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1K2 Modifier for Legendre or Cosine coefficients of theform k**2 d-Sig/d-Omega = Sum(a(L)*p(L)), wherek = wave vector2AG times 2 * isotopic abund. and stat. weight factor 2G times 2 * statistical weight factor 2L2 Modifier for Legendre or Cosine coefficients of theform d-Sig/d-Omega = (1/2)Sum((2L+1)*a(L)*p(L))4AG times 4 * isotopic abund. and stat. weight factor 4PI times 4 pi AA Adler-Adler formalismfor resonance parametersAG times isotopic abund. and stat. weight factor AL1 Coefficients for first-order associated Legendrefunctions of the first kindAMP Amplitude (for resonance parameters) ANA Vector analyzing power, A(y), for incident beam ASY Asymmetry of polarization of outgoing particles AXX Tensor analyzing power, Cartesian coord. AYY Tensor analyz.power,inc.proj.spin normal to scatt.planeTensor analyzing power, incident projectile spinnormal to scattering planeAZZ Tensor analyz.power,inc.proj.spin parall.to scatt.planeTensor analyzing power, incident projectile spinparallel to beam direction in scattering planeC Spin correlation parameter COS Cosine coefficients CS2 Coefficients of the form d-Sig/d-Omega = a(0) +a(1)*Sin**2(Theta) + a(2)*Sin**2(Theta)*Cos(Theta) +a(3)*Sin**2(Theta)*Cos**2(Theta)D Spin rotation parameter DSP Difference for spins parallel - antiparallel DT production thick/thin target yield G times statistical weight factor IPA integrated over partial angular range K Spin transfer parameter L4P Modifier for Legendre or Cos coefficients of the form4pi*d-Sig/d-Omega =Sum((2L+1)*a(L)*p(L))LEG Legendre coefficients LIM Modifier for a resonance integral given for alimited EN-range onlyMOT relative to Mott scattering MXD Spectrum rel.to Maxw.distr.of given temperature NCP Non-coplanar NSF Non-spin-flip PHY Physical yield PP Inc.proj.parallel/perpendicular to reac.plane RES at peak of resonance RG times (2J(i)+1) * (2J(j)+1) RM Reich-Moore formalismfor resonance parametersRMT R-matrix formalismfor resonance parametersRNV Non-1/v partof cross-section or resonance-integralRS Times 4pi/SigmaModifier for diff.cross-sections 4pi/Sig d-Sig/d-Omegaand for Legendre or Cosine coefficients of the form:(4pi/Sig)*(d-Sig/d-Omega) = Sum(a(L)*p(L))RS0 Modifier for Legendre or Cosine coefficients of theform:(d-Sig/d-Omega)/(d-Sig/d-Omega at 0 deg)=Sum(a(L)*p(L)RSD Modifier for Legendre or Cosine coefficients of theform:(d-Sig/d-Omega)/(d-Sig/d-Omega at 90 deg) == 1 +Sum(a(L)*p(L))Also modifier for angular distributions of the form:Sig(Theta)/Sig(90deg) and for the anisotropy-coeffSig(0)/Sig(90deg)RSL Modifier for Legendre or Cosine coefficients of theform:(4pi/Sig)*(d-Sig/d-Omega)=Sum((2L+1)*a(L)*p(L))RTE times square-root(E) RTH relative to Rutherford scattering RV 1/v part only S0 times total peak cross section S2T Coefficients of the form: d-Sig/d-Omega =a(0) + A(1)*sin**2(Theta) + a(2)*sin**2(2*Theta)SF Spin flip SFC S-factor SN2 Coefficients for a sum in power of Sine**2 SQ Quantity squared SRF Spin rotation function SS Spin-spin cross section TAP Tensor analyzing power, spherical coordinates TM per 1 MeV target thickness (for thick target yields) TRN Transmission TST Total spin transfer TT Measured for thick target VAP Vector analyzing power, spherical coordinates VGT Vogt formalismfor resonance parameters=======================================================The following modifiers may be added to any quantitycode without entry in Dictionary 36. These generalquantity modifiers must be coded after any modifierincluded in Dictionary 36.=======================================================(A) Uncertain if corrected for natural isotopic abund.Unclear whether corrected for natural isotopicabundance of target. To be used only when data aregiven for an isotope, but were measured on a targetwith natural isotopic composition.For enriched targets use modifier 'FCT' instead.A Data times natural isotopic abundanceTo be used only when data are given for an isotope,but were measured on a target with natural isotopiccomposition. For enriched targets use modifier'FCT' instead.AV Average FCT times a factor (see text) MSC Approximate definition only, see REACTION text==Note==This is approximate definition only, see textGeneral purpose modifier for unusual data types. Exactdefinition is given in free text following thereaction code. Use with code from dict.36 which isclosest to data given.RAW Raw data (see REACTION text) REL Relative dataTo be combined with arbitrary units.Otherwise use 'FCT'.BRA Bremsstrahlung spectrum average BRS Average over part of bremsstrahlung spectrum EPI Epithermal neutron spectrum average FIS Fission spectrum average FST Fast reactor neutron spectrum average MXW Maxwellian averageThe appropriate spectrum temperature is to be givenunder data heading 'KT', or the mean energy under'EN-MEAN' (if given by author) or 'EN-DUMMY' (ifassumed by compiler).==Note== 'MXW' previously meant 'thermal Maxwellianaverage'.SPA Spectrum average