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note
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A steepest descent analysis reveals that 1/β increases with C. Note that for C < O a power law is obtained.
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With the advent of metallic melts, sufficiently resistant to crystallization in the undercooled regime, see e.g. A. Inoue, T. Zhang and T. Masumoto, J. Non-Cryst. Solids 156, 473 (1993); A. Peker and W. L. Johnson, Appl. Phys. Lett. 63, 2342 (1993); G. Wilde, G. P. Görler, R. Willnecker, and G. Dietz, Appl. Phys. Lett. 65, 397 (1994), it appears possible that some of these hard sphere materials will turn out to be even more fragile than TPP.
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0342961160
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With the advent of metallic melts, sufficiently resistant to crystallization in the undercooled regime, see e.g. A. Inoue, T. Zhang and T. Masumoto, J. Non-Cryst. Solids 156, 473 (1993); A. Peker and W. L. Johnson, Appl. Phys. Lett. 63, 2342 (1993); G. Wilde, G. P. Görler, R. Willnecker, and G. Dietz, Appl. Phys. Lett. 65, 397 (1994), it appears possible that some of these hard sphere materials will turn out to be even more fragile than TPP.
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Peker, A.1
Johnson, W.L.2
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0000476558
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With the advent of metallic melts, sufficiently resistant to crystallization in the undercooled regime, see e.g. A. Inoue, T. Zhang and T. Masumoto, J. Non-Cryst. Solids 156, 473 (1993); A. Peker and W. L. Johnson, Appl. Phys. Lett. 63, 2342 (1993); G. Wilde, G. P. Görler, R. Willnecker, and G. Dietz, Appl. Phys. Lett. 65, 397 (1994), it appears possible that some of these hard sphere materials will turn out to be even more fragile than TPP.
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Wilde, G.1
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