gcbryan is right; a bigger diameter does not at all need a bigger reflector for throw per se.
Actually the SST-90, the biggest one, can compete with, say, the XP-E in 'surface brightness', and both would throw equally well with the same reflector or lens - the XP-E @ 1A, the SST-90 @ 9A, that is. The SST-90 would give a spot 9 times as big as the XP-E, containing 9 times as much light (luminous flux), but with the same intensity, thus with the same throw.
A larger reflector isn't even more efficient (or only a negligible bit), defining efficiency here as percentage of light going into the spot instead of the spill. Efficiency in that sense only depends on the aperture angle of the reflector or lens; it's about 75% for a typical reflector with ~60° full opening angle - for a reflector. A typical 60°-lens gets the forward 25%...
XM-L U2 has about 30% less emittance ('surface brightness') than the XR-E R2 EZ900, which is the king in that respect - those data are according to the specs, i.e. at their specific max current and at 25°C junction temperature...
The viewing angle does have some influence - but not the specified full-width-at-half-maximum (FWHM) viewing angle, but instead the maximum viewing angle, which is ~180° for all XP-*, XM-L and SST-*0 - but only about 120° for the XP-*, caused by those LEDs' collar. That causes a bigger 'dead hole', that is the center part of the reflector not hit by the LED light. That area does not contribute to throw then. With aspheric lenses the viewing angle has *no* direct influence on throw.
oldbobk, absorption in the lens usually is rather negligible unless you use really low quality lenses. The gain from diameter is much higher: 30% more diameter for example will yield ~70% more spot intensity!
agenthex: That equation only holds under the condition of a constant aperture angle; in that case the bigger aperture area S comes with a bigger focal length, and it is that focal length that reduces the beam divergence alpha. With a single (aspheric) lens, alpha=arctan(s/2f), or just s/2f for small angles, where s is the apparent LED diameter and f is the focal length. You can produce a *very* thin beam with, say, XP-G and an f=25cm lens of only 20mm diameter, f counts, not the diameter. *Much* losses though.