HX-PGS-AIM-Android/Library/PackageCache/com.unity.render-pipelines..../ShaderLibrary/BSDF.hlsl

#ifndef UNITY_BSDF_INCLUDED
#define UNITY_BSDF_INCLUDED

#if SHADER_API_MOBILE || SHADER_API_GLES3 || SHADER_API_SWITCH || defined(UNITY_UNIFIED_SHADER_PRECISION_MODEL)
#pragma warning (disable : 3205) // conversion of larger type to smaller
#endif

#include "Packages/com.unity.render-pipelines.core/ShaderLibrary/Color.hlsl"

// Note: All NDF and diffuse term have a version with and without divide by PI.
// Version with divide by PI are use for direct lighting.
// Version without divide by PI are use for image based lighting where often the PI cancel during importance sampling

//-----------------------------------------------------------------------------
// Help for BSDF evaluation
//-----------------------------------------------------------------------------

// Cosine-weighted BSDF (a BSDF taking the projected solid angle into account).
// If some of the values are monochromatic, the compiler will optimize accordingly.
struct CBSDF
{
    float3 diffR; // Diffuse  reflection   (T -> MS -> T, same sides)
    float3 specR; // Specular reflection   (R, RR, TRT, etc)
    float3 diffT; // Diffuse  transmission (rough T or TT, opposite sides)
    float3 specT; // Specular transmission (T, TT, TRRT, etc)
};

//-----------------------------------------------------------------------------
// Fresnel term
//-----------------------------------------------------------------------------

real F_Schlick(real f0, real f90, real u)
{
    real x = 1.0 - u;
    real x2 = x * x;
    real x5 = x * x2 * x2;
    return (f90 - f0) * x5 + f0;                // sub mul mul mul sub mad
}

real F_Schlick(real f0, real u)
{
    return F_Schlick(f0, 1.0, u);               // sub mul mul mul sub mad
}

real3 F_Schlick(real3 f0, real f90, real u)
{
    real x = 1.0 - u;
    real x2 = x * x;
    real x5 = x * x2 * x2;
    return f0 * (1.0 - x5) + (f90 * x5);        // sub mul mul mul sub mul mad*3
}

real3 F_Schlick(real3 f0, real u)
{
    return F_Schlick(f0, 1.0, u);               // sub mul mul mul sub mad*3
}

// Does not handle TIR.
real F_Transm_Schlick(real f0, real f90, real u)
{
    real x = 1.0 - u;
    real x2 = x * x;
    real x5 = x * x2 * x2;
    return (1.0 - f90 * x5) - f0 * (1.0 - x5);  // sub mul mul mul mad sub mad
}

// Does not handle TIR.
real F_Transm_Schlick(real f0, real u)
{
    return F_Transm_Schlick(f0, 1.0, u);        // sub mul mul mad mad
}

// Does not handle TIR.
real3 F_Transm_Schlick(real3 f0, real f90, real u)
{
    real x = 1.0 - u;
    real x2 = x * x;
    real x5 = x * x2 * x2;
    return (1.0 - f90 * x5) - f0 * (1.0 - x5);  // sub mul mul mul mad sub mad*3
}

// Does not handle TIR.
real3 F_Transm_Schlick(real3 f0, real u)
{
    return F_Transm_Schlick(f0, 1.0, u);        // sub mul mul mad mad*3
}

// Compute the cos of critical angle: cos(asin(eta)) == sqrt(1.0 - eta*eta)
// eta == IORMedium/IORSource
// If eta >= 1 the it's an AirMedium interation, otherwise it's MediumAir interation
real CosCriticalAngle(real eta)
{
    return sqrt(max(1.0 - Sq(eta), 0.0));
    // For 1 <= IOR <= 4: Max error: 0.0268594
    //return eta >= 1.0 ? 0.0 : (((3.0 + eta) * sqrt(max(0.0, 1.0 - eta))) / (2.0 * sqrt(2.0)));
    // For 1 <= IOR <= 4: Max error: 0.00533065
    //return eta >= 1.0 ? 0.0 : (-((-23.0 - 10.0 * eta + Sq(eta)) * sqrt(max(0.0, 1.0 - eta))) / (16.0 * sqrt(2.0)));
    // For 1 <= IOR <= 4: Max error: 0.00129402
    //return eta >= 1.0 ? 0.0 : (((91.0 + 43.0 * eta - 7.0 * Sq(eta) + pow(eta, 3)) * sqrt(max(0.0, 1.0 - eta))) / (64. * sqrt(2.0)));
}

