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Volumn 61, Issue 10, 2000, Pages

Creation and evolution of magnetic helicity

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EID: 17144409114     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.61.105015     Document Type: Article
Times cited : (69)

References (24)
  • 4
    • 0004287813 scopus 로고
    • Cambridge University Press, Cambridge, UK
    • For background, see D. Biskamp, Nonlinear Magnetohydrodynamics (Cambridge University Press, Cambridge, UK, 1993).
    • (1993) Nonlinear Magnetohydrodynamics
    • Biskamp, D.1
  • 15
    • 0347486071 scopus 로고    scopus 로고
    • There are physically interesting situations where this term survives; see R. Jackiw and S.-Y. Pi, Phys. Lett. B 423, 364 (1998)
    • (1998) Phys. Lett. B , vol.423 , pp. 364
    • Jackiw, R.1    Pi, S.-Y.2
  • 17
    • 0004012649 scopus 로고
    • Princeton University Press, Princeton, N.J., S. Treiman, R. Jackiw, B. Zumino, E. Witten
    • R. Jackiw, in Current Algebra and Anomalies, edited by S. Treiman, R. Jackiw, B. Zumino, and E. Witten (Princeton University Press, Princeton, N.J., 1985).
    • (1985) Current Algebra and Anomalies
    • Jackiw, R.1
  • 19
  • 20
    • 85037223156 scopus 로고    scopus 로고
    • The response to more general gauge transformations is as follows. Choosing the gauge function (Formula presented) [so that the form (2.23) is preserved] (Formula presented) change into (Formula presented) (Formula presented). Consequently the winding number becomes (Formula presented) Configurations with integer winding remain gauge invariant [provided (Formula presented) does not increase too rapidly at infinity]. For all other configurations, (Formula presented) must vanish at infinity to maintain gauge invariance of H. Moreover, the gauge function (Formula presented) is “well defined” at infinity only for vanishing (Formula presented). (We thank A. Polychronakos for discussion.)
    • The response to more general gauge transformations is as follows. Choosing the gauge function (Formula presented) [so that the form (2.23) is preserved] (Formula presented) change into (Formula presented) (Formula presented). Consequently the winding number becomes (Formula presented) Configurations with integer winding remain gauge invariant [provided (Formula presented) does not increase too rapidly at infinity]. For all other configurations, (Formula presented) must vanish at infinity to maintain gauge invariance of H. Moreover, the gauge function (Formula presented) is “well defined” at infinity only for vanishing (Formula presented). (We thank A. Polychronakos for discussion.)
  • 21
    • 85037199692 scopus 로고    scopus 로고
    • Equation (2.28) was integrated numerically by Y. Bergner
    • Equation (2.28) was integrated numerically by Y. Bergner.
  • 22
    • 17044439056 scopus 로고    scopus 로고
    • This magnetic field with integer winding number has also been constructed by C. Adam, B. Muratori, and C. Nash, Phys. Rev. D 60, 125001 (1999)
    • (1999) Phys. Rev. D , vol.60 , pp. 125001
    • Adam, C.1    Muratori, B.2    Nash, C.3
  • 24
    • 17044390796 scopus 로고    scopus 로고
    • Phys. Rev. DHalf-integer winding numbers are studied also in Adam et al. in the work cited as well as in K. Haller, L. Chen, and Y. S. Choi, 60, 125010 (1999).
    • (1999) Phys. Rev. D , vol.60 , pp. 125010
    • Haller, K.1    Chen, L.2    Choi, Y.S.3


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.