Scattering of multicomponent polymer blends

Abstract

The random phase approximation for polymer blends was developed by H. Benoît and described small angle scattering functions as well as mean field phase boundaries. It is a pure mean field theory that loses validity close to the real phase boundaries due to strong fluctuations. However, it gives a very clear roadmap about phase diagrams and scattering functions. A simplification of the random phase approximation is discussed that comes into effect when several polymers are mixed that involve a rather low number of chemically different repeat units. Then, the correlation functions of the same repeat unit pairs can be added up in a specific way such that the overall complexity for the calculations is reduced. The scattering functions and mean field phase boundaries are discussed within this concept.

Graphical abstract

Introduction

The random phase approximation is a mean field approach that is often applied to polymer blends [1,2,3]. It yields a simplified view on the scattering function and phase diagrams including interactions that neglects strong thermal composition fluctuations close to the phase transitions that can be of first or second order [4,5,6,7]. For binary homopolymer blends, it was the Flory-Huggins theory that described the mean field binodal and spinodal in a rather simple manner [8,9,10,11,12]. For this, entropic contributions were identified to arise from the translational entropy of placing polymers in a volume, and enthalpic contributions arise due to the monomer-monomer interactions. All of this was described on a cubic lattice. For the scattering functions [1,2,3], the undisturbed correlations play the role of entropy, while the interactions remain in this picture enthalpic (the independence of the scattering vector Q corresponds to local neighbor-neighbor interactions). Experimentally [4] and theoretically [13, 14], the interaction parameter displayed enthalpic and entropic properties that are due to monomeric structure and compressibility or free volume. However, the undisturbed correlations remained to be fully understood on the basis of the polymer architecture. For diblock copolymer blends, it was L. Leibler who introduced the mean field treatment and who predicted a phase diagram and a scattering function [15]. The strength of the mean field approach is that it can clearly give ideas about the scattering pattern and the phase diagram in a simplified way but for rather complicated polymer architectures and mixtures of them [16]. In this way, a simplified road map of a polymeric system is obtained that then could be refined by including strong fluctuations, either experimentally and/or theoretically. So for A/B/AB homopolymer/diblock copolymer blends, the group around F. Bates studies extensively the phase diagrams and scattering [17, 18]. Polymeric systems with many components are nowadays still highly interesting in the field of organic solar cells [19].

Theory

Let us consider P different polymers, being different either in architecture or in the making by chemically different monomers. I call N_i the degree of polymerization (number of repeat units) that enters in the molecular volume of the polymers V_i ∝ N_i and the radius of gyration R_g,i ∝ √N_i (i = 1..P). I call M_i the number of chemically different repeat unit species (monomers) of polymer species i (to some extent the number M_i could be the number of blocks, but in the later example of an ABA triblock copolymer M_i = 2 because I did not distinguish the A repeat units of the two blocks.) The overall number of chemically different repeat unit species of the whole set of polymers I call M.

The well-known formula of Benoit [1,2,3] is derived from a mean field approach applied to the scattering of polymers (polymer blends). It reads:

$$ \boldsymbol{S}={\left({\boldsymbol{S}}_0^{-1}+\boldsymbol{V}\right)}^{-1} $$

(1)

where S is the correlation matrix of the blended polymers, S₀ the correlation matrix of undisturbed polymers, and V the interaction matrix. Each row and column stands for a distinguishable repeat unit species (monomer) of a specific component (distinguishable polymer) that in principle can all be distinguished even if they are chemically identical (and then the interactions and scattering lengths will be the same in the respective positions of the matrices). So a system with P components (i.e. different polymers), where each polymer has M_i chemically different repeat unit species, would lead to a total dimensionality of ΣM_i for Eq. (1). I now want to extend the matrices in this sense that each single polymer can in principle carry correlations between all occurring chemically different repeat unit species, but the chemically same repeat unit species–even between different polymers–shall then be treated equally. The dimensionality of Eq. (1) becomes then PM (with M = max M_i in most cases). So there are undisturbed correlation matrices s_0,i that have the dimension from all chemically distinguishable repeat unit species. If the repeat units of a particular species do not appear in this component i, the corresponding entries are zero (or a small δ). On the higher level, S₀ is now a “diagonal” matrix with the entries of the s_0,i matrices:

$$ {S}_0=\left(\begin{array}{cccc}{s}_{0,1}& 0& \cdots & 0\\ {}0& {s}_{0,2}& \ddots & \vdots \\ {}\vdots & \ddots & \ddots & 0\\ {}0& \cdots & 0& {s}_{0,N}\end{array}\right) $$