// Ref: https://seblagarde.wordpress.com/2013/04/29/memo-on-fresnel-equations/
// Fresnel dielectric / dielectric
real F_FresnelDielectric(real ior, real u)
{
    real g = sqrt(Sq(ior) + Sq(u) - 1.0);

    // The "1.0 - saturate(1.0 - result)" formulation allows to recover form cases where g is undefined, for IORs < 1
    return 1.0 - saturate(1.0 - 0.5 * Sq((g - u) / (g + u)) * (1.0 + Sq(((g + u) * u - 1.0) / ((g - u) * u + 1.0))));
}

// Fresnel dieletric / conductor
// Note: etak2 = etak * etak (optimization for Artist Friendly Metallic Fresnel below)
// eta = eta_t / eta_i and etak = k_t / n_i
real3 F_FresnelConductor(real3 eta, real3 etak2, real cosTheta)
{
    real cosTheta2 = cosTheta * cosTheta;
    real sinTheta2 = 1.0 - cosTheta2;
    real3 eta2 = eta * eta;

    real3 t0 = eta2 - etak2 - sinTheta2;
    real3 a2plusb2 = sqrt(t0 * t0 + 4.0 * eta2 * etak2);
    real3 t1 = a2plusb2 + cosTheta2;
    real3 a = sqrt(0.5 * (a2plusb2 + t0));
    real3 t2 = 2.0 * a * cosTheta;
    real3 Rs = (t1 - t2) / (t1 + t2);

    real3 t3 = cosTheta2 * a2plusb2 + sinTheta2 * sinTheta2;
    real3 t4 = t2 * sinTheta2;
    real3 Rp = Rs * (t3 - t4) / (t3 + t4);

    return 0.5 * (Rp + Rs);
}

// Conversion FO/IOR

TEMPLATE_2_FLT_HALF(IorToFresnel0, transmittedIor, incidentIor, return Sq((transmittedIor - incidentIor) / (transmittedIor + incidentIor)) )
// ior is a value between 1.0 and 3.0. 1.0 is air interface
real IorToFresnel0(real transmittedIor)
{
    return IorToFresnel0(transmittedIor, 1.0);
}

// Assume air interface for top
// Note: We don't handle the case fresnel0 == 1
//real Fresnel0ToIor(real fresnel0)
//{
//    real sqrtF0 = sqrt(fresnel0);
//    return (1.0 + sqrtF0) / (1.0 - sqrtF0);
//}
TEMPLATE_1_FLT_HALF(Fresnel0ToIor, fresnel0, return ((1.0 + sqrt(fresnel0)) / (1.0 - sqrt(fresnel0))) )

// This function is a coarse approximation of computing fresnel0 for a different top than air (here clear coat of IOR 1.5) when we only have fresnel0 with air interface
// This function is equivalent to IorToFresnel0(Fresnel0ToIor(fresnel0), 1.5)
// mean
// real sqrtF0 = sqrt(fresnel0);
// return Sq(1.0 - 5.0 * sqrtF0) / Sq(5.0 - sqrtF0);
// Optimization: Fit of the function (3 mad) for range [0.04 (should return 0), 1 (should return 1)]
TEMPLATE_1_FLT_HALF(ConvertF0ForAirInterfaceToF0ForClearCoat15, fresnel0, return saturate(-0.0256868 + fresnel0 * (0.326846 + (0.978946 - 0.283835 * fresnel0) * fresnel0)))

// Even coarser approximation of ConvertF0ForAirInterfaceToF0ForClearCoat15 (above) for mobile (2 mad)
TEMPLATE_1_FLT_HALF(ConvertF0ForAirInterfaceToF0ForClearCoat15Fast, fresnel0, return saturate(fresnel0 * (fresnel0 * 0.526868 + 0.529324) - 0.0482256))

