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// Helper functions/variable specific to this material |
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//----------------------------------------------------------------------------- |
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//----------------------------------------------------------------------------- |
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// Iridescence |
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//----------------------------------------------------------------------------- |
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// Ref: https://belcour.github.io/blog/research/2017/05/01/brdf-thin-film.html |
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// Evaluation XYZ sensitivity curves in Fourier space |
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float3 EvalSensitivity(float opd, float shift) |
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{ |
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// Use Gaussian fits, given by 3 parameters: val, pos and var |
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float phase = 2.0 * PI * opd * 1e-6; |
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float3 val = float3(5.4856e-13, 4.4201e-13, 5.2481e-13); |
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float3 pos = float3(1.6810e+06, 1.7953e+06, 2.2084e+06); |
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float3 var = float3(4.3278e+09, 9.3046e+09, 6.6121e+09); |
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float3 xyz = val * sqrt(2.0 * PI * var) * cos(pos * phase + shift) * exp(-var * phase * phase); |
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xyz.x += 9.7470e-14 * sqrt(2.0 * PI * 4.5282e+09) * cos(2.2399e+06 * phase + shift) * exp(-4.5282e+09 * phase * phase); |
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return xyz / 1.0685e-7; |
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} |
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// Evaluate the reflectance for a thin-film layer on top of a dielectric medum. |
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float3 EvalIridescence(float eta_1, float cosTheta1, BSDFData bsdfData) |
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{ |
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// thicknessIridescence unit is micrometer for this equation here. Mean 0.5 is 500nm. |
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float Dinc = 3.0 * bsdfData.thicknessIridescence; |
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// Note: Unlike the code provide with the paper, here we use schlick approximation |
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// Schlick is a very poor approximation when dealing with iridescence to the Fresnel |
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// term and there is no "neutral" value in this unlike in the original paper. |
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// We use Iridescence mask here to allow to have neutral value |
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// Hack: In order to use only one parameter (DInc), we deduced the ior of iridescence from current Dinc thicknessIridescence |
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// and we use mask instead to fade out the effect |
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float eta_2 = lerp(2.0, 1.0, bsdfData.thicknessIridescence); |
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// Following line from original code is not needed for us, it create a discontinuity |
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// Force eta_2 -> eta_1 when Dinc -> 0.0 |
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// float eta_2 = lerp(eta_1, eta_2, smoothstep(0.0, 0.03, Dinc)); |
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// Evaluate the cosTheta on the base layer (Snell law) |
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float cosTheta2 = sqrt(1.0 - Sq(eta_1 / eta_2) * (1.0 - Sq(cosTheta1))); |
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// First interface |
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float R0 = IorToFresnel0(eta_2, eta_1); |
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float R12 = F_Schlick(R0, cosTheta1); |
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float R21 = R12; |
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float T121 = 1.0 - R12; |
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float phi12 = 0.0; |
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float phi21 = PI - phi12; |
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// Second interface |
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float3 R23 = F_Schlick(bsdfData.fresnel0, cosTheta2); |
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float phi23 = 0.0; |
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// Phase shift |
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float OPD = Dinc * cosTheta2; |
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float phi = phi21 + phi23; |
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// Compound terms |
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float3 R123 = R12 * R23; |
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float3 r123 = sqrt(R123); |
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float3 Rs = Sq(T121) * R23 / (float3(1.0, 1.0, 1.0) - R123); |
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// Reflectance term for m = 0 (DC term amplitude) |
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float3 C0 = R12 + Rs; |
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float3 I = C0; |
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// Reflectance term for m > 0 (pairs of diracs) |
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float3 Cm = Rs - T121; |
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for (int m = 1; m <= 2; ++m) |
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{ |
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Cm *= r123; |
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float3 Sm = 2.0 * EvalSensitivity(m * OPD, m * phi); |
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//vec3 SmP = 2.0 * evalSensitivity(m*OPD, m*phi2.y); |
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I += Cm * Sm; |
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} |
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// Convert back to RGB reflectance |
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//I = clamp(mul(I, XYZ_TO_RGB), float3(0.0, 0.0, 0.0), float3(1.0, 1.0, 1.0)); |
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//I = mul(XYZ_TO_RGB, I); |
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return I; |
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} |
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#if HAS_REFRACTION |
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# include "CoreRP/ShaderLibrary/Refraction.hlsl" |
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void FillMaterialIridescence(float mask, float thickness, inout BSDFData bsdfData) |
