Numerically determine perturbation effects beyond the analytic approximation

Determine numerically the cosmological-perturbation dynamics and inflationary observables for the non-minimally coupled warm-inflation model when temperature-dependent dissipation coefficients and higher-order slow-roll effects are included, thereby characterizing the resulting running of spectral indices and non-Gaussianity.

Background

The analytic scalar power spectrum derived in the paper assumes a temperature-independent dissipation coefficient, negligible metric perturbations, and zeroth order in the slow-roll parameters. For temperature-dependent dissipation, the perturbation equations become coupled and generally require numerical treatment.

The authors note that the modified-gravity factor in the effective dissipation coefficient can produce field dependence not captured by standard power-law parametrizations. A more complete numerical analysis is therefore needed to determine the associated corrections and to compute higher-order observables, including the running of spectral indices and non-Gaussianity.

References

For these reasons, a more detailed numerical investigation of such effects is left for future work.

— Non-Minimally Coupled Warm Inflation in the Defining Frame  (2608.20293 - Casado-Turrión et al., 20 Aug 2026) in Section 3.2, paragraph following Eq. (fullpowerspectrum); Summary and Conclusions

Several questions remain unresolved. The possibility that gravitational waves acquire a thermal enhancement in warm inflation remains debated.

— Einstein-Gauss-Bonnet quintessential inflation: From super-inflation to emergent warm inflation  (2610.01665 - Chahboun et al., 1 Oct 2026) in Conclusion and comments, Section 6

The dissipation coefficient and the growth function are derived from numerical fits within general relativity; a self-consistent calculation is preferable.

— Einstein-Gauss-Bonnet quintessential inflation: From super-inflation to emergent warm inflation  (2610.01665 - Chahboun et al., 1 Oct 2026) in Conclusion and comments, Section 6