// Artist Friendly Metallic Fresnel Ref: http://jcgt.org/published/0003/04/03/paper.pdf

real3 GetIorN(real3 f0, real3 edgeTint)
{
    real3 sqrtF0 = sqrt(f0);
    return lerp((1.0 - f0) / (1.0 + f0), (1.0 + sqrtF0) / (1.0 - sqrt(f0)), edgeTint);
}

real3 getIorK2(real3 f0, real3 n)
{
    real3 nf0 = Sq(n + 1.0) * f0 - Sq(f0 - 1.0);
    return nf0 / (1.0 - f0);
}

// same as regular refract except there is not the test for total internal reflection + the vector is flipped for processing
real3 CoatRefract(real3 X, real3 N, real ieta)
{
    real XdotN = saturate(dot(N, X));
    return ieta * X + (sqrt(1 + ieta * ieta * (XdotN * XdotN - 1)) - ieta * XdotN) * N;
}

//-----------------------------------------------------------------------------
// Specular BRDF
//-----------------------------------------------------------------------------

float Lambda_GGX(float roughness, float3 V)
{
    return 0.5 * (sqrt(1.0 + (Sq(roughness * V.x) + Sq(roughness * V.y)) / Sq(V.z)) - 1.0);
}

real D_GGXNoPI(real NdotH, real roughness)
{
    real a2 = Sq(roughness);
    real s = (NdotH * a2 - NdotH) * NdotH + 1.0;

    // If roughness is 0, returns (NdotH == 1 ? 1 : 0).
    // That is, it returns 1 for perfect mirror reflection, and 0 otherwise.
    return SafeDiv(a2, s * s);
}

real D_GGX(real NdotH, real roughness)
{
    return INV_PI * D_GGXNoPI(NdotH, roughness);
}

// Ref: Understanding the Masking-Shadowing Function in Microfacet-Based BRDFs, p. 19, 29.
// p. 84 (37/60)
real G_MaskingSmithGGX(real NdotV, real roughness)
{
    // G1(V, H)    = HeavisideStep(VdotH) / (1 + Lambda(V)).
    // Lambda(V)        = -0.5 + 0.5 * sqrt(1 + 1 / a^2).
    // a           = 1 / (roughness * tan(theta)).
    // 1 + Lambda(V)    = 0.5 + 0.5 * sqrt(1 + roughness^2 * tan^2(theta)).
    // tan^2(theta) = (1 - cos^2(theta)) / cos^2(theta) = 1 / cos^2(theta) - 1.
    // Assume that (VdotH > 0), e.i. (acos(LdotV) < Pi).

    return 1.0 / (0.5 + 0.5 * sqrt(1.0 + Sq(roughness) * (1.0 / Sq(NdotV) - 1.0)));
}

// Precompute part of lambdaV
real GetSmithJointGGXPartLambdaV(real NdotV, real roughness)
{
    real a2 = Sq(roughness);
    return sqrt((-NdotV * a2 + NdotV) * NdotV + a2);
}

// Note: V = G / (4 * NdotL * NdotV)
// Ref: http://jcgt.org/published/0003/02/03/paper.pdf
real V_SmithJointGGX(real NdotL, real NdotV, real roughness, real partLambdaV)
{
    real a2 = Sq(roughness);

    // Original formulation:
    // lambda_v = (-1 + sqrt(a2 * (1 - NdotL2) / NdotL2 + 1)) * 0.5
    // lambda_l = (-1 + sqrt(a2 * (1 - NdotV2) / NdotV2 + 1)) * 0.5
    // G        = 1 / (1 + lambda_v + lambda_l);

    // Reorder code to be more optimal:
    real lambdaV = NdotL * partLambdaV;
    real lambdaL = NdotV * sqrt((-NdotL * a2 + NdotL) * NdotL + a2);

