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For N=2 the collinear FP is (Ref.) u1 =6.3(4), u2 =-8.3(3) (MZM) and u1 =0.33(3), u2 =-0.30(2) (3d- MS̄). For N=3 the collinear FP is u1 =4.3(5), u2 =-7.5(6) (MZM) and u1 =0.23(5), u2 =-0.23(3) (3d- MS̄).
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For N=2 the collinear FP is (Ref.) u1 =6.3(4), u2 =-8.3(3) (MZM) and u1 =0.33(3), u2 =-0.30(2) (3d- MS̄). For N=3 the collinear FP is u1 =4.3(5), u2 =-7.5(6) (MZM) and u1 =0.23(5), u2 =-0.23(3) (3d- MS̄).
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At the chiral FP we use (Refs.) ν=0.60(8), y11 =2.3(2), and y02 =1.52(6) (N=3) and ν=0.63(9), y11 =2.45(25), and y02 =1.30(15) (N=2). At the collinear FP, for N=3 we use (Refs.) ν=0.60(5), y11 =1.20(15), and y02 =2.0(2). For N=2, we use the mapping with the XY model (Refs.) and the results of PRBMDO 0163-1829
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At the chiral FP we use (Refs.) ν=0.60(8), y11 =2.3(2), and y02 =1.52(6) (N=3) and ν=0.63(9), y11 =2.45(25), and y02 =1.30(15) (N=2). At the collinear FP, for N=3 we use (Refs.) ν=0.60(5), y11 =1.20(15), and y02 =2.0(2). For N=2, we use the mapping with the XY model (Refs.) and the results of M. Campostrini, M. Hasenbusch, A. Pelissetto, and E. Vicari, Phys. Rev. B PRBMDO 0163-1829 74 (2006) (in press), ν=0.6717(1), y11 =1 ν=1.4888(2), and y02 =2-η=1.9619(2).
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It is interesting to note that the exponents of the O(4) O(2) model are also relevant for quantum chromodynamics (the theory of strong interactions) with two quarks at finite temperature if the anomaly contribution at the critical point is small
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It is interesting to note that the exponents of the O(4) O(2) model are also relevant for quantum chromodynamics (the theory of strong interactions) with two quarks at finite temperature if the anomaly contribution at the critical point is small [F. Basile, A. Pelissetto, and E. Vicari, POS (LAT2005) 199;
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Basile, F.1
Pelissetto, A.2
Vicari, E.3
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