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3
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0001309752
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[English translation: G. P. Ivantsov, in Dynamics of Curved Fronts, edited by P. Pelcé (Academic Press, New York, 1998), pp. 243–246
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G. P. Ivantsov, Dokl. Akad. Nauk SSSR 58, 567 (1947), [English translation: G. P. Ivantsov, in Dynamics of Curved Fronts, edited by P. Pelcé (Academic Press, New York, 1998), pp. 243–246.
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33646950662
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E. Ben-Jacob, P. Garik, T. Mueller, and D. Grier, Phys. Rev. A 38, 1370 (1988)
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Phys. Rev. A
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10
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5544302094
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J. S. Langer, Science 243, 1150 (1989).
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Langer, J.S.1
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12
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0000599539
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Eckler, K.1
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Jurisch, M.5
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14
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21344435863
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E. A. Brener and D. E. Temkin, Zh. Éksp. Teor. Fiz. 109, 1038 (1996) [JETP 82, 559 (1996)]
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JETP
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Brener, E.A.1
Temkin, D.E.2
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16
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5844327614
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E. Ben-Jacob, R. Godbey, N. D. Goldenfeld, J. Koplik, H. Levine, T. Mueller, and L. M. Sander, Phys. Rev. Lett. 55, 1315 (1985)
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Ben-Jacob, E.1
Godbey, R.2
Goldenfeld, N.D.3
Koplik, J.4
Levine, H.5
Mueller, T.6
Sander, L.M.7
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20
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0001483067
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O. Shochet, Klaus Kassner, E. Ben-Jacob, S. G. Lipson, and H. Müller-Krumbhaar, Physica A 181, 136 (1992).
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Shochet, O.1
Kassner, K.2
Ben-Jacob, E.3
Lipson, S.G.4
Müller-Krumbhaar, H.5
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23
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85037210950
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BDH Limited, Broom Road, Poole, BH12 4NN, England. 10 OCB exists in a smectic A phase in the range (Formula presented) Below this range, its equilibrium form is a solid, at higher temperatures, it is an isotropic liquid
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BDH Limited, Broom Road, Poole, BH12 4NN, England. 10 OCB exists in a smectic A phase in the range (Formula presented) Below this range, its equilibrium form is a solid, at higher temperatures, it is an isotropic liquid.
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24
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85037182561
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P. E. Cladis, P. Palffy-Muhoray, Addison-Wesley, Reading, Massachusetts
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John Bechhoefer, in Spatio-Temporal Patterns in Nonequilibrium Complex Systems, Santa Fe Institute: Studies in the Sciences of Complexity, Vol. 21, edited by P. E. Cladis and P. Palffy-Muhoray (Addison-Wesley, Reading, Massachusetts, 1994), pp. 107–122.
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(1994)
John Bechhoefer, in Spatio-Temporal Patterns in Nonequilibrium Complex Systems, Santa Fe Institute: Studies in the Sciences of Complexity, Vol. 21
, pp. 107-122
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-
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25
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85037194836
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ZLI 2510, E. Merck, Darmstadt, Germany
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ZLI 2510, E. Merck, Darmstadt, Germany.
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-
-
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26
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85037236611
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HS1-i Microscope Hot Stage and Temperature Controller, Instec, Inc., Boulder, CO 80306
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HS1-i Microscope Hot Stage and Temperature Controller, Instec, Inc., Boulder, CO 80306.
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-
-
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27
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85037242649
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Olympus BH-2, Olympus Optical Company, Lmt., Tokyo, Japan
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Olympus BH-2, Olympus Optical Company, Lmt., Tokyo, Japan.
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-
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28
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85037206242
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Pulnix TM-7CN, Pulnix America, Inc., Sunnyvale, CA 94086
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Pulnix TM-7CN, Pulnix America, Inc., Sunnyvale, CA 94086.
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-
-
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29
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85037235156
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Scion LG-3, Scion Corporation, Frederick, MD 21701
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Scion LG-3, Scion Corporation, Frederick, MD 21701.
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-
-
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30
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85037250488
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Canon 108mm, (Formula presented) macro lens
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Canon 108mm, (Formula presented) macro lens.
