The name is absent

For the arm segments, initiator to the I2 function is

ŋɪθ = J ⅛'exp[B_c(r')] [Ar(r'ψ-¹ A^(c’^m)(r, r').          (7.32)

And,
ŋr) = / *'exp[‰ι(r')]∕₂^a,^ι(r')∆^+¹∖r,r^z).        (7.33)

The ʃɪ function for the arm segments is

ʃɪɪ(r) = 1,

∕‰^m(r) = / ^dr' exp[Bα-ι(r')]∕ι^α^₁(r^,)Δ^-¹^(r,r').         (7.34)

Finally, the density profile of the arm segment ⁱa^, in terms of ʃɪ and T₂ functions is
given as

pɑ(r) = exp(⅛) exp[P_α(r)]∕₁^o7(r)∕₂-^m(r).             (7.35)

This is physically depicted in fig. 7.2b.

Picard-type iteration method is applied to solve the set of eqs. 7.31 and 7.35 for
the density profile of the articulation and the arm segments of the star polymer. For
the systems considered in this work, the inhomogeneity is only in one dimension (z).
All the numerical integrations are done using the trapezoidal rule.

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