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4
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0004287813
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Cambridge University Press, Cambridge, UK
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For background, see D. Biskamp, Nonlinear Magnetohydrodynamics (Cambridge University Press, Cambridge, UK, 1993).
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(1993)
Nonlinear Magnetohydrodynamics
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Biskamp, D.1
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15
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0347486071
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There are physically interesting situations where this term survives; see R. Jackiw and S.-Y. Pi, Phys. Lett. B 423, 364 (1998)
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(1998)
Phys. Lett. B
, vol.423
, pp. 364
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Jackiw, R.1
Pi, S.-Y.2
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17
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0004012649
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Princeton University Press, Princeton, N.J., S. Treiman, R. Jackiw, B. Zumino, E. Witten
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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).
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(1985)
Current Algebra and Anomalies
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Jackiw, R.1
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19
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0041612876
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R. Epstein and W. Feldman
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G. Field, in Magnetospheric Phenomena in Astrophysics, edited by R. Epstein and W. Feldman, AIP Conf. Proc. No.144 (AIP, New York, 1986), p. 324.
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(1986)
Magnetospheric Phenomena in Astrophysics
, pp. 324
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Field, G.1
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20
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85037223156
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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.)
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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.)
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21
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85037199692
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Equation (2.28) was integrated numerically by Y. Bergner
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Equation (2.28) was integrated numerically by Y. Bergner.
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22
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17044439056
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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)
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(1999)
Phys. Rev. D
, vol.60
, pp. 125001
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Adam, C.1
Muratori, B.2
Nash, C.3
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24
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17044390796
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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).
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(1999)
Phys. Rev. D
, vol.60
, pp. 125010
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Haller, K.1
Chen, L.2
Choi, Y.S.3
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