1990
DOI: 10.1364/josaa.7.001736
|View full text |Cite
|
Sign up to set email alerts
|

Perfect blazing for transmission gratings

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

1990
1990
2017
2017

Publication Types

Select...
3
2
1

Relationship

0
6

Authors

Journals

citations
Cited by 11 publications
(2 citation statements)
references
References 6 publications
0
2
0
Order By: Relevance
“…Au + k2(x,y)u -0, (13) which can be called a generalized Helmholtz equation because k2 -kv(x,y) is not a constant .…”
Section: Differential Methods (Dl'!)mentioning
confidence: 99%
“…Au + k2(x,y)u -0, (13) which can be called a generalized Helmholtz equation because k2 -kv(x,y) is not a constant .…”
Section: Differential Methods (Dl'!)mentioning
confidence: 99%
“…The power distribution between the different orders and within a given order as a function of wavelength, however, depends on the groove geometry: the shape of the individual grooves, their orientation with respect to the grating normal, and the width of the grooves relative to the size of the spacing between them. Derivation of the blaze function is complex and requires detailed calculation of the electromagnetic behavior of the groove structure, taking into account the geometry, the material properties, and the polarization of the radiation (Nevière et al 1990;Neviere 1991). The most common sorts of infrared grisms for astronomy either employ flat-faceted grooves that fill the groove intervals and have 90 • corners or, in the case of micro-machined Si grisms, flat-faceted grooves with 70 • vertices and small (filling-factor ∼ 10%) lands parallel to the grating surface in between the facets (Figure 3).…”
Section: Blazementioning
confidence: 99%