Abstract, final paragraph: the claim that surface mobility of 2-ethyl-1-hexanol is >4 orders of magnitude lower than that of ethylcyclohexane at 0.85 T_g is load-bearing for the central hypothesis, yet the comparison does not demonstrate that bulk properties (fragility index, self-diffusion coefficients, or relaxation mechanisms) have been matched or corrected between the hydrogen-bonding alcohol and the non-polar hydrocarbon. Without such controls, differences in the mapping from deposition rate to stability cannot be attributed solely to surface mobility.
minor comments (2)
  1. The abstract states that several hypotheses were tested but does not enumerate them or report the outcome for each; a brief summary in the abstract or a dedicated section would improve clarity.
  2. Error analysis, uncertainties on transformation times, and full data tables for the rate series are not referenced; inclusion of these would strengthen the reported three-order-of-magnitude effect.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful review and for raising this important point about our comparison between 2-ethyl-1-hexanol and ethylcyclohexane. We address the comment below and have revised the manuscript to qualify the surface-mobility estimate and to discuss potential confounding bulk-property differences.

read point-by-point responses
  1. Referee: [abstract, final paragraph] Abstract, final paragraph: the claim that surface mobility of 2-ethyl-1-hexanol is >4 orders of magnitude lower than that of ethylcyclohexane at 0.85 T_g is load-bearing for the central hypothesis, yet the comparison does not demonstrate that bulk properties (fragility index, self-diffusion coefficients, or relaxation mechanisms) have been matched or corrected between the hydrogen-bonding alcohol and the non-polar hydrocarbon. Without such controls, differences in the mapping from deposition rate to stability cannot be attributed solely to surface mobility.

    Authors: We agree that the original manuscript does not demonstrate explicit matching or correction for bulk properties such as fragility index, self-diffusion coefficients, or relaxation mechanisms between the two molecules. The >4-order-of-magnitude estimate is an inference based on the deposition rates needed to reach comparable kinetic stabilities at the same reduced temperature (0.85 Tg). We have revised the abstract and added a dedicated paragraph in the discussion to state this limitation explicitly, to note the known differences in bulk dynamics between hydrogen-bonding and non-polar glass-formers, and to emphasize that independent surface-diffusion measurements would be required for a definitive separation of surface versus bulk contributions. The strong rate dependence observed for 2-ethyl-1-hexanol nevertheless remains the primary experimental evidence supporting limited surface mobility as the inhibiting factor. revision: yes

Circularity Check

0 steps flagged

No circularity; experimental comparison stands on independent measurements

full rationale

The paper reports direct measurements of isothermal transformation times versus deposition rate for 2-ethyl-1-hexanol, then compares those rates to published ethylcyclohexane data to infer a surface-mobility difference. No equation defines surface mobility from the stability result and then re-uses that definition as a prediction; the central claim is an inference from two independent data sets rather than a self-referential fit or self-citation chain. The derivation chain therefore remains self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Experimental study with no mathematical derivations; no free parameters, axioms, or invented entities are introduced.

pith-pipeline@v0.9.1-grok · 5831 in / 1144 out tokens · 30957 ms · 2026-06-25T21:50:32.381990+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

73 extracted references · 70 canonical work pages

  1. [1]

    The third hypothesis, that stable glass formation in 2-ethyl-1-hexanol is inhibited by limited surface mobility, is consistent with our experimental results as we discuss below

    These observations in combination with the reasonably high kinetic stability achieved at the lowest deposition rates allow us to reject the second hypothesis. The third hypothesis, that stable glass formation in 2-ethyl-1-hexanol is inhibited by limited surface mobility, is consistent with our experimental results as we discuss below. For the rest of the ...