(2)

where each polymer i is treated separately (i = 1..P), while the interaction matrix now looks like:

$$ V=\left(\begin{array}{ccc}v& \cdots & v\\ {}\vdots & \ddots & \vdots \\ {}v& \cdots & v\end{array}\right)=\left(\begin{array}{c}1\\ {}\vdots \\ {}1\end{array}\right)\left(1\kern0.5em \cdots \kern0.5em 1\right)\otimes v=\overrightarrow{1}\ {\overrightarrow{1}}^{\mathrm{tr}}\otimes v $$

(3)

where the latter expression is to be understood in the bracket writing that is frequently used in quantum mechanics (dyadic product). Let us call the vector $\overrightarrow{\mathbf{1}}$ that I do not normalize. All matrices S₀, V, s_0,i and v are Hermitian by definition. For a given vector of scattering length densities $\overrightarrow{b}$, I would obtain the final scattering function S(Q):

$$ S(Q)={\left(\overrightarrow{\mathbf{1}}\otimes \overrightarrow{b}\right)}^{\mathrm{tr}}{\left({\boldsymbol{S}}_0^{-1}+\boldsymbol{V}\right)}^{-1}\left(\overrightarrow{\mathbf{1}}\otimes \overrightarrow{b}\right) $$

(4)

From that I can expand the expression for large interactions v → ∞ (incompressibility):

$$ S(Q)={\left(\overrightarrow{\mathbf{1}}\otimes \overrightarrow{b}\right)}^{\mathrm{tr}}\left(\frac{1}{\boldsymbol{V}}-\frac{1}{\boldsymbol{V}{\boldsymbol{S}}_0\boldsymbol{V}}+\frac{1}{\boldsymbol{V}{\boldsymbol{S}}_0\boldsymbol{V}{\boldsymbol{S}}_0\boldsymbol{V}}-\cdots \right)\left(\overrightarrow{\mathbf{1}}\otimes \overrightarrow{b}\right) $$

(5)

From the bracket writing of the interaction matrix, I then obtain:

$$ S(Q)={\left(\overrightarrow{\mathbf{1}}\otimes \overrightarrow{b}\right)}^{\mathrm{tr}}\left(\frac{1}{\overrightarrow{\mathbf{1}}\ {\overrightarrow{\mathbf{1}}}^{\mathrm{tr}}\otimes \boldsymbol{v}}-\frac{1}{\overrightarrow{\mathbf{1}}\ {\overrightarrow{\mathbf{1}}}^{\mathrm{tr}}\otimes \boldsymbol{v}{\boldsymbol{s}}_{0,+}\boldsymbol{v}}+\frac{1}{\overrightarrow{\mathbf{1}}\ {\overrightarrow{\mathbf{1}}}^{\mathrm{tr}}\otimes \boldsymbol{v}{\boldsymbol{s}}_{0,+}\boldsymbol{v}{\boldsymbol{s}}_{0,+}\boldsymbol{v}}-\cdots \right)\left(\overrightarrow{\mathbf{1}}\otimes \overrightarrow{b}\right) $$

(6)

with

$$ {\boldsymbol{s}}_{0,+}=\sum {\boldsymbol{s}}_{0,i} $$

(7)

For the reciprocal matrix of V, i.e. the first term, I obtain:

$$ {\left(\overrightarrow{\mathbf{1}}\otimes \overrightarrow{b}\right)}^{\mathrm{tr}}\frac{1}{\boldsymbol{V}}\left(\overrightarrow{\mathbf{1}}\otimes \overrightarrow{b}\right)={\left(\overrightarrow{\mathbf{1}}\otimes \overrightarrow{b}\right)}^{\mathrm{tr}}\left(\frac{1}{P^2}\overrightarrow{\mathbf{1}}\ {\overrightarrow{\mathbf{1}}}^{\mathrm{tr}}\otimes {\boldsymbol{v}}^{-\mathbf{1}}+\sum {\overrightarrow{\boldsymbol{r}}}_{\boldsymbol{i}}{\overrightarrow{\boldsymbol{r}}}_{\boldsymbol{i}}^{\mathrm{tr}}\otimes {\boldsymbol{\varepsilon}}_{\boldsymbol{i}}^{-\mathbf{1}}\right)\left(\overrightarrow{\mathbf{1}}\otimes \overrightarrow{b}\right)={\overrightarrow{b}}^{\mathrm{tr}}{\boldsymbol{v}}^{-\mathbf{1}}\overrightarrow{b} $$

