Direct comparison of sterile neutrino constraints from cosmological data, $$\nu _{e}$$ disappearance data and $$\nu _{\mu } \rightarrow \nu _{e} $$ appearance data in a $$3+1$$ model
Abstract We present a quantitative, direct comparison of constraints on sterile neutrinos derived from neutrino oscillation experiments and from Planck data, interpreted assuming standard cosmological evolution. We extend a $$1+1$$ 1 + 1 model, which is used to compare exclusion contours at the 95%...
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Published in | The European physical journal. C, Particles and fields Vol. 80; no. 8 |
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Main Authors | , , , , , , |
Format | Journal Article |
Language | English |
Published |
01.08.2020
|
Online Access | Get full text |
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Summary: | Abstract
We present a quantitative, direct comparison of constraints on sterile neutrinos derived from neutrino oscillation experiments and from Planck data, interpreted assuming standard cosmological evolution. We extend a
$$1+1$$
1
+
1
model, which is used to compare exclusion contours at the 95% Cl derived from Planck data to those from
$$\nu _{e}$$
ν
e
-disappearance measurements, to a
$$3+1$$
3
+
1
model. This allows us to compare the Planck constraints with those obtained through
$$\nu _{\mu }\rightarrow \nu _{e}$$
ν
μ
→
ν
e
appearance searches, which are sensitive to more than one active-sterile mixing angle. We find that the cosmological data fully exclude the allowed regions published by the LSND, MiniBooNE and Neutrino-4 collaborations, and those from the gallium and rector anomalies, at the 95% Cl. Compared to the exclusion region from the Daya Bay
$$\nu _{e}$$
ν
e
-disappearance search, the Planck data are more strongly excluding above
$$|\Delta m^{2}_{41}|\approx 0.1\,\mathrm {eV}^{2}$$
|
Δ
m
41
2
|
≈
0.1
eV
2
and
$$m_\mathrm {eff}^\mathrm {sterile}\approx 0.2\,\mathrm {eV}$$
m
eff
sterile
≈
0.2
eV
, with the Daya Bay exclusion being stronger below these values. Compared to the combined Daya Bay/Bugey/MINOS exclusion region on
$$\nu _{\mu }\rightarrow \nu _{e}$$
ν
μ
→
ν
e
appearance, the Planck data is more strongly excluding above
$$\Delta m^{2}_{41}\approx 5\times 10^{-2}\,\mathrm {eV}^{2}$$
Δ
m
41
2
≈
5
×
10
-
2
eV
2
, with the exclusion strengths of the Planck data and the Daya Bay/Bugey/MINOS combination becoming comparable below this value. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-020-8197-y |