  In this sequel to our work on triply excited hollow resonances in
three-electron atomic systems, a density functional theory (DFT)-based
formalism is employed to investigate similar resonances in Li-isoelectronic
series (Z=4--10). A combination of the work-function-based local nonvariational
exchange potential and the popular gradient plus Laplacian included
Lee-Yang-Parr correlation energy functional is used. First, all the 8 n=2
intrashell states of B$^{2+}$, N$^{4+}$ and F$^{6+}$ are presented, which are
relatively less studied in the literature compared to the remaining 4 members.
Then calculations are performed for the 8 $2l2l'$n$l"$ (3$\leq$n$\leq$6) hollow
resonance series; {\em viz.,} 2s$^2$ns $^2$S$^e$, 2s$^2$np $^2$P$^o$, 2s$^2$nd
$^2$D$^e$, 2s2pns $^4$P$^o$, 2s2pnp $^4$D$^e$, 2p$^2$ns $^4$P$^e$, 2p$^2$np
$^4$D$^o$ and 2p$^2$ns $^2$D$^e$, of all the 7 positive ions. Next, as an
illustration, higher resonance positions of the 2s$^2$ns $^2$S$^e$ series are
calculated for all the ions with a maximum of n=25. The excitation energies
calculated from this single-determinantal approach are in excellent agreement
with the available literature data (for the n=2 intrashell states the deviation
is within 0.125% and excepting only one case, the same for the resonance series
is well below 0.50%). With an increase in Z, the deviations tend to decrease.
Radial densities are also presented for some of the selected states. The only
result available in the literature for the lower resonances (corresponding to a
maximum of n=17) have been reported very recently. The n$>$16 ($>17$ for
F$^{6+}$) resonances are examined here for the first time. This gives a
promising viable and general DFT scheme for the accurate calculation of these
and other hollow resonances in many-electron atoms.
