Planck 2015 results
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Table 24

Constraints on models with excited initial states (non-Bunch-Davies models), as well as warm inflation.

SMICA SEVEM NILC Commander

Flattened-type model A ± σA S / N A ± σA S / N A ± σA S / N A ± σA S / N

Flat model T-only 49 ± 65 0.8 57 ± 65 0.9 47 ± 65 0.7 19 ± 65 0.3
Flat model T+E 44 ± 37 1.2 70 ± 37 1.9 33 ± 37 0.9 47 ± 37 1.3
Non-Bunch-Davies T-only 42 ± 82 0.5 53 ± 82 0.6 26 ± 82 0.3 17 ± 82 0.2
Non-Bunch-Davies T+E 61 ± 47 1.3 76 ± 47 1.6 43 ± 47 0.9 58 ± 47 1.2
NBD sine T-only 567 ± 341 1.7 513 ± 341 1.5 588 ± 341 1.7 604 ± 341 1.8
NBD sine T+E 387 ± 206 1.9 485 ± 218 2.2 425 ± 206 2.1 417 ± 210 2.0
NBD1 cos flattened T-only 10 ± 22 0.5 4 ± 22 0.2 8 ± 22 0.4 9 ± 22 0.4
NBD1 cos flattened T+E 20 ± 19 1.1 10 ± 19 0.5 19 ± 19 1.0 14 ± 19 0.8
NBD2 cos squeezed T-only 10 ± 17 0.6 10 ± 17 0.6 8 ± 17 0.5 2.5 ± 17 0.1
NBD2 cos squeezed T+E 3 ± 5 0.5 0.8 ± 5.5 0.1 4 ± 5 0.8 3.8 ± 5.5 0.7
NBD1 sin flattened T-only 25 ± 22 1.1 27 ± 22 1.2 18 ± 22 0.8 33 ± 23 1.4
NBD1 sin flattened T+E 48 ± 30 1.6 49 ± 33 1.5 35 ± 31 1.1 26 ±34 0.8
NBD2 sin squeezed T-only 2.0 ± 1.4 1.4 1.4 ± 1.4 1.0 1.6 ± 1.4 1.1 1.3 ± 1.4 0.9
NBD2 sin squeezed T+E 0.8 ± 0.4 1.9 0.5 ± 0.4 1.2 0.6 ± 0.4 1.4 0.5 ± 0.4 1.2
NBD3 non-canonical T-only (× 1000) 5.9 ± 6.7 0.9 6.0 ± 6.8 0.9 5.4 ± 6.8 0.8 5.5 ± 6.7 0.8
NBD3 non-canonical T+E (× 1000) 8.7 ± 5.0 1.7 6.2 ± 5.2 1.2 7.5 ± 5.2 1.5 9.4 ± 5.2 1.8
WarmS inflation T-only 23 ± 36 0.6 26 ± 36 0.7 32 ±36 0.9 24 ± 36 0.7
WarmS inflation T+E 14 ± 23 0.6 28 ± 23 1.2 21 ± 23 0.9 17 ± 23 0.7

Notes. See Sect. 2 for further explanation and the labelling of these classes of NBD models. Note that the NBD, NBD1, and NBD2 models contain free parameters, so here we quote the maximum significance found over the available parameter range; the maximum for T and T+E can occur at different parameter values (on which the error bars are also dependent).

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