  2. [2]

    Yu, Surface mobility of molecular glasses and its importance in physical stability, Adv

    L. Yu, Surface mobility of molecular glasses and its importance in physical stability, Adv. Drug Deliv. Rev. 100 3–9. (2016).; DOI:10.1016/j.addr.2016.01.005

  3. [3]

    M. D. Ediger and J. A. Forrest, Dynamics near Free Surfaces and the Glass Transition in Thin Polymer Films: A View to the Future, Macromolecules 47 471–478. (2014).; DOI:10.1021/ma4017696

  4. [4]

    C. B. Roth and J. R. Dutcher, Glass transition and chain mobility in thin polymer films, J. Electroanal. Chem. 584 13–22. (2005).; DOI:10.1016/j.jelechem.2004.03.003

  5. [5]

    Li and G

    X. Li and G. B. McKenna, Ultrathin Polymer Films: Rubbery Stiffening, Fragility, and Tg Reduction, Macromolecules 48 6329–6336. (2015).; DOI:10.1021/acs.macromol.5b01263

  6. [6]

    E. C. Glor, R. J. Composto and Z. Fakhraai, Glass Transition Dynamics and Fragility of Ultrathin Miscible Polymer Blend Films, Macromolecules 48 6682–6689. (2015).; DOI:10.1021/acs.macromol.5b00979

  7. [7]

    J. L. Keddie, R. A. L. Jones and R. A. Cory, Size-Dependent Depression of the Glass Transition Temperature in Polymer Films, Europhys. Lett. 27 59–64. (1994).; DOI:10.1209/0295- 24 5075/27/1/011

  8. [8]

    Reiter, Mobility of Polymers in Films Thinner than Their Unperturbed Size, Europhys

    G. Reiter, Mobility of Polymers in Films Thinner than Their Unperturbed Size, Europhys. Lett. 23 579–584. (1993).; DOI:10.1209/0295-5075/23/8/007

  9. [9]

    J. A. Forrest, K. Dalnoki-Veress and J. R. Dutcher, Interface and chain confinement effects on the glass transition temperature of thin polymer films, Phys. Rev. E 56 5705–5716. (1997).; DOI:10.1103/PhysRevE.56.5705

  10. [10]

    D. Qi, M. Ilton and J. A. Forrest, Measuring surface and bulk relaxation in glassy polymers, Eur. Phys. J. E 34 56. (2011).; DOI:10.1140/epje/i2011-11056-1

  11. [11]

    C. W. Brian and L. Yu, Surface self-diffusion of organic glasses, J. Phys. Chem. A 117 13303–13309. (2013).; DOI:10.1021/jp404944s

  12. [12]

    Hasebe, D

    M. Hasebe, D. Musumeci and L. Yu, Fast Surface Crystallization of Molecular Glasses: Creation of Depletion Zones by Surface Diffusion and Crystallization Flux, J. Phys. Chem. B 119 3304–3311. (2015).; DOI:10.1021/jp512400c

  13. [13]

    Zhang, C

    W. Zhang, C. Brian and L. Yu, Fast Surface Diffusion of Amorphous ortho-Terphenyl and its Competition with Viscous Flow in Surface Evolution, J. Phys. Chem. B 119 5071–5078. (2015).; DOI:10.1021/jp5127464

  14. [14]

    S. Ruan, W. Zhang, Y. Sun, M. D. Ediger and L. Yu, Surface Diffusion and Surface Crystal Growth of tris-Napthyl Benzene Glasses, J. Chem. Phys. 145 64503. (2016).; DOI:10.1063/1.4960301

  15. [15]

    S. F. Swallen, K. L. Kearns, M. K. Mapes, Y. S. Kim, R. J. McMahon, M. D. Ediger, T. Wu, L. Yu and S. Satija, Organic glasses with exceptional thermodynamic and kinetic stability, Science 315 353–

  16. [16]

    (2007).; DOI:10.1126/science.1135795

  17. [17]

    Ishii and H

    K. Ishii and H. Nakayama, Structural relaxation of vapor-deposited molecular glasses and supercooled liquids., Phys. Chem. Chem. Phys. 16 12073–12092. (2014).; DOI:10.1039/c4cp00458b

  18. [18]

    K. L. Kearns, S. F. Swallen, M. D. Ediger, T. Wu, Y. Sun and L. Yu, Hiking down the energy landscape: progress toward the Kauzmann temperature via vapor deposition, J. Phys. Chem. B 112 4934–4942. (2008).; DOI:10.1021/jp7113384

  19. [19]

