MODULE XC2SG3P USE XC2NS3P CONTAINS * * ..File: xc2sg3p.f F_2^PS and F_2^G * * * ..Parametrizations of the 3-loop MS(bar) pure-singlet and gluon coef- * ficient functions for the electromagnetic structure function F_2 * at mu_r = mu_f = Q. The expansion parameter is alpha_s/(4 pi). * * ..The relative accuracy of these parametrizations, as well as of * the convolution results, is one part in thousand or better. * * ..Reference: J. Vermaseren, A. Vogt and S. Moch * hep-ph/0504242 = Nucl. Phys. B724 (2005) 3 * * ===================================================================== * * * ..The pure-singlet coefficient function, regular piece * FUNCTION C2S3A (Y, DL, NF, CC) IMPLICIT REAL*8 (A-Z) DIMENSION FL(6), FLS(6) INTEGER NF INTEGER CC ! charged current DATA FL / -1.d0, 0.5d0, 0.d0, 0.5d0, 0.2d0, 0.5d0 / DATA FLS / 1.d0, 0.1d0, 0.d0, 0.1d0, 0.018181818d0, 0.1d0 / * Y1 = Y1VAL(Y, DL) DL1 = DL1VAL(Y, DL) D9 = 1./9.D0 D81 = D9*D9 FL11 = FL(NF) FLS11 = FLS(NF) * C2S3A = 0.D0 IF (CC.EQ.1) THEN C2S31 = ( 856.*D81 * DL1**4 - 6032.*D81 * DL1**3 + 130.57* DL1**2 , - 542.0 * DL1 + 8501. - 4714.* Y + 61.50 * Y**2 ) * Y1 , + DL*DL1 * (8831.* DL + 4162.* Y1) - 15.44 * Y*DL**5 , + 3333.* Y*DL**2 + 1615.* DL + 1208.* DL**2 , - 333.73 * DL**3 + 4244.*D81 * DL**4 - 40.*D9 * DL**5 , - 2731.82 * Y1/Y - 414.262 * DL/Y C2S32 = ( - 64.*D81 * DL1**3 + 208.*D81 * DL1**2 + 23.09 * DL1 , - 220.27 + 59.80 * Y - 177.6 * Y**2) * Y1 + , - DL*DL1 * (160.3 * DL + 135.4 * Y1) - 24.14 * Y*DL**3 , - 215.4 * Y*DL**2 - 209.8 * DL - 90.38 * DL**2 , - 3568./243.* DL**3 - 184.*D81 * DL**4 + 40.2426 * Y1/Y C2S3A = NF * ( C2S31 + NF * C2S32 ) ELSE C2S3F = ( ( 126.42 - 50.29 * Y - 50.15 * Y**2) * Y1 - 26.717 , - 320.*D81 * DL**2 * (DL+5.D0) + 59.59 * DL , - Y*DL**2 * (101.8 + 34.79 * DL + 3.070 * DL**2) , - 9.075 * Y*Y1*DL1 ) * Y C2S3A = NF * (FLS11-FL11) * C2S3F ENDIF * RETURN END FUNCTION * * --------------------------------------------------------------------- * * * ..The (truncated) 'local' piece due to the FL11 contribution * FUNCTION C2S3C (Y, NF) IMPLICIT REAL*8 (A - Z) INTEGER NF DIMENSION FL(6), FLS(6) DATA FL / -1.d0, 0.5d0, 0.d0, 0.5d0, 0.2d0, 0.5d0 / DATA FLS / 1.d0, 0.1d0, 0.d0, 0.1d0, 0.018181818d0, 0.1d0 / * FL11 = FL(NF) FLS11 = FLS(NF) C2S3C = - (FLS11-FL11) * NF * 11.8880 * RETURN END FUNCTION * * --------------------------------------------------------------------- * * * ..The gluon coefficient function * FUNCTION C2G3A (Y, DL, NF, CC) IMPLICIT REAL*8 (A-Z) DIMENSION FLG(6) INTEGER NF INTEGER CC ! charged current DATA FLG / 1.d0, 0.1d0, 0.d0, 0.1d0, 0.018181818d0, 0.1d0 / * YI = 1./Y DL1 = DL1VAL(Y, DL) D9 = 1./9.D0 D81 = D9*D9 FLG11 = FLG(NF) * C2G3A = 0.D0 IF (CC.EQ.1) THEN C2G31 = , 966.*D81 * DL1**5 - 935.5*D9 * DL1**4 + 89.31 * DL1**3 , + 979.2 * DL1**2 - 2405. * DL1 + 1372.* (1.-Y)* DL1**4 , - 15729. - 310510.* Y + 331570.* Y**2 - 244150.* Y*DL**2 , - 253.3* Y*DL**5 , + DL*DL1 * (138230. - 237010.* DL) - 11860.* DL , - 700.8 * DL**2 - 1440.* DL**3 + 2480.5*D81 * DL**4 , - 134.*D9 * DL**5 - 6362.54 * YI - 932.089 * DL*YI C2G32 = , 131.*D81 * DL1**4 - 14.72 * DL1**3 + 3.607 * DL1**2 , - 226.1 * DL1 + 4.762 - 190.0 * Y - 818.4 * Y**2 , - 4019.* Y*DL**2 - DL*DL1 * (791.5 + 4646 * DL) , + 739.0 * DL + 418.0 * DL**2 + 104.3 * DL**3 , + 809.*D81 * DL**4 + 12.*D9 * DL**5 + 84.423 * YI C2G3A = NF * ( C2G31 + NF * C2G32 ) ELSE C2G3F = 3.211 * DL1**2 + 19.04 * Y*DL1 + 0.623 * (1.-Y)*DL1**3 , - 64.47 * Y + 121.6 * Y**2 - 45.82 * Y**3 - Y*DL*DL1 , * ( 31.68 + 37.24 * DL) - Y*DL * (82.40 + 16.08 * DL) , + Y*DL**3 * (520.*D81 + 11.27 * Y) + 60.*D81 * Y*DL**4 C2G3A = NF * NF * FLG11 * C2G3F ENDIF * RETURN END FUNCTION * * --------------------------------------------------------------------- * * * ..The artificial 'local' piece, introduced to fine-tune the accuracy. * FUNCTION C2G3C (Y, NF) IMPLICIT REAL*8 (A - Z) INTEGER NF * C2G3C = 0.625 * NF * RETURN END FUNCTION * * =================================================================av== END MODULE XC2SG3P