    // Simplify visibility term: (2.0 * NdotL * NdotV) /  ((4.0 * NdotL * NdotV) * (lambda_v + lambda_l))
    return 0.5 / max(lambdaV + lambdaL, REAL_MIN);
}

real V_SmithJointGGX(real NdotL, real NdotV, real roughness)
{
    real partLambdaV = GetSmithJointGGXPartLambdaV(NdotV, roughness);
    return V_SmithJointGGX(NdotL, NdotV, roughness, partLambdaV);
}

// Inline D_GGX() * V_SmithJointGGX() together for better code generation.
real DV_SmithJointGGX(real NdotH, real NdotL, real NdotV, real roughness, real partLambdaV)
{
    real a2 = Sq(roughness);
    real s = (NdotH * a2 - NdotH) * NdotH + 1.0;

    real lambdaV = NdotL * partLambdaV;
    real lambdaL = NdotV * sqrt((-NdotL * a2 + NdotL) * NdotL + a2);

    real2 D = real2(a2, s * s);            // Fraction without the multiplier (1/Pi)
    real2 G = real2(1, lambdaV + lambdaL); // Fraction without the multiplier (1/2)

    // This function is only used for direct lighting.
    // If roughness is 0, the probability of hitting a punctual or directional light is also 0.
    // Therefore, we return 0. The most efficient way to do it is with a max().
    return INV_PI * 0.5 * (D.x * G.x) / max(D.y * G.y, REAL_MIN);
}

real DV_SmithJointGGX(real NdotH, real NdotL, real NdotV, real roughness)
{
    real partLambdaV = GetSmithJointGGXPartLambdaV(NdotV, roughness);
    return DV_SmithJointGGX(NdotH, NdotL, NdotV, roughness, partLambdaV);
}

// Precompute a part of LambdaV.
// Note on this linear approximation.
// Exact for roughness values of 0 and 1. Also, exact when the cosine is 0 or 1.
// Otherwise, the worst case relative error is around 10%.
// https://www.desmos.com/calculator/wtp8lnjutx
real GetSmithJointGGXPartLambdaVApprox(real NdotV, real roughness)
{
    real a = roughness;
    return NdotV * (1 - a) + a;
}

real V_SmithJointGGXApprox(real NdotL, real NdotV, real roughness, real partLambdaV)
{
    real a = roughness;

    real lambdaV = NdotL * partLambdaV;
    real lambdaL = NdotV * (NdotL * (1 - a) + a);

    return 0.5 / (lambdaV + lambdaL);
}

real V_SmithJointGGXApprox(real NdotL, real NdotV, real roughness)
{
    real partLambdaV = GetSmithJointGGXPartLambdaVApprox(NdotV, roughness);
    return V_SmithJointGGXApprox(NdotL, NdotV, roughness, partLambdaV);
}

// roughnessT -> roughness in tangent direction
// roughnessB -> roughness in bitangent direction
real D_GGXAnisoNoPI(real TdotH, real BdotH, real NdotH, real roughnessT, real roughnessB)
{
    real a2 = roughnessT * roughnessB;
    real3 v = real3(roughnessB * TdotH, roughnessT * BdotH, a2 * NdotH);
    real  s = dot(v, v);

    // If roughness is 0, returns (NdotH == 1 ? 1 : 0).
    // That is, it returns 1 for perfect mirror reflection, and 0 otherwise.
    return SafeDiv(a2 * a2 * a2, s * s);
}

real D_GGXAniso(real TdotH, real BdotH, real NdotH, real roughnessT, real roughnessB)
{
    return INV_PI * D_GGXAnisoNoPI(TdotH, BdotH, NdotH, roughnessT, roughnessB);
}

real GetSmithJointGGXAnisoPartLambdaV(real TdotV, real BdotV, real NdotV, real roughnessT, real roughnessB)
{
    return length(real3(roughnessT * TdotV, roughnessB * BdotV, NdotV));
}

