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Table 1 Parameters used during numerical experiment

From: An inertial-type algorithm for approximation of solutions of Hammerstein integral inclusions in Hilbert spaces

BOY (3.1)

MM (1.17)

CS12 (4.1)

CS13 (4.2)

S14 (4.3)

\(\lambda _{n} = (n+1)^{-\frac{1}{4}}\)

\(\lambda _{n} = (n+1)^{-\frac{1}{4}}\)

\(\beta _{n} = (n+1)^{-1}\)

\(\lambda _{n} = (n+1)^{-\frac{1}{4}}\)

\(\beta _{n} = (n+1)^{-1}\)

\(\theta _{n} = (n+1)^{-\frac{1}{5}}\)

\(\theta _{n} = (n+1)^{-\frac{1}{5}}\)

 

\(\theta _{n} = (n+1)^{-\frac{1}{5}}\)

 
   

\(\alpha _{n} = (n+1)^{-\frac{1}{4}}\)

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