2011
DOI: 10.1088/2040-8978/13/7/075601
|View full text |Cite
|
Sign up to set email alerts
|

Efficient surface relief grating generated in azobenzene-containing material using an He–Ne laser

Abstract: Very efficient holographic surface relief grating inscription has been demonstrated using an He-Ne laser in an azobenzene-containing material. Alternatively other lasers such as an Ar + laser at 488 nm and a DPSS laser at 532 nm were also successfully used for inscription in the same material.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
11
0

Year Published

2012
2012
2023
2023

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 16 publications
(11 citation statements)
references
References 24 publications
0
11
0
Order By: Relevance
“…22 p(m-DY7) and p(o-MHA), having well-separated π−π* and n−π* bands, are rather unconventional for SRG formation, yet they confirm that it is not the extent of initial absorption, but efficient trans−cis−trans cycling that is key to efficient SRG formation in the context of amorphous materials. 46 Because the initial absorption at writing wavelength, 488 nm, is already lower than at the π−π* absorption, the thickness of the films is not an issue and the films can, for example, be easily manipulated from the backside if needed. Although p(DY7) is more efficient in terms of absolute SRG formation efficiency, in terms of how efficiently the absorbed photons are transferred into mass transport of the polymer, p(m-DY7) is clearly superior to the conjugated p(DY7).…”
Section: Chemistry Of Materialsmentioning
confidence: 99%
“…22 p(m-DY7) and p(o-MHA), having well-separated π−π* and n−π* bands, are rather unconventional for SRG formation, yet they confirm that it is not the extent of initial absorption, but efficient trans−cis−trans cycling that is key to efficient SRG formation in the context of amorphous materials. 46 Because the initial absorption at writing wavelength, 488 nm, is already lower than at the π−π* absorption, the thickness of the films is not an issue and the films can, for example, be easily manipulated from the backside if needed. Although p(DY7) is more efficient in terms of absolute SRG formation efficiency, in terms of how efficiently the absorbed photons are transferred into mass transport of the polymer, p(m-DY7) is clearly superior to the conjugated p(DY7).…”
Section: Chemistry Of Materialsmentioning
confidence: 99%
“…[7][8][9] During this process, the polymer topography deforms following the distribution of the intensity or polarization of the incoming UV light. [10][11][12][13][14][15][16][17][18][19] The process takes place in air, where the polymer film is solid-like.…”
Section: Introductionmentioning
confidence: 99%
“…Among them, SRGs have attracted rapidly increasing attention because they are promising candidates for optical data storage, 31,32 micro/nanopatterning 28,[33][34][35][36][37][38] and chemical sensing. 39,40 SRGs can be inscribed on the azo polymer films at a temperature well below their glass transition temperatures (T g ) upon irradiation with interfering polarization laser beams with an appropriate wavelength, [41][42][43][44] and they are erasable by thermal treatment or by irradiation with a uniform circularly polarized laser beam. 20,31,45 During this process, the azo molecules undergo a reversible trans-cis-trans isomerization and are aligned perpendicularly to the electrical field vector of the polarization light through the repetition of such isomerization cycles.…”
Section: Introductionmentioning
confidence: 99%