// Note: V = G / (4 * NdotL * NdotV)
// Ref: https://cedec.cesa.or.jp/2015/session/ENG/14698.html The Rendering Materials of Far Cry 4
real V_SmithJointGGXAniso(real TdotV, real BdotV, real NdotV, real TdotL, real BdotL, real NdotL, real roughnessT, real roughnessB, real partLambdaV)
{
    real lambdaV = NdotL * partLambdaV;
    real lambdaL = NdotV * length(real3(roughnessT * TdotL, roughnessB * BdotL, NdotL));

    return 0.5 / (lambdaV + lambdaL);
}

real V_SmithJointGGXAniso(real TdotV, real BdotV, real NdotV, real TdotL, real BdotL, real NdotL, real roughnessT, real roughnessB)
{
    real partLambdaV = GetSmithJointGGXAnisoPartLambdaV(TdotV, BdotV, NdotV, roughnessT, roughnessB);
    return V_SmithJointGGXAniso(TdotV, BdotV, NdotV, TdotL, BdotL, NdotL, roughnessT, roughnessB, partLambdaV);
}

// Inline D_GGXAniso() * V_SmithJointGGXAniso() together for better code generation.
real DV_SmithJointGGXAniso(real TdotH, real BdotH, real NdotH, real NdotV,
                           real TdotL, real BdotL, real NdotL,
                           real roughnessT, real roughnessB, real partLambdaV)
{
    real a2 = roughnessT * roughnessB;
    real3 v = real3(roughnessB * TdotH, roughnessT * BdotH, a2 * NdotH);
    real  s = dot(v, v);

    real lambdaV = NdotL * partLambdaV;
    real lambdaL = NdotV * length(real3(roughnessT * TdotL, roughnessB * BdotL, NdotL));

    real2 D = real2(a2 * a2 * a2, s * s);  // Fraction without the multiplier (1/Pi)
    real2 G = real2(1, lambdaV + lambdaL); // Fraction without the multiplier (1/2)

    // This function is only used for direct lighting.
    // If roughness is 0, the probability of hitting a punctual or directional light is also 0.
    // Therefore, we return 0. The most efficient way to do it is with a max().
    return (INV_PI * 0.5) * (D.x * G.x) / max(D.y * G.y, REAL_MIN);
}

real DV_SmithJointGGXAniso(real TdotH, real BdotH, real NdotH,
                           real TdotV, real BdotV, real NdotV,
                           real TdotL, real BdotL, real NdotL,
                           real roughnessT, real roughnessB)
{
    real partLambdaV = GetSmithJointGGXAnisoPartLambdaV(TdotV, BdotV, NdotV, roughnessT, roughnessB);
    return DV_SmithJointGGXAniso(TdotH, BdotH, NdotH, NdotV,
                                 TdotL, BdotL, NdotL,
                                 roughnessT, roughnessB, partLambdaV);
}

// Get projected roughness for a certain normalized direction V in tangent space
// and an anisotropic roughness
// Ref: Understanding the Masking-Shadowing Function in Microfacet-Based BRDFs, Heitz 2014, pp. 86, 88 - 39/60, 41/60
float GetProjectedRoughness(float TdotV, float BdotV, float NdotV, float roughnessT, float roughnessB)
{
    float2 roughness = float2(roughnessT, roughnessB);
    float sinTheta2 = max((1 - Sq(NdotV)), FLT_MIN);
    // if sinTheta^2 = 0, NdotV = 1, TdotV = BdotV = 0 and roughness is arbitrary, no real azimuth
    // as there's a breakdown of the spherical parameterization, so we clamp under by FLT_MIN in any case
    // for safe division
    // Note:
    //       sin(thetaV)^2 * cos(phiV)^2 = (TdotV)^2
    //       sin(thetaV)^2 * sin(phiV)^2 = (BdotV)^2
    float2 vProj2 = Sq(float2(TdotV, BdotV)) * rcp(sinTheta2);
    //       vProj2 = (cos^2(phi), sin^2(phi))
    float projRoughness = sqrt(dot(vProj2, roughness*roughness));
    return projRoughness;
}

