1970
DOI: 10.1126/science.168.3929.396
|View full text |Cite
|
Sign up to set email alerts
|

Ice Survey by the U. S. Coast Guard work

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
2
0

Year Published

1970
1970
2013
2013

Publication Types

Select...
3
1

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(2 citation statements)
references
References 0 publications
0
2
0
Order By: Relevance
“…35 At low energies, this kinetic mixing may be considered as effectively a mixing between the ordinary photon and the dark photon. Two cases have been considered at length in the literature: (i) photon-mirror-photon mixing in the context of mirror matter, where the mirror photon is massless and its couplings to mirror states are identical in form and strength to the coupling of ordinary photons to ordinary charged particles [208,[339][340][341], and (ii) a more generic setup where the dark photon has a mass M D , and phenomenological constraints and detection prospects are analysed in terms the two-dimensional parameter space (ǫ, M D ) (for a recent compilation of bounds, see Ref. [369]).…”
Section: Dark Force Constraintsmentioning
confidence: 99%
See 1 more Smart Citation
“…35 At low energies, this kinetic mixing may be considered as effectively a mixing between the ordinary photon and the dark photon. Two cases have been considered at length in the literature: (i) photon-mirror-photon mixing in the context of mirror matter, where the mirror photon is massless and its couplings to mirror states are identical in form and strength to the coupling of ordinary photons to ordinary charged particles [208,[339][340][341], and (ii) a more generic setup where the dark photon has a mass M D , and phenomenological constraints and detection prospects are analysed in terms the two-dimensional parameter space (ǫ, M D ) (for a recent compilation of bounds, see Ref. [369]).…”
Section: Dark Force Constraintsmentioning
confidence: 99%
“…The most important constraint comes from BBN. If ǫ is too large, then kinetic-mixing-induced processes such as e + e − → e ′+ e ′− , where e ′ is the mirror electron, will bring the mirror sector into thermal equilibrium with the visible sector and spoil BBN [339,341]. The critical parameter is the ratio of the mirror-and visible-sector temperatures, T ′ /T , and one may track the thermal production of mirror particles from the visible-sector bath as a function of ǫ.…”
Section: Dark Force Constraintsmentioning
confidence: 99%