    Molecular orientation in small-mol ecule organic light-emitting diodes

    D. Yokoyama, Molecular orientation in small-molecule organic light-emitting diodes, J. Mater. 25 Chem. 21 19187. (2011).; DOI:10.1039/c1jm13417e

  20. [20]

    S. S. Dalal, D. M. Walters, I. Lyubimov, J. J. de Pablo and M. D. Ediger, Tunable molecular orientation and elevated thermal stability of vapor-deposited organic semiconductors, Proc. Natl. Acad. Sci. 112 4227–4232. (2015).; DOI:10.1073/pnas.1421042112

  21. [21]

    Z. Shi, P. G. Debenedetti and F. H. Stillinger, Properties of model atomic free-standing thin films, J. Chem. Phys. 134 114524. (2011).; DOI:10.1063/1.3565480

  22. [22]

    Malshe, M

    R. Malshe, M. D. Ediger, L. Yu and J. J. de Pablo, Evolution of glassy gratings with variable aspect ratios under surface diffusion., J. Chem. Phys. 134 194704. (2011).; DOI:10.1063/1.3573903

  23. [23]

    J. A. Torres, P. F. Nealey and J. J. De Pablo, Molecular Simulation of Ultrathin Polymeric Films near the Glass Transition, Phys. Rev. Lett. 85 3221–3224. (2000).; DOI:10.1103/PhysRevLett.85.3221

  24. [24]

    Shavit and R

    A. Shavit and R. A. Riggleman, Physical Aging, the Local Dynamics of Glass-Forming Polymers under Nanoscale Confinement, J. Phys. Chem. B 118 9096–9103. (2014).; DOI:10.1021/jp502952n

  25. [25]

    P. Z. Hanakata, J. F. Douglas and F. W. Starr, Local variation of fragility and glass transition temperature of ultra-thin supported polymer films, J. Chem. Phys. 137 244901. (2012).; DOI:10.1063/1.4772402

  26. [26]

    Peter, H

    S. Peter, H. Meyer and J. Baschnagel, Thickness-dependent reduction of the glass-transition temperature in thin polymer films with a free surface, J. Polym. Sci. Part B Polym. Phys. 44 2951–

  27. [27]

    (2006).; DOI:10.1002/polb.20924

  28. [28]

    Scheidler, W

    P. Scheidler, W. Kob, K. Binder and G. Parisi, Growing length scales in a supercooled liquid close to an interface, Philos. Mag. Part B 82 283–290. (2002).; DOI:10.1080/13642810208221307

  29. [29]

    Barrat, J

    J.-L. Barrat, J. Baschnagel and A. Lyulin, Molecular dynamics simulations of glassy polymers, Soft Matter 6 3430–3446. (2010).; DOI:10.1039/b927044b

  30. [30]

    J. H. Mangalara, M. D. Marvin and D. S. Simmons, Three-Layer Model for the Emergence of Ultrastable Glasses from the Surfaces of Supercooled Liquids, J. Phys. Chem. B 120 4861–4865. (2016).; DOI:10.1021/acs.jpcb.6b04736

  31. [32]

    Mirigian and K

    S. Mirigian and K. S. Schweizer, Theory of activated glassy relaxation, mobility gradients, surface diffusion, and vitrification in free standing thin films, J. Chem. Phys. 143 244705. (2015).; DOI:10.1063/1.4937953

  32. [34]

    R. P. White, C. C. Price and J. E. G. Lipson, Effect of Interfaces on the Glass Transition of Supported and Freestanding Polymer Thin Films, Macromolecules 48 4132–4141. (2015).; DOI:10.1021/acs.macromol.5b00510

  33. [35]

    Dawson, L

    K. Dawson, L. A. Kopff, L. Zhu, R. J. McMahon, L. Yu, R. Richert and M. D. Ediger, Molecular packing in highly stable glasses of vapor-deposited tris-naphthylbenzene isomers, J. Chem. Phys. 136 94505. (2012).; DOI:10.1063/1.3686801

  34. [36]

    K. R. Whitaker, M. Tylinski, M. Ahrenberg, C. Schick and M. D. Ediger, Kinetic stability and heat capacity of vapor-deposited glasses of o-terphenyl, J. Chem. Phys. 143 84511. (2015).; DOI:10.1063/1.4929511