(8)

The normalization by the number of polymer components P is due to the fact that the vector $\overrightarrow{\mathbf{1}}$ remains to be normalized. The vectors ${\overrightarrow{\boldsymbol{r}}}_{\boldsymbol{i}}$ are normalized and orthogonal to $\overrightarrow{\mathbf{1}}$, and they altogether span the full vector space. The rather large contributions deviating from the vector $\overrightarrow{\mathbf{1}}$ and involving ε_i become zero in the projection. Now applying this technique to all terms, the final expression is

$$ S(Q)={\overrightarrow{b}}^{\mathrm{tr}}{\left({\boldsymbol{s}}_{0,+}^{-1}+\boldsymbol{v}\right)}^{-\mathbf{1}}\overrightarrow{b} $$

(9)

This simplification becomes evident if the different polymers include many chemically identical repeat units such that they are not distinguished in the final expression anymore. The dimensionality of Eq. 9 is now M. A simplification is reached when M < ΣM_i.

Examples

One example could be a mixture of a homopolymer A, an AB diblock copolymer and a symmetric (or telechelic) ABA triblock copolymer that all consist of repeat units of type A and/or B. Then, the final expression looks like [20]:

$$ {\boldsymbol{s}}_{0,+}={\boldsymbol{s}}_{01}+{\boldsymbol{s}}_{02}+{\boldsymbol{s}}_{03} $$

(10)

with the undisturbed correlation matrices:

$$ {s}_{01}={\phi}_1{V}_1\left(\begin{array}{cc}{g}_1& 0\\ {}0& 0\end{array}\right) $$

(11)

$$ {s}_{02}={\phi}_2{V}_2\left(\begin{array}{cc}{g}_{f_2}& \frac{1}{2}\left({g}_1-{g}_{f_2}-{g}_{1-{f}_2}\right)\\ {}\frac{1}{2}\left({g}_1-{g}_{f_2}-{g}_{1-{f}_2}\right)& {g}_{1-{f}_2}\end{array}\right) $$

(12)

$$ {s}_{03}={\phi}_3{V}_3\left(\begin{array}{cc}2{g}_{f_3}+{g}_1+{g}_{1-2{f}_3}-2{g}_{1-{f}_3}& {g}_{1-{f}_3}-{g}_{f_3}-{g}_{1-2{f}_3}\\ {}{g}_{1-{f}_3}-{g}_{f_3}-{g}_{1-2{f}_3}& {g}_{1-2{f}_3}\end{array}\right) $$

(13)

with the volume fractions ϕ_i and the molar volumes V_i of all polymers and the modified Debye functions ${g}_f(x)=\frac{2}{x^2}\left(\exp \left(- fx\right)-1+ fx\right)$ with $x={Q}^2{R}_{\mathrm{g},i}^2$. The magnitude Q is the scattering vector, and R_g,i is the radius of gyration of the whole respective polymer. The fractions of block A in the three polymers are 1, f₂ and f₃, where the latter measures the single end-block that occurs at either end and thus must be smaller than ½. Equation (12 and (13 can be obtained by shifting the integration limits of the correlation functions, and so all expressions are sums of Debye functions. This polymeric system was motivated in a study of a bad batch of diblock copolymers, where on the one hand homopolymers were left from an incomplete functionalization for the second block and triblock copolymers occurred due to the presence of oxygen in the termination such that two B-blocks were linked together [20]. For simplicity, I can assume f₂ = ½ and f₃ = ¼. In this two-dimensional case (with only repeat units of type A and B), the additional simplification can be made as a result of incompressibility (v_AA, v_BB, v_AB large and negative):

$$ S(Q)=\frac{\Delta {\rho}^2}{\frac{\mathrm{sum}\ {\boldsymbol{s}}_{0,+}}{\det\ {\boldsymbol{s}}_{0,+}}-2\chi } $$

(14)

with the sum over all matrix elements in sum s_0,+ and the interaction parameter $\chi =\frac{\det \boldsymbol{v}}{2\ \overline{v_{i,j}}}=\frac{1}{2}\left(2{v}_{A,B}-{v}_{A,A}-{v}_{B,B}\right)$ and the contrast Δρ². The whole formula is valid for large matrix elements v_i,j. In linear chains, the sum over all matrix elements in s_0,+ is connected to whole chain scattering ~g₁. This formula has been found many times in the literature [3, 21].