//-----------------------------------------------------------------------------
// Diffuse BRDF - diffuseColor is expected to be multiply by the caller
//-----------------------------------------------------------------------------

real LambertNoPI()
{
    return 1.0;
}

real Lambert()
{
    return INV_PI;
}

real DisneyDiffuseNoPI(real NdotV, real NdotL, real LdotV, real perceptualRoughness)
{
    // (2 * LdotH * LdotH) = 1 + LdotV
    // real fd90 = 0.5 + (2 * LdotH * LdotH) * perceptualRoughness;
    real fd90 = 0.5 + (perceptualRoughness + perceptualRoughness * LdotV);
    // Two schlick fresnel term
    real lightScatter = F_Schlick(1.0, fd90, NdotL);
    real viewScatter = F_Schlick(1.0, fd90, NdotV);

    // Normalize the BRDF for polar view angles of up to (Pi/4).
    // We use the worst case of (roughness = albedo = 1), and, for each view angle,
    // integrate (brdf * cos(theta_light)) over all light directions.
    // The resulting value is for (theta_view = 0), which is actually a little bit larger
    // than the value of the integral for (theta_view = Pi/4).
    // Hopefully, the compiler folds the constant together with (1/Pi).
    return rcp(1.03571) * (lightScatter * viewScatter);
}

#ifndef BUILTIN_TARGET_API
real DisneyDiffuse(real NdotV, real NdotL, real LdotV, real perceptualRoughness)
{
    return INV_PI * DisneyDiffuseNoPI(NdotV, NdotL, LdotV, perceptualRoughness);
}
#endif

// Ref: Diffuse Lighting for GGX + Smith Microsurfaces, p. 113.
real3 DiffuseGGXNoPI(real3 albedo, real NdotV, real NdotL, real NdotH, real LdotV, real roughness)
{
    real facing = 0.5 + 0.5 * LdotV;              // (LdotH)^2
    real rough = facing * (0.9 - 0.4 * facing) * (0.5 / NdotH + 1);
    real transmitL = F_Transm_Schlick(0, NdotL);
    real transmitV = F_Transm_Schlick(0, NdotV);
    real smooth = transmitL * transmitV * 1.05;   // Normalize F_t over the hemisphere
    real single = lerp(smooth, rough, roughness); // Rescaled by PI
    real multiple = roughness * (0.1159 * PI);      // Rescaled by PI

    return single + albedo * multiple;
}

real3 DiffuseGGX(real3 albedo, real NdotV, real NdotL, real NdotH, real LdotV, real roughness)
{
    // Note that we could save 2 cycles by inlining the multiplication by INV_PI.
    return INV_PI * DiffuseGGXNoPI(albedo, NdotV, NdotL, NdotH, LdotV, roughness);
}

//-----------------------------------------------------------------------------
// Iridescence
//-----------------------------------------------------------------------------

// Ref: https://belcour.github.io/blog/research/2017/05/01/brdf-thin-film.html
// Evaluation XYZ sensitivity curves in Fourier space
real3 EvalSensitivity(real opd, real shift)
{
    // Use Gaussian fits, given by 3 parameters: val, pos and var
    real phase = 2.0 * PI * opd * 1e-6;
    real3 val = real3(5.4856e-13, 4.4201e-13, 5.2481e-13);
    real3 pos = real3(1.6810e+06, 1.7953e+06, 2.2084e+06);
    real3 var = real3(4.3278e+09, 9.3046e+09, 6.6121e+09);
    real3 xyz = val * sqrt(2.0 * PI * var) * cos(pos * phase + shift) * exp(-var * phase * phase);
    xyz.x += 9.7470e-14 * sqrt(2.0 * PI * 4.5282e+09) * cos(2.2399e+06 * phase + shift) * exp(-4.5282e+09 * phase * phase);
    xyz /= 1.0685e-7;

    // Convert to linear sRGb color space here.
    // EvalIridescence works in linear sRGB color space and does not switch...
    real3 srgb = mul(XYZ_2_REC709_MAT, xyz);
    return srgb;
}

// Evaluate the reflectance for a thin-film layer on top of a dielectric medum.
real3 EvalIridescence(real eta_1, real cosTheta1, real iridescenceThickness, real3 baseLayerFresnel0, real iorOverBaseLayer = 0.0)
{
    real3 I;

    // iridescenceThickness unit is micrometer for this equation here. Mean 0.5 is 500nm.
    real Dinc = 3.0 * iridescenceThickness;