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{ |
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bsdfData.iridescenceMask = mask; |
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bsdfData.thicknessIridescence = thickness; |
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bsdfData.iridescenceThickness = thickness; |
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} |
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// Note: this modify the parameter perceptualRoughness and fresnel0, so they need to be setup |
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bsdfData.thickness = max(thickness, 0.0001); |
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} |
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// Remap IOR in range 1..2.5 to 0..1 |
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float RemapIor25to01(float ior) |
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{ |
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return saturate((ior - 1.0) / 1.5); |
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} |
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float RemapIor01to25(float ior) |
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{ |
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return ior * 1.5 + 1.0; |
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} |
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// For image based lighting, a part of the BSDF is pre-integrated. |
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// This is done both for specular and diffuse (in case of DisneyDiffuse) |
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void GetPreIntegratedFGD(float NdotV, float perceptualRoughness, float3 fresnel0, out float3 specularFGD, out float diffuseFGD, out float reflectivity) |
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if (HasFeatureFlag(surfaceData.materialFeatures, MATERIALFEATUREFLAGS_LIT_IRIDESCENCE)) |
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{ |
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FillMaterialIridescence(surfaceData.iridescenceMask, surfaceData.thicknessIridescence, bsdfData); |
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FillMaterialIridescence(surfaceData.iridescenceMask, surfaceData.iridescenceThickness, bsdfData); |
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} |
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if (HasFeatureFlag(surfaceData.materialFeatures, MATERIALFEATUREFLAGS_LIT_CLEAR_COAT)) |
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{ |
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materialFeatureId = GBUFFER_LIT_IRIDESCENCE; |
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outGBuffer2.rgb = float3(surfaceData.iridescenceMask, surfaceData.thicknessIridescence, |
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outGBuffer2.rgb = float3(surfaceData.iridescenceMask, surfaceData.iridescenceThickness, |
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PackFloatInt8bit(surfaceData.metallic, 0, 8)); |
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} |
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else // Standard |
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result = (surfaceData.materialFeatures.xxx) / 255.0; // Aloow to read with color picker debug mode |
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break; |
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case DEBUGVIEW_LIT_SURFACEDATA_INDEX_OF_REFRACTION: |
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result = RemapIor25to01(surfaceData.ior).xxx; |
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result = saturate((surfaceData.ior - 1.0) / 1.5).xxx; |
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break; |
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} |
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} |
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result = (bsdfData.materialFeatures.xxx) / 255.0; // Aloow to read with color picker debug mode |
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break; |
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case DEBUGVIEW_LIT_BSDFDATA_IOR: |
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result = RemapIor25to01(bsdfData.ior).xxx; |
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result = saturate((bsdfData.ior - 1.0) / 1.5).xxx; |
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break; |
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} |
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} |
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if (bsdfData.iridescenceMask > 0.0) |
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{ |
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bsdfData.fresnel0 = lerp(bsdfData.fresnel0, EvalIridescence(topIor, viewAngle, bsdfData), bsdfData.iridescenceMask); |
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bsdfData.fresnel0 = lerp(bsdfData.fresnel0, EvalIridescence(topIor, viewAngle, bsdfData.iridescenceThickness, bsdfData.fresnel0), bsdfData.iridescenceMask); |
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} |
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} |
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float LdotH = saturate(invLenLV * LdotV + invLenLV); |
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float NdotV = ClampNdotV(preLightData.NdotV); |
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float3 F = F_Schlick(bsdfData.fresnel0, LdotH); |
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// Note: Here we are suppose to call EvalIridescence with LdotH |
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// This is to expensive for our need, so instead we use the NdotV |
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// Moreover, the bsdfData.fresnel0 here already contain the evaluation of F_Schlick |
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// in the context of iridescence, so if iridescence is enabled, don't apply schlick a second time |
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float3 F; |
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// Remark: Fresnel must be use with LdotH angle. But Fresnel for iridescence is expensive to compute at each light. |
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// Instead we use the incorrect angle NdotV as an approximation for LdotH for Fresnel evaluation. |
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// The Fresnel with iridescence and NDotV angle is precomputed ahead and here we jsut reuse the result. |
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// Thus why we shouldn't apply a second time Fresnel on the value if iridescence is enabled. |
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} |
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else |
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{ |
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F = F_Schlick(bsdfData.fresnel0, LdotH); |
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} |
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float DV; |
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Sebastien Lagarde
7 年前