  35. [37]

    Tylinski, Y

    M. Tylinski, Y. Z. Chua, M. S. Beasley, C. Schick and M. D. Ediger, Vapor-deposited alcohol glasses reveal a wide range of kinetic stability, J. Chem. Phys. 145 174506. (2016).; DOI:10.1063/1.4966582

  36. [38]

    S. S. Dalal, Z. Fakhraai and M. D. Ediger, High-throughput ellipsometric characterization of vapor- deposited indomethacin glasses, J. Phys. Chem. B 117 15415–25. (2013).; DOI:10.1021/jp405005n

  37. [39]

    Nakayama, K

    H. Nakayama, K. Omori, K. Ino-u-e and K. Ishii, Molar volumes of ethylcyclohexane and butyronitrile glasses resulting from vapor deposition: dependence on deposition temperature and comparison to alkylbenzenes., J. Phys. Chem. B 117 10311–9. (2013).; DOI:10.1021/jp404256r

  38. [40]

    T. Liu, K. Cheng, E. Salami-Ranjbaran, F. Gao, C. Li, X. Tong, Y.-C. Lin, Y. Zhang, W. Zhang, L. Klinge, P. J. Walsh and Z. Fakhraai, The effect of chemical structure on the stability of physical vapor deposited glasses of 1,3,5-triarylbenzene, J. Chem. Phys. 143 84506. (2015).; DOI:10.1063/1.4928521

  39. [41]

    Leon-Gutierrez, A

    E. Leon-Gutierrez, A. Sepúlveda, G. Garcia, M. T. Clavaguera-Mora and J. Rodríguez-Viejo, 27 Stability of thin film glasses of toluene and ethylbenzene formed by vapor deposition: an in situ nanocalorimetric study., Phys. Chem. Chem. Phys. 12 14693–14698. (2010).; DOI:10.1039/c0cp00208a

  40. [42]

    S. L. L. M. Ramos, A. K. Chigira and M. Oguni, Devitrification properties of vapor-deposited ethylcyclohexane glasses and interpretation of the molecular mechanism for formation of vapor- deposited glasses, J. Phys. Chem. B 119 4076–4083. (2015).; DOI:10.1021/jp5109174

  41. [44]

    Singh and J

    S. Singh and J. J. de Pablo, A molecular view of vapor deposited glasses, J. Chem. Phys. 134 194903. (2011).; DOI:10.1063/1.3586805

  42. [45]

    Helfferich, I

    J. Helfferich, I. Lyubimov, D. Reid and J. J. de Pablo, Inherent structure energy is a good indicator of molecular mobility in glasses, Soft Matter 12 5898–5904. (2016).; DOI:10.1039/C6SM00810K

  43. [46]

    E. A. Di Marzio and A. J. M. Yang, Configurational Entropy Approach to the Kinetics of Glasses, J. Res. Natl. Inst. Stand. Technol. 102 135–157. (1997).; DOI:10.6028/jres.102.011

  44. [47]

    P. A. O’Connell and G. B. McKenna, Arrhenius-type temperature dependence of the segmental relaxation below Tg, J. Chem. Phys. 110 11054. (1999).; DOI:10.1063/1.479046

  45. [48]

    J. P. Garrahan and D. Chandler, Coarse-grained microscopic model of glass formers., Proc. Natl. Acad. Sci. U. S. A. 100 9710–9714. (2003).; DOI:10.1073/pnas.1233719100

  46. [49]

    J. Zhao, S. L. Simon and G. B. McKenna, Using 20-million-year-old amber to test the super- Arrhenius behaviour of glass-forming systems, Nat. Commun. 4 1783. (2013).; DOI:10.1038/ncomms2809

  47. [50]

    Walters, David Ro dney, M

    I. Lyubimov, L. Antony, D. M. Walters, D. Rodney, M. D. Ediger and J. J. de Pablo, Orientational anisotropy in simulated vapor-deposited molecular glasses, J. Chem. Phys. 143 94502. (2015).; DOI:10.1063/1.4928523

  48. [51]