For clarity, I calculated the scattering functions for the three materials and their mixtures. The molar volumes of an A and/or B block were assumed to be 20.,000 cm³/mol (only in the triblock the B-block was double this size). The f-values were f₂ = ½ and f₃ = ¼. The radii of gyration were connected to values for poly butylene oxide [22] as an example (R_g1 = 32Å, R_g2 = 45Å, R_g3 = 63Å), and the compositions were ϕ₁ = 0.1, ϕ₂ = 0.8 and ϕ₃ = 0.1. We can see the scattering functions in Fig. 1. All scattering is obtained by dividing by the contrast Δρ. For the homopolymer, I multiplied by the composition ϕ₁ = 0.1. Otherwise for the pure components, I assumed the compositions ϕ_i = 1. We can see that the peak of the mixture lies between the diblock and triblock copolymer, and the forward scattering is elevated due to the presence of homopolymer (A composition can fluctuate at long length scales), while the block copolymers display the correlation hole at long length scales (no fluctuations at long length scales due to the covalent bond between A and B).

Fig. 1

The scattering functions of a homopolymer, a diblock copolymer and a triblock copolymer and the resulting one of a mixture, all with no preferable interaction, i.e. χ = 0

In the next example, the interaction parameter is χ = 0.0001 mol/cm³ (see Fig. 2). Furthermore, the original formulation with extended dimensions (Eqs. (1)–(3), see Appendix (16)–(23)) is tested against the final formulation (Eqs. (10)–(14)) with a transition of compressibility, i.e. v_AA = v_BB = 0.001 over 0.01 mol/cm³ to ∞ and the respective v_AB = v_AA + χ. For a rather compressible system (stage 1), a nearly constant contribution is added to the scattering of the incompressible system. This additive contribution becomes smaller for a less compressible system (stage 2). Finally, the incompressible system does not show any numerically significant differences between the different formulations of Eqs. (16)–(18) (Appendix) vs. Eq. (14). So, the numerical calculations also prove the validity of Eq. (14) with reduced dimensions in the limit of incompressibility.

Fig. 2

The scattering function of a mixture of an A-homopolymer, an A-B diblock copolymer and an A-B-A triblock copolymer (see text) with a finite interaction parameter χ = 0.0001 mol/cm³. Additionally, the monomer-monomer interactions are rendered from v_AA = v_BB = 0.001 (stage 1) over 0.01 mol/cm³ (stage 2) to ∞ (and the respective v_AB = v_AA + χ) to simulate different states of compressibility

The diblock copolymer that the model was developed for was a polybutadiene-polyisoprene (Fig. 3) with impurities [20]. The model could easily be adapted by changing the homopolymer fraction to 30% and the diblock copolymer fraction to 60%. The radii of gyration were multiplied by 5, the interaction parameter was χ = 0.000047 mol/cm³, and the molar volume was 3.7 x 10⁵ cm³/mol. As one can see, the model describes the scattering very well. The high amount of homopolymer is in the range measured by a GPC/SEC trace. However, the polydispersity of the block fraction f could also contribute to the high scattering level at lowest Q. We discuss polydispersity further below.

Fig. 3

The measured polybutadiene-polyisoprene (d-PB(1,4)-PI) diblock copolymer at 130°C with a molar mass of 350 kg/mol as described with the model. The homopolymer fraction was 30%. The interaction parameter was χ = 0.000047 mol/cm³. The set of radii of gyration was 5 times larger

Generally, mean field phase diagrams, i.e. the spinodals, can be obtained by finding the zeros of the determinant:

$$ \det\ \left({\boldsymbol{s}}_{0,+}^{-1}+\boldsymbol{v}\right)=0 $$

(15)

By the analysis, which vector leads to the zero of the determinant, one can distinguish the type of phase separation [16, 23]. An example was the blend of an AB and an BC diblock copolymer, where the indices follow the order A, B, C. Then, the vector (1,0,−1)/√2 at the critical scattering vector Q* = 0 indicates macrophase separation, and another vector including components of (1, 2, 1)/√6 at a critical scattering vector Q* > 0 indicates microphase separation. The periodicity of the phase-separated domains is given by d = 2π/Q*. When the two conditions merge at a single point, the Lifshitz critical point is obtained. Here, the macrophase and microphase separations are indistinguishable. However, in the practical examples, this behavior has not been observed [19]. Another example for a Lifshitz criticality is the mixture of A/B homopolymers with AB diblock copolymers [24, 25]. This criticality leads to a formation of bicontinuous microemulsion domain structures that extend to quite low temperatures. It has to be mentioned that the quite severe extension of the microemulsion phase is due to the presence of strong fluctuations that are neglected by the mean field approach discussed here.

