This study presents a novel measurement, and simulation, of the time-resolved room temperature chlorophyll a £uorescence emission spectra from leaves of the barley wild-type and chlorophyll-b-de¢cient chlorina (clo) f 2 and f104 mutants. The primary data were collected with a streak-camera-based picosecond-pulsed £uorometer that simultaneously records the spectral distribution and time dependence of the £uorescence decay. A new global spectral-kinetic analysis programme method, termed the double convolution integral (DCI) method, was developed to convolve the exciting laser pulse shape with a multimodal-distributed decay pro¢le function that is again convolved with the spectral emission band amplitude functions. We report several key results obtained by the simultaneous spectral-kinetic acquisition and DCI methods. First, under conditions of dark-level £uorescence, when photosystem II (PS II) photochemistry is at a maximum at room temperature, both the clo f 2 and clo f104 mutants exhibit very similar PS II spectral-decay contours as the wild-type (wt), with the main band centred around 685 nm. Second, dark-level £uorescence is strongly in£uenced beyond 700 nm by broad emission bands from PS I, and its associated antennae proteins, which exhibit much more rapid decay kinetics and strong integrated amplitudes. In particular a 705^720 nm band is present in all three samples, with a 710 nm band predominating in the clo f 2 leaves. When the PS II photochemistry becomes inhibited, maximizing the £uorescence yield, both the clo f104 mutant and the wt exhibit lifetime increases for their major distribution modes from the minimal 250^500 ps range to the maximal 1500^2500 ps range for both the 685 nm and 740 nm bands. The clo f 2 mutant, however, exhibits several unique spectral-kinetic properties, attributed to its unique PS I antennae and thylakoid structure, indicating changes in both PS II £uorescence reabsorption and PS II to PS I energy transfer pathways compared to the wt and clo f104. Photoprotective energy dissipation mediated by the xanthophyll cycle pigments and the PsbS protein was uninhibited in the clo f 104 mutant but, as commonly reported in the literature, signi¢cantly inhibited in the clo f 2; the inhibited energy dissipation is partly attributed to its thylakoid structure and PS II to PS I energy transfer properties. It is concluded that it is imperative with steady-state £uorometers, especially for in vivo studies of PS II e¤ciency or photoprotective energy dissipation, to quantify the in£uence of the PS I spectral emission.