We compute CBR anisotropies in mixed models with different hot components,
including neutrinos or volatile HDM arising from the decay of heavier
particles. The CBR power spectra of these models exhibit a higher doppler peak
than CDM, and the discrepancy is even stronger in volatile models when the
decay gives rise also to a neutral scalar. CBR experiments, together with Large
Scale Structure (LSS) data, are then used to constrain the space parameter of
mixed models, when values of the primeval spectral index n > 1 are also
considered. Even if n>1 is allowed, however, LSS alone prescribes that \Omega_h
\mincir 0.30. LSS can be fitted by taking simultaneously a low derelativization
redshift z_der (down to \simeq 600) and a high n, while CBR data from
baloon--borne experiment cause a severe selection on this part of the parameter
space. In fact, while late derelativization and n>1 have opposite effects on
the fluctuation spectrum P(k), they sum their action on the angular spectrum
C_l. Henceforth n \magcir 1.3 seems excluded by baloon--borne experiment
outputs, while a good fit of almost all CBR and LSS data is found for Omega_h
values between 0.11 and 0.16, n \sim 1.1 and z_der \sim 2000--5000. A smaller n
is allowed, but z_der should never be smaller than \simeq 1200.Comment: 13 pages, 15 figures, uses mn.sty, submitted to MNRA