    // Note: Unlike the code provide with the paper, here we use schlick approximation
    // Schlick is a very poor approximation when dealing with iridescence to the Fresnel
    // term and there is no "neutral" value in this unlike in the original paper.
    // We use Iridescence mask here to allow to have neutral value

    // Hack: In order to use only one parameter (DInc), we deduced the ior of iridescence from current Dinc iridescenceThickness
    // and we use mask instead to fade out the effect
    real eta_2 = lerp(2.0, 1.0, iridescenceThickness);
    // Following line from original code is not needed for us, it create a discontinuity
    // Force eta_2 -> eta_1 when Dinc -> 0.0
    // real eta_2 = lerp(eta_1, eta_2, smoothstep(0.0, 0.03, Dinc));
    // Evaluate the cosTheta on the base layer (Snell law)
    real sinTheta2Sq = Sq(eta_1 / eta_2) * (1.0 - Sq(cosTheta1));

    // Handle TIR:
    // (Also note that with just testing sinTheta2Sq > 1.0, (1.0 - sinTheta2Sq) can be negative, as emitted instructions
    // can eg be a mad giving a small negative for (1.0 - sinTheta2Sq), while sinTheta2Sq still testing equal to 1.0), so we actually
    // test the operand [cosTheta2Sq := (1.0 - sinTheta2Sq)] < 0 directly:)
    real cosTheta2Sq = (1.0 - sinTheta2Sq);
    // Or use this "artistic hack" to get more continuity even though wrong (no TIR, continue the effect by mirroring it):
    //   if( cosTheta2Sq < 0.0 ) => { sinTheta2Sq = 2 - sinTheta2Sq; => so cosTheta2Sq = sinTheta2Sq - 1 }
    // ie don't test and simply do
    //   real cosTheta2Sq = abs(1.0 - sinTheta2Sq);
    if (cosTheta2Sq < 0.0)
        I = real3(1.0, 1.0, 1.0);
    else
    {

        real cosTheta2 = sqrt(cosTheta2Sq);

        // First interface
        real R0 = IorToFresnel0(eta_2, eta_1);
        real R12 = F_Schlick(R0, cosTheta1);
        real R21 = R12;
        real T121 = 1.0 - R12;
        real phi12 = 0.0;
        real phi21 = PI - phi12;

        // Second interface
        // The f0 or the base should account for the new computed eta_2 on top.
        // This is optionally done if we are given the needed current ior over the base layer that is accounted for
        // in the baseLayerFresnel0 parameter:
        if (iorOverBaseLayer > 0.0)
        {
            // Fresnel0ToIor will give us a ratio of baseIor/topIor, hence we * iorOverBaseLayer to get the baseIor
            real3 baseIor = iorOverBaseLayer * Fresnel0ToIor(baseLayerFresnel0 + 0.0001); // guard against 1.0
            baseLayerFresnel0 = IorToFresnel0(baseIor, eta_2);
        }

        real3 R23 = F_Schlick(baseLayerFresnel0, cosTheta2);
        real  phi23 = 0.0;

        // Phase shift
        real OPD = Dinc * cosTheta2;
        real phi = phi21 + phi23;

        // Compound terms
        real3 R123 = clamp(R12 * R23, 1e-5, 0.9999);
        real3 r123 = sqrt(R123);
        real3 Rs = Sq(T121) * R23 / (real3(1.0, 1.0, 1.0) - R123);

        // Reflectance term for m = 0 (DC term amplitude)
        real3 C0 = R12 + Rs;
        I = C0;

        // Reflectance term for m > 0 (pairs of diracs)
        real3 Cm = Rs - T121;
        for (int m = 1; m <= 2; ++m)
        {
            Cm *= r123;
            real3 Sm = 2.0 * EvalSensitivity(m * OPD, m * phi);
            //vec3 SmP = 2.0 * evalSensitivity(m*OPD, m*phi2.y);
            I += Cm * Sm;
        }

        // Since out of gamut colors might be produced, negative color values are clamped to 0.
        I = max(I, float3(0.0, 0.0, 0.0));
    }

    return I;
}

//-----------------------------------------------------------------------------
// Fabric
//-----------------------------------------------------------------------------

