We have recorded threshold photoelectron spectra of HF and DP over the oute
r valence ionization region under good resolution conditions (3-6 meV) usin
g synchrotron radiation and employing the penetrating-field electron detect
ion technique. The spectra show extensive vibrational structure in the X(2
Pi(i)) system in the first Franck-Condon gap region that is attributed to r
esonance autoionization of Rydberg states lying in this energy range. The R
ydberg states responsible for these effects are identified as [A((2)Sigma())]ns sigma (1)Sigma(+), with n = 4-6. Analyses of all the vibrational data
contained in these spectra for the X ((2)Pi(i)) state using a modified iso
topic vibrational Dunham equation have led to greatly improved spectroscopi
c constants for this state in HF+ and DF+. The same method was also used to
determine improved spectroscopic constants for the A((2)Sigma(+)) state. A
utoionization is found not to be important in the formation of the A(2 Sigm
a+) state due to the absence of Rydberg states in the energy region of the
A state. Based on the observations and interpretations of the present work,
combined with literature data, we have constructed a potential-energy diag
ram of the relevant states of HF and HF+. Partially rotationally resolved t
hreshold photoelectron spectra of HF+ and DF+ over the nu(+) = 0 vibrationa
l band of the X (2)Pi(i) system show pronounced effects due to autoionizati
on processes.