Abstract
The 1-arm exponent \(\rho \) for the ferromagnetic Ising model on \(\mathbb {Z}^d\) is the critical exponent that describes how fast the critical 1-spin expectation at the center of the ball of radius r surrounded by plus spins decays in powers of r. Suppose that the spin-spin coupling J is translation-invariant, \(\mathbb {Z}^d\)-symmetric and finite-range. Using the random-current representation and assuming the anomalous dimension \(\eta =0\), we show that the optimal mean-field bound \(\rho \le 1\) holds for all dimensions \(d>4\). This significantly improves a bound previously obtained by a hyperscaling inequality.
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Acknowledgements
The work of AS is supported by the JSPS Grant-in-Aid for Challenging Exploratory Research 15K13440. The work of SH is supported by the Ministry of Education, Culture, Sports, Science and Technology through Program for Leading Graduate Schools (Hokkaido University “Ambitious Leader’s Program”). We thank Aernout van Enter for providing references about the history of the problem.
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We dedicate this work to Chuck Newman on the occasion of his 70th birthday.
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Handa, S., Heydenreich, M., Sakai, A. (2019). Mean-Field Bound on the 1-Arm Exponent for Ising Ferromagnets in High Dimensions. In: Sidoravicius, V. (eds) Sojourns in Probability Theory and Statistical Physics - I. Springer Proceedings in Mathematics & Statistics, vol 298. Springer, Singapore. https://doi.org/10.1007/978-981-15-0294-1_8
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