The continuous Heisenberg chain is quantised semiclassically. The spectrum consists of unit spin bosons (magnons) and integer spin bosons (solitons) with dispersion laws E=JS(ka) 2 and E n =16JS 3 sin 2 (ka/4S)/n (n=1...) respectively. It is proposed that the n=1 soliton is the magnon and that the spectrum is exact, including all quantum corrections. For S= 1 / 2 the spectrum agrees with results for the discrete chain and it is inferred that the soliton is a multi-magnon bound state.
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Hans C. Fogedby (1980) studied this question.
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