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New York: Wiley, ρ is a scalar rather than the time-component of a Lorentz vector. This distinction makes no difference in the noninteracting case, but our choice allows introducing self-interactions in a Lorentz-invariant manner
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Bazeia1
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14. This result was established with a hodographic transformation for d = 2 by Bordemann and Hoppe (first paper in Ref. [2]) and for arbitrary d by Jackiw and Polychronakos, Ref. [11]; see also Bazeia, Ref. [4]. The present, simple approach was shown to us by Hoppe; see also Hoppe, J.: Phys. Lett. B329, 10 (1994)
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15. This result was established with a hodographic transformation for d = 2 by Bordemann and Hoppe (second paper in Ref. [2]); see also Hoppe, Ref. [14]
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