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PLEEE8
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Aoki, K.M.1
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Göz, M.F.1
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24
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85035226671
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More precisely, the critical point on the neutral curve is the bifurcation point from a homoclinic solution (trajectory to connect one stable point) such as KdV pulses to a heteroclinic solution (trajectory to connect two stable points) such as MKdV kinks.
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More precisely, the critical point on the neutral curve is the bifurcation point from a homoclinic solution (trajectory to connect one stable point) such as KdV pulses to a heteroclinic solution (trajectory to connect two stable points) such as MKdV kinks.
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26
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0000152599
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EK. Nakanishi, K. Itoh, Y. Igarashi, and M. Bando, Phys. Rev.55, 6519 (1997).
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27
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85035215113
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T. S. Komatsu, Ph.D. thesis, Tohoku University, 1996 (unpublished).
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T. S. Komatsu, Ph.D. thesis, Tohoku University, 1996 (unpublished).
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30
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0004261332
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Cambridge University Press, Cambridge
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E. J. Hinch, Perturbation Methods (Cambridge University Press, Cambridge, 1991).
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Perturbation Methods
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Hinch, E.J.1
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36
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85035196993
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In other words, the contribution from the term [formula presented] exists if the system is under the free boundary condition 22
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In other words, the contribution from the term ρ41 exists if the system is under the free boundary condition 22.
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41
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21844507865
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It should be noted that to obtain the exponent -4/3 requires a well-controlled experiment about air flow. Thus, early experiments without controll of the air flow reported slightly larger values of the exponent, e.g., -1.5 rather than -4/3. See, e.g., the earlier papers of, JUPSAU
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It should be noted that to obtain the exponent -4/3 requires a well-controlled experiment about air flow. Thus, early experiments without controll of the air flow reported slightly larger values of the exponent, e.g., -1.5 rather than -4/3. See, e.g., the earlier papers of S. Horikawa, A. Nakahara, T. Nakayama, and M. Matsushita, J. Phys. Soc. Jpn. 64, 1870 (1995);
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J. Phys. Soc. Jpn.
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Horikawa, S.1
Nakahara, A.2
Nakayama, T.3
Matsushita, M.4
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42
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0030395077
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where they have refined the experimental setup and concluded 4/3 in their recent paper 10 PHYADX
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S. Horikawa, T. Isoda, T. Nakayama, A. Nakahara, and M. Matsushita, Physica A 233, 699 (1996), where they have refined the experimental setup and concluded 4/3 in their recent paper 10.
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(1996)
Physica A
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Horikawa, S.1
Isoda, T.2
Nakayama, T.3
Nakahara, A.4
Matsushita, M.5
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