Abstract
Specific examples are given of artifacts in photoionization‐efficiency curves that result from the use of a discrete‐line light source. A comparative technique is used to distinguish this false structure from genuine structure marking energy levels above the ionization potential (I.P.). More accurate I.P.'s than previously available are given for HCl, CH3Cl, CH3NO2, CH3CN, C2H4, C3H6, C2H2 and new values for CH4, CD4, C2H6, C3H8.