In the example system, for which I calculated the scattering functions, all matrices become 2-dimensional, and a further simplification applies: The denominator of Eq. 14 must become zero at the mean field phase boundary, and so values of the interaction parameter χ can be calculated for the Q-value zero and at the minimum Q* of sum s_0,+ / det s_0,+. The two phase boundaries and the values of Q* are depicted in Fig. 4. The phase boundary connected to Q = 0 is the spinodal of the macrophase separation and the other one the order-disorder phase transition (i.e. microphase transition). As a system, we assumed that the A homopolymer has a constant molar volume of V₁ = 20.,000 cm³/mol, while the A block molar volumes vary with the f-value (f₃ = f₂/2).

Fig. 4

Phase diagram of an A-homopolymer, an A-B diblock copolymer and an A-B-A triblock copolymer (see text). The molar volume of the A-homopolymer of 20.,000 cm³/mol is constant while the molar volumes of the A-blocks vary according to the f-value, i.e. f₂=f and f₃=f/2.

It should be stressed that the equations above hold for one-phase disordered systems. So, if the phase boundary is crossed, the approach is invalid and does not predict the scattering function anymore. Good comparisons between calculations and experiments can be found in [21].

The simplification of reduced dimensions as expressed in Eqs. (9) and (15) was already implicitly used for polydisperse systems [26, 27], where one simply argues that the different components due to the polydispersity are such similar that this simplified approach is valid. However, I argue that even very different polymers can lead to the simplified expressions as mentioned in this paper.

Conclusions

The final theoretical result of this paper is given in Eqs. (7) and (9). It reduces the unnecessary dimensions of the correlations that may arise if chemically same repeat units on different polymers are distinguished. I presented a calculation on how these dimensions can be minimized, although the intermediate matrices are expanded to dimension n × n = (PM) × (PM), with P being the number of different polymers and M being the overall number of all chemically different repeat units involved. The final formula reduces the matrices to a dimension M × M. An example for a blend of an A homopolymer, an AB diblock copolymer and a symmetric ABA triblock copolymer is discussed explicitly. We displayed scattering functions and a mean field phase diagram. Other examples of AB and BC diblock copolymer blends and A/B homopolymer blends with AB diblock copolymers are discussed peripherally and are referred to the cited literature.

Appendix

For the example system of the three polymers, an A homopolymer, an AB diblock copolymer and an ABA triblock copolymer (Eqs. (11)–(13)), we explicitly show the simplification. The original correlation matrix S₀ is then:

$$ {\boldsymbol{S}}_0=\left(\begin{array}{cccccc}{\phi}_1{V}_1{g}_1& 0& 0& 0& 0& 0\\ {}0& \delta & 0& 0& 0& 0\\ {}0& 0& {\phi}_2{V}_2{g}_{f_2}& \frac{1}{2}{\phi}_2{V}_2\left({g}_1-{g}_{f_2}-{g}_{1-{f}_2}\right)& 0& 0\\ {}0& 0& \frac{1}{2}{\phi}_2{V}_2\left({g}_1-{g}_{f_2}-{g}_{1-{f}_2}\right)& {\phi}_2{V}_2{g}_{1-{f}_2}& 0& 0\\ {}0& 0& 0& 0& {\phi}_3{V}_3\left(2{g}_{f_3}+{g}_1+{g}_{1-2{f}_3}-2{g}_{1-{f}_3}\right)& {\phi}_3{V}_3\left({g}_{1-{f}_3}-{g}_{f_3}-{g}_{1-2{f}_3}\right)\\ {}0& 0& 0& 0& {\phi}_3{V}_3\left({g}_{1-{f}_3}-{g}_{f_3}-{g}_{1-2{f}_3}\right)& {\phi}_3{V}_3{g}_{1-2{f}_3}\end{array}\right) $$

(16)

