  The neutron-rich $^{28,29}$F isotopes have been recently studied via knockout
and interaction cross-section measurements. The $2n$ halo in $^{29}$F has been
linked to the occupancy of $pf$ intruder configurations. We investigate bound
and continuum states in $^{29}$F, focusing on the $E1$ response of low-lying
excitations and the effect of dipole couplings on nuclear reactions.
$^{29}\text{F}$ ($^{27}\text{F}+n+n$) wave functions are built within the
hyperspherical harmonics formalism, and reaction cross sections are calculated
using the Glauber theory. Continuum states and $B(E1)$ transition probabilities
are described in a pseudostate approach using the analytical THO basis. The
corresponding structure form factors are used in CDCC calculations to describe
low-energy scattering. Parity inversion in $^{28}$F leads to a $^{29}$F ground
state characterized by 57.5% of $(p_{3/2})^2$ intruder components, a strong
dineutron configuration, and an increase of the matter radius with respect to
the core radius of $\Delta R=0.20$ fm. Glauber-model calculations for a carbon
target at 240 MeV/nucleon provide a total reaction cross section of 1370 mb, in
agreement with recent data. The model produces also a barely bound excited
state corresponding to a quadrupole excitation. $B(E1)$ calculations into the
continuum yield a total strength of 1.59 e$^2$fm$^2$ up to 6 MeV, and the $E1$
distribution exhibits a resonance at $\approx$ 0.85 MeV. Results using a
standard shell-model order for $^{28}$F lead to a considerable reduction of the
$B(E1)$ distribution. The four-body CDCC calculations for
$^{29}\text{F}+^{120}\text{Sn}$ around the Coulomb barrier are dominated by
dipole couplings, which totally cancel the Fresnel peak in the elastic cross
section. These results are consistent with a two-neutron halo and may guide
future experimental campaigns.
