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Volumn 14, Issue 10, 2007, Pages

Instability of current sheets and formation of plasmoid chains

Author keywords

[No Author keywords available]

Indexed keywords

ELECTRIC CURRENTS; GROWTH RATE; PERTURBATION TECHNIQUES; PLASMONS; WAVE EFFECTS;

EID: 36049011695     PISSN: 1070664X     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.2783986     Document Type: Article
Times cited : (750)

References (31)
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    • C. J. Xiao X. G. Wang, Z. Y. Pu, H. Zhao, J. X. Wang, Z. W. Ma, S. Y. Fu, M. G. Kivelson, Z. X. Liu, Q. G. Zong, K. H. Glassmeier, A. Balogh, A. Korth, H. Reme, and C. P. Escoubet, Nat. Phys. 2, 478 (2006).
    • C. J. Xiao X. G. Wang, Z. Y. Pu, H. Zhao, J. X. Wang, Z. W. Ma, S. Y. Fu, M. G. Kivelson, Z. X. Liu, Q. G. Zong, K. H. Glassmeier, A. Balogh, A. Korth, H. Reme, and C. P. Escoubet, Nat. Phys. 2, 478 (2006).
  • 9
    • 0000056210 scopus 로고
    • edited by W. N. Hess NASA, Washington, D.C
    • H. E. Petscheck, in The Physics of Solar Flares, edited by W. N. Hess (NASA, Washington, D.C., 1964), pp. 425.
    • (1964) The Physics of Solar Flares , pp. 425
    • Petscheck, H.E.1
  • 11
    • 0001387019 scopus 로고    scopus 로고
    • DOI: 10.1029/1999JA900449
    • J. Birn et al., J. Geophys. Res. 106, 3715, DOI: 10.1029/1999JA900449 (2001).
    • (2001) J. Geophys. Res , vol.106 , pp. 3715
    • Birn, J.1
  • 14
    • 10644228588 scopus 로고    scopus 로고
    • DOI:10.1029/2004GL020692
    • Q.-G. Zong et al., Geophys. Res. Lett. 31, 18803, DOI:10.1029/2004GL020692 (2004).
    • (2004) Geophys. Res. Lett , vol.31 , pp. 18803
    • Zong, Q.-G.1
  • 31
    • 36048969514 scopus 로고    scopus 로고
    • Going to the next order in our outer solution results in an additional subdominant contribution to Δ′ comparable to the second term in Eq, 15, Note that while the contribution of the second term in Eq, 13 to Δ′ is negligible, the term, itself cannot be dropped because it ensures that the solution has a finite value at Ξ=0. Note also that there exists an unstable solution that is entirely confined inside the current sheet, so that Ψ(±Ξ0, 0. For this solution, C 1±=0 in Eq, 11) and to the lowest order in κ2ε2, Δ′ is given just by the second term in Eq, 15, Solving Eq, 10) to the next order in κ2ε2, we find Δ′(κ)≈ 0.57-1.47κ2ε2. The growth rate then is obtained from. Eq, 18) in the limit Λ≪1. The result is γ/ Γ0 ≈0.61κ2/5
    • 2≈0.08.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.