TY - JOUR
T1 - High-order fuchsian equations for the square lattice Ising model
T2 - χ(6)
AU - Boukraa, S.
AU - Hassani, S.
AU - Jensen, I.
AU - Maillard, J. M.
AU - Zenine, N.
PY - 2010/2/26
Y1 - 2010/2/26
N2 - This paper deals with χ(6), the six-particle contribution to the magnetic susceptibility of the square lattice Ising model. We have generated, modulo a prime, series coefficients for χ(6). The length of the series is sufficient to produce the corresponding Fuchsian linear differential equation (modulo a prime). We obtain the Fuchsian linear differential equation that annihilates the depleted series θ(6) = χ(6) - 2/3χ(4) ?+ 2/45 χ(2). The factorization of the corresponding differential operator is performed using a method of factorization modulo a prime, introduced in a previous paper. The depleted differential operator is shown to have a structure similar to the corresponding operator for χ(5). It splits into factors of smaller orders, with the left-most factor of order 6 being equivalent to the symmetric fifth power of the linear differential operator corresponding to the elliptic integral E. The right-most factor has a direct sum structure, and using series calculated modulo several primes, all the factors in the direct sum have been reconstructed in exact arithmetics.
AB - This paper deals with χ(6), the six-particle contribution to the magnetic susceptibility of the square lattice Ising model. We have generated, modulo a prime, series coefficients for χ(6). The length of the series is sufficient to produce the corresponding Fuchsian linear differential equation (modulo a prime). We obtain the Fuchsian linear differential equation that annihilates the depleted series θ(6) = χ(6) - 2/3χ(4) ?+ 2/45 χ(2). The factorization of the corresponding differential operator is performed using a method of factorization modulo a prime, introduced in a previous paper. The depleted differential operator is shown to have a structure similar to the corresponding operator for χ(5). It splits into factors of smaller orders, with the left-most factor of order 6 being equivalent to the symmetric fifth power of the linear differential operator corresponding to the elliptic integral E. The right-most factor has a direct sum structure, and using series calculated modulo several primes, all the factors in the direct sum have been reconstructed in exact arithmetics.
UR - http://www.scopus.com/inward/record.url?scp=77649249430&partnerID=8YFLogxK
UR - http://purl.org/au-research/grants/ARC/DP0770705
U2 - 10.1088/1751-8113/43/11/115201
DO - 10.1088/1751-8113/43/11/115201
M3 - Article
AN - SCOPUS:77649249430
SN - 1751-8113
VL - 43
JO - Journal of Physics. A: Mathematical and Theoretical
JF - Journal of Physics. A: Mathematical and Theoretical
IS - 11
M1 - 115201
ER -