1990NonlinearityOpen access

A numerical calculation of a weakly non-local solitary wave: the ϕ4breather

John P. Boyd

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Abstract

The breather of the phi 4 field theory decays by radiation to infinity. The concept of a solitary wave is still useful, however, because alpha , the amplitude of the 'far field' radiation, is exponentially small in in , the breather amplitude. (The phrase 'weakly non-local' in the title means that the quasisoliton has non-zero but very tiny amplitude as mod x mod to infinity .) The author introduces novel numerical methods to compute phi 4 breathers. He calculates solutions both on a finite, spatially periodic interval and on x in (- infinity , infinity ).

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The breather of the phi 4 field theory decays by radiation to infinity. The concept of a solitary wave is still useful, however, because alpha , the amplitude of the 'far field' radiation, is exponentially small in in , the breather amplitude. (The phrase 'weakly non-local' in the title means that the quasisoliton has non-zero but very tiny amplitude as mod x mod to infinity .) The author introduces novel numerical methods to compute phi 4 breathers. He calculates solutions both on a finite, spatially periodic interval and on x in (- infinity , infinity ).

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Available abstract

The breather of the phi 4 field theory decays by radiation to infinity. The concept of a solitary wave is still useful, however, because alpha , the amplitude of the 'far field' radiation, is exponentially small in in , the breather amplitude. (The phrase 'weakly non-local' in the title means that the quasisoliton has non-zero but very tiny amplitude as mod x mod to infinity .) The author introduces novel numerical methods to compute phi 4 breathers. He calculates solutions both on a finite, spatially periodic interval and on x in (- infinity , infinity ).

Key concepts: Breather, Infinity, Mathematics, Amplitude, Interval (graph theory), Mathematical analysis, Mathematical physics, Field (mathematics)

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