    Y. Chen, W. Zhang and L. Yu, Hydrogen Bonding Slows Down Surface Diffusion of Molecular Glasses, J. Phys. Chem. B 120 8007–8015. (2016).; DOI:10.1021/acs.jpcb.6b05658

  49. [52]

    Ahrenberg, Y

    M. Ahrenberg, Y. Z. Chua, K. R. Whitaker, H. Huth, M. D. Ediger and C. Schick, In situ investigation 28 of vapor-deposited glasses of toluene and ethylbenzene via alternating current chip- nanocalorimetry, J. Chem. Phys. 138 24501. (2013).; DOI:10.1063/1.4773354

  50. [53]

    Bhattacharya and V

    D. Bhattacharya and V. Sadtchenko, Enthalpy and high temperature relaxation kinetics of stable vapor-deposited glasses of toluene, J. Chem. Phys. 141 94502. (2014).; DOI:10.1063/1.4893716

  51. [58]

    Ahrenberg, E

    M. Ahrenberg, E. Shoifet, K. R. Whitaker, H. Huth, M. D. Ediger and C. Schick, Differential alternating current chip calorimeter for in situ investigation of vapor-deposited thin films, Rev. Sci. Instrum. 83 33902. (2012).; DOI:10.1063/1.3692742

  52. [59]

    Tylinski, A

    M. Tylinski, A. Sepúlveda, D. M. Walters, Y. Z. Chua, C. Schick and M. D. Ediger, Vapor-deposited glasses of methyl-m-toluate: How uniform is stable glass transformation?, J. Chem. Phys. 143 244509. (2015).; DOI:10.1063/1.4938420

  53. [60]

    Sepúlveda, S

    A. Sepúlveda, S. F. Swallen, L. A. Kopff, R. J. McMahon and M. D. Ediger, Stable glasses of indomethacin and α,α,β-tris-naphthylbenzene transform into ordinary supercooled liquids, J. Chem. Phys. 137 204508. (2012).; DOI:10.1063/1.4768168

  54. [61]

    Rodríguez-Tinoco, M

    C. Rodríguez-Tinoco, M. Gonzalez-Silveira, J. Ràfols-Ribé, A. F. Lopeandía, M. T. Clavaguera-Mora and J. Rodríguez-Viejo, Evaluation of growth front velocity in ultrastable glasses of indomethacin over a wide temperature interval, J. Phys. Chem. B 118 10795–10801. (2014).; DOI:10.1021/jp506782d

  55. [62]

    Sepúlveda, S

    A. Sepúlveda, S. F. Swallen and M. D. Ediger, Manipulating the properties of stable organic 29 glasses using kinetic facilitation, J. Chem. Phys. 138 12A517. (2013).; DOI:10.1063/1.4772594

  56. [63]

    R. C. Bell, H. Wang, M. J. Iedema and J. P. Cowin, Nanometer-Resolved Interfacial Fluidity, J. Am. Chem. Soc. 125 5176–5185. (2003).; DOI:10.1021/ja0291437

  57. [64]

    L. Zhu, C. W. Brian, S. F. Swallen, P. T. Straus, M. D. Ediger and L. Yu, Surface Self-Diffusion of an Organic Glass, Phys. Rev. Lett. 106 256103. (2011).; DOI:10.1103/PhysRevLett.106.256103

  58. [65]

    Fragiadakis, C

    D. Fragiadakis, C. M. Roland and R. Casalini, Insights on the origin of the Debye process in monoalcohols from dielectric spectroscopy under extreme pressure conditions, J. Chem. Phys. 132 144505. (2010).; DOI:10.1063/1.3374820

  59. [66]

    Fakhraai and J

    Z. Fakhraai and J. A. Forrest, Probing Slow Dynamics in Supported Thin Polymer Films, Phys. Rev. Lett. 95 25701. (2005).; DOI:10.1103/PhysRevLett.95.025701

  60. [67]

    Zhang, E

    Y. Zhang, E. C. Glor, M. Li, T. Liu, K. Wahid, W. Zhang, R. A. Riggleman and Z. Fakhraai, Long-range correlated dynamics in ultra-thin molecular glass films, J. Chem. Phys. 145 114502. (2016).; DOI:10.1063/1.4962734