// Ref: https://knarkowicz.wordpress.com/2018/01/04/cloth-shading/
real D_CharlieNoPI(real NdotH, real roughness)
{
    float invR = rcp(roughness);
    float cos2h = NdotH * NdotH;
    float sin2h = 1.0 - cos2h;
    // Note: We have sin^2 so multiply by 0.5 to cancel it
    return (2.0 + invR) * PositivePow(sin2h, invR * 0.5) / 2.0;
}

real D_Charlie(real NdotH, real roughness)
{
    return INV_PI * D_CharlieNoPI(NdotH, roughness);
}

real CharlieL(real x, real r)
{
    r = saturate(r);
    r = 1.0 - (1.0 - r) * (1.0 - r);

    float a = lerp(25.3245, 21.5473, r);
    float b = lerp(3.32435, 3.82987, r);
    float c = lerp(0.16801, 0.19823, r);
    float d = lerp(-1.27393, -1.97760, r);
    float e = lerp(-4.85967, -4.32054, r);

    return a / (1. + b * PositivePow(x, c)) + d * x + e;
}

// Note: This version don't include the softening of the paper: Production Friendly Microfacet Sheen BRDF
real V_Charlie(real NdotL, real NdotV, real roughness)
{
    real lambdaV = NdotV < 0.5 ? exp(CharlieL(NdotV, roughness)) : exp(2.0 * CharlieL(0.5, roughness) - CharlieL(1.0 - NdotV, roughness));
    real lambdaL = NdotL < 0.5 ? exp(CharlieL(NdotL, roughness)) : exp(2.0 * CharlieL(0.5, roughness) - CharlieL(1.0 - NdotL, roughness));

    return 1.0 / ((1.0 + lambdaV + lambdaL) * (4.0 * NdotV * NdotL));
}

// We use V_Ashikhmin instead of V_Charlie in practice for game due to the cost of V_Charlie
real V_Ashikhmin(real NdotL, real NdotV)
{
    // Use soft visibility term introduce in: Crafting a Next-Gen Material Pipeline for The Order : 1886
    return 1.0 / (4.0 * (NdotL + NdotV - NdotL * NdotV));
}

// A diffuse term use with fabric done by tech artist - empirical
real FabricLambertNoPI(real roughness)
{
    return lerp(1.0, 0.5, roughness);
}

real FabricLambert(real roughness)
{
    return INV_PI * FabricLambertNoPI(roughness);
}

real G_CookTorrance(real NdotH, real NdotV, real NdotL, real HdotV)
{
    return min(1.0, 2.0 * NdotH * min(NdotV, NdotL) / HdotV);
}

//-----------------------------------------------------------------------------
// Hair
//-----------------------------------------------------------------------------

//http://web.engr.oregonstate.edu/~mjb/cs519/Projects/Papers/HairRendering.pdf
real3 ShiftTangent(real3 T, real3 N, real shift)
{
    return normalize(T + N * shift);
}

// Note: this is Blinn-Phong, the original paper uses Phong.
real3 D_KajiyaKay(real3 T, real3 H, real specularExponent)
{
    real TdotH = dot(T, H);
    real sinTHSq = saturate(1.0 - TdotH * TdotH);

    real dirAttn = saturate(TdotH + 1.0); // Evgenii: this seems like a hack? Do we really need this?

                                           // Note: Kajiya-Kay is not energy conserving.
                                           // We attempt at least some energy conservation by approximately normalizing Blinn-Phong NDF.
                                           // We use the formulation with the NdotL.
                                           // See http://www.thetenthplanet.de/archives/255.
    real n = specularExponent;
    real norm = (n + 2) * rcp(2 * PI);

    return dirAttn * norm * PositivePow(sinTHSq, 0.5 * n);
}

#if SHADER_API_MOBILE || SHADER_API_GLES3 || SHADER_API_SWITCH
#pragma warning (enable : 3205) // conversion of larger type to smaller
#endif

#endif // UNITY_BSDF_INCLUDED