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31
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0003905979
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D. T. J. Hurle, Elsevier, Amsterdam, Chap. 18
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P. J. Phillips, in Handbook of Crystal Growth, Vol. 2, edited by D. T. J. Hurle (Elsevier, Amsterdam, 1993), Chap. 18.
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(1993)
Handbook of Crystal Growth, Vol. 2
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Phillips, P.J.1
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32
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85037230699
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Image processing was performed using NIH Image, v. 1.61, National Institute of Health, Division of Computer Research and Technology, USA
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Image processing was performed using NIH Image, v. 1.61, National Institute of Health, Division of Computer Research and Technology, USA.
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33
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85037213779
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We assume in the following that these modes are governed by thermal, rather than impurity, diffusion. The measured melting range of the smectic A phase (it was difficult to accurately measure the melting range of the multidomain solid phase) is (Formula presented) indicating a low impurity concentration. Moreover, addition of (Formula presented) to the samples produced no change in either growth morphologies or transition temperatures of the solid phase, indicating little sensitivity to the presence of impurities
-
We assume in the following that these modes are governed by thermal, rather than impurity, diffusion. The measured melting range of the smectic A phase (it was difficult to accurately measure the melting range of the multidomain solid phase) is (Formula presented) indicating a low impurity concentration. Moreover, addition of (Formula presented) to the samples produced no change in either growth morphologies or transition temperatures of the solid phase, indicating little sensitivity to the presence of impurities.
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34
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85037223503
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This estimate derives from modeling the flat interface of thickness d as a cylindrical heat source of circumference d moving at velocity (Formula presented) through a uniform infinite medium of thermal diffusivity D. The indicated correction follows for (Formula presented) See J.-C. Geminard, thesis (l’Université Claude Bernard, Lyon, France, 1994) and J. L. Hutter, thesis (Simon Fraser University, Burnaby, Canada, 1997)
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This estimate derives from modeling the flat interface of thickness d as a cylindrical heat source of circumference d moving at velocity (Formula presented) through a uniform infinite medium of thermal diffusivity D. The indicated correction follows for (Formula presented) See J.-C. Geminard, thesis (l’Université Claude Bernard, Lyon, France, 1994) and J. L. Hutter, thesis (Simon Fraser University, Burnaby, Canada, 1997).
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35
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85037244164
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The fractal dimension was measured using a NIH Image macro written by Tom Smith, National Institute of Health, Bethesda, MD
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The fractal dimension was measured using a NIH Image macro written by Tom Smith, National Institute of Health, Bethesda, MD.
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36
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85037241778
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(Formula presented) was identified as a distinct mode after modes (Formula presented) had been defined. We continue to use this label for consistency with earlier publications
-
(Formula presented) was identified as a distinct mode after modes (Formula presented) had been defined. We continue to use this label for consistency with earlier publications.
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37
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85037199490
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This model is a variant of one discussed in Ref. 10 and is discussed in Ref. 14
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This model is a variant of one discussed in Ref. 10 and is discussed in Ref. 14.
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40
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0028336304
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B. Miao, D. O. Northwood, W. Bian, K. Fang, and M. H. Fan, J. Mater. Sci. 29, 255 (1994).
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(1994)
J. Mater. Sci.
, vol.29
, pp. 255
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Miao, B.1
Northwood, D.O.2
Bian, W.3
Fang, K.4
Fan, M.H.5
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42
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85037255111
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C. N. R. Rao and K. J. Rao, Phase Transitions in Solids (McGraw-Hill, London, 1978), pp. 120–133
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C. N. R. Rao and K. J. Rao, Phase Transitions in Solids (McGraw-Hill, London, 1978), pp. 120–133.
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43
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85037220865
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An example of a continuous nucleation transition is the unwinding of a cholesteric helix by a magnetic field that is transverse to the pitch axis. See P. G. de Gennes and J. Prost, The Physics of Liquid Crystals (Clarendon Press, Oxford, 1993), pp. 286–293
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An example of a continuous nucleation transition is the unwinding of a cholesteric helix by a magnetic field that is transverse to the pitch axis. See P. G. de Gennes and J. Prost, The Physics of Liquid Crystals (Clarendon Press, Oxford, 1993), pp. 286–293.
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