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Lorentz-invariant scalar field theories in d+1 dimensions with second-order derivative terms are unable to support static soliton solutions that are both finite in energy and stable for d>2, a result known as Derrick's theorem.
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G. H. Derrick, J. Math. Phys. 5, 1252 (1964)
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E. B. Bogomol’nyi, Sov. J. Nucl. Phys. 24, 4 (1976); M. K. Prasad and C. M. Sommerfield, Phys. Rev. Lett. 35, 760 (1975)
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G. Parisi and N. Sourlas, Nucl. Phys. B206, 321 (1982)
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P. Hořava and C. M. Melby-Thompson, [arXiv:1007.3657]
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Closest in time.
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J. E. Thompson and R. R. Volkas, [arXiv:1008.2054]
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