  61. [68]

    Paeng, S

    K. Paeng, S. F. Swallen and M. D. Ediger, Direct Measurement of Molecular Motion in Freestanding Polystyrene Thin Films, J. Am. Chem. Soc. 133 8444–8447. (2011).; DOI:10.1021/ja2022834

  62. [69]

    E. C. Glor and Z. Fakhraai, Facilitation of interfacial dynamics in entangled polymer films, J. Chem. Phys. 141 194505. (2014).; DOI:10.1063/1.4901512

  63. [70]

    Berthier , author G

    L. Berthier, G. Biroli, J.-P. Bouchaud, L. Cipelletti, D. El Masri, D. L’Hôte, F. Ladieu and M. Pierno, Direct Experimental Evidence of a Growing Length Scale Accompanying the Glass Transition, Science 310 1797–1800. (2005).; DOI:10.1126/science.1120714

  64. [71]

    Dalle-Ferrier, C

    C. Dalle-Ferrier, C. Thibierge, C. Alba-Simionesco, L. Berthier, G. Biroli, J.-P. Bouchaud, F. Ladieu, D. L’Hôte and G. Tarjus, Spatial correlations in the dynamics of glassforming liquids: Experimental determination of their temperature dependence, Phys. Rev. E 76 41510. (2007).; DOI:10.1103/PhysRevE.76.041510

  65. [72]

    Cavagna, Supercooled liquids for pedestrians, Phys

    A. Cavagna, Supercooled liquids for pedestrians, Phys. Rep. 476 51–124. (2009).; DOI:10.1016/j.physrep.2009.03.003

  66. [73]

    Richert, Supercooled Liquid Dynamics: Advances and Challenges, Struct

    R. Richert, Supercooled Liquid Dynamics: Advances and Challenges, Struct. Glas. Supercooled Liq. 30 1–30. (2012), Hoboken, NJ, USA: John Wiley & Sons, Inc.; DOI:10.1002/9781118202470.ch1 Supplemental Material for: Limited surface mobility inhibits stable glass formation for 2-ethyl-1-hexanol M. TylinskiA, M. S. BeasleyA, Y. Z. ChuaB, C. SchickB, M. D. Edi...

  67. [74]

    Capaccioli, K

    S. Capaccioli, K. L. Ngai, M. Paluch and D. Prevosto, Mechanism of fast surface self-diffusion of an organic glass, Phys. Rev. E 86 51503. (2012).; DOI:10.1103/PhysRevE.86.051503

  68. [75]

    Y. Z. Chua, M. Ahrenberg, M. Tylinski, M. D. Ediger and C. Schick, How much time is needed to form a kinetically stable glass? AC calorimetric study of vapor-deposited glasses of ethylcyclohexane, J. Chem. Phys. 142 54506. (2015).; DOI:10.1063/1.4906806

  69. [76]

    Huth, L.-M

    H. Huth, L.-M. Wang, C. Schick and R. Richert, Comparing calorimetric and dielectric polarization modes in viscous 2-ethyl-1-hexanol, J. Chem. Phys. 126 104503. (2007).; DOI:10.1063/1.2539105

  70. [77]

    Mandanici, W

    A. Mandanici, W. Huang, M. Cutroni and R. Richert, Dynamics of glass-forming liquids. XII. Dielectric study of primary and secondary relaxations in ethylcyclohexane., J. Chem. Phys. 128 124505. (2008).; DOI:10.1063/1.2844797

  71. [78]

    Mandanici, W

    A. Mandanici, W. Huang, M. Cutroni and R. Richert, On the features of the dielectric response of supercooled ethylcyclohexane, Philos. Mag. 88 3961–3971. (2008).; DOI:10.1080/14786430802537753

  72. [79]

    M. R. Carpenter, D. B. Davies and A. J. Matheson, Measurement of the Glass-Transition Temperature of Simple Liquids, J. Chem. Phys. 46 2451. (1967).; DOI:10.1063/1.1841068

  73. [80]

    J. D. Stevenson and P. G. Wolynes, On the surface of glasses, J. Chem. Phys. 129 234514. (2008).; DOI:10.1063/1.3041651