The interaction matrix reads then:

$$ \boldsymbol{V}=\left(\begin{array}{cccccc}{v}_{A,A}& {v}_{A,B}& {v}_{A,A}& {v}_{A,B}& {v}_{A,A}& {v}_{A,B}\\ {}{v}_{A,B}& {v}_{B,B}& {v}_{A,B}& {v}_{B,B}& {v}_{A,B}& {v}_{B,B}\\ {}{v}_{A,A}& {v}_{A,B}& {v}_{A,A}& {v}_{A,B}& {v}_{A,A}& {v}_{A,B}\\ {}{v}_{A,B}& {v}_{B,B}& {v}_{A,B}& {v}_{B,B}& {v}_{A,B}& {v}_{B,B}\\ {}{v}_{A,A}& {v}_{A,B}& {v}_{A,A}& {v}_{A,B}& {v}_{A,A}& {v}_{A,B}\\ {}{v}_{A,B}& {v}_{B,B}& {v}_{A,B}& {v}_{B,B}& {v}_{A,B}& {v}_{B,B}\end{array}\right) $$

(17)

The original formula to be calculated, now including the scattering length densities b_A and b_B would finally read:

$$ S(Q)={\left({b}_A\kern0.5em {b}_B\kern0.5em {b}_A\kern0.5em {b}_B\kern0.5em {b}_A\kern0.5em {b}_B\right)\left({\boldsymbol{S}}_0^{-1}+\boldsymbol{V}\right)}^{-1}\left(\begin{array}{c}{b}_A\\ {}{b}_B\\ {}{b}_A\\ {}{b}_B\\ {}{b}_A\\ {}{b}_B\end{array}\right) $$

(18)

The calculation in a computer would not face large difficulties. However, the envisaged analytical simplifications provide a better insight and errors can be found easier. So the sum of the 2 × 2 correlation matrices reads:

$$ {\boldsymbol{s}}_{0,+}=\left(\begin{array}{cc}{\phi}_1{V}_1{g}_1+{\phi}_2{V}_2{g}_{f_2}+{\phi}_3{V}_3\left(2{g}_{f_3}+{g}_1+{g}_{1-2{f}_3}-2{g}_{1-{f}_3}\right)& \frac{1}{2}{\phi}_2{V}_2\left({g}_1-{g}_{f_2}-{g}_{1-{f}_2}\right)+{\phi}_3{V}_3\left({g}_{1-{f}_3}-{g}_{f_3}-{g}_{1-2{f}_3}\right)\\ {}\frac{1}{2}{\phi}_2{V}_2\left({g}_1-{g}_{f_2}-{g}_{1-{f}_2}\right)+{\phi}_3{V}_3\left({g}_{1-{f}_3}-{g}_{f_3}-{g}_{1-2{f}_3}\right)& {\phi}_2{V}_2{g}_{1-{f}_2}+{\phi}_3{V}_3{g}_{1-2{f}_3}\end{array}\right) $$

(19)

and the interaction matrix reads:

$$ \boldsymbol{v}=\left(\begin{array}{cc}{v}_{A,A}& {v}_{A,B}\\ {}{v}_{A,B}& {v}_{B,B}\end{array}\right) $$

(20)

So, the general result in terms of a simplified Benoit theory (Eq. 9) would arrive at:

$$ S(Q)=\left({b}_A\kern0.5em {b}_B\right){\left({\boldsymbol{s}}_{0,+}^{-1}+\boldsymbol{v}\right)}^{-1}\left(\begin{array}{c}{b}_A\\ {}{b}_B\end{array}\right) $$

(21)

The final scattering formula, assuming incompressibility, would now read (as in Eq. 14):

$$ S(Q)=\frac{\Delta {\rho}^2}{\frac{\mathrm{sum}\ {\boldsymbol{s}}_{0,+}}{\det\ {\boldsymbol{s}}_{0,+}}-2\chi } $$

(22)

Note that we call Δρ = b_A − b_B. As a cross check, we obtain for the sum of all entries from s_0,+ the single chain scattering:

$$ \mathrm{sum}\ {\boldsymbol{s}}_{0,+}={\phi}_1{V}_1{g}_1+{\phi}_2{V}_2{g}_1+{\phi}_3{V}_3{g}_1 $$

(23)

Please note that the entries for the radii of gyration to the terms g₁(QR_g,i) may be different in the three addends. So the only remaining difficult term is the determinant of s_0,+, which introduces products of correlations.