2014
DOI: 10.1016/j.optmat.2013.12.012
|View full text |Cite
|
Sign up to set email alerts
|

Ultrafast third-order optical nonlinearities of heavy metal oxide glasses containing gold nanoparticles

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
9
0
1

Year Published

2017
2017
2019
2019

Publication Types

Select...
6
2

Relationship

1
7

Authors

Journals

citations
Cited by 48 publications
(10 citation statements)
references
References 22 publications
0
9
0
1
Order By: Relevance
“…Third-order optical nonlinearities (TONL) of glass materials have been extensively studied, mainly due to their possible applications in telecommunications as ultrafast optical switches, modulators, and electro-optical devices [1][2][3][4]. Among several formed glass lattices, TeO 2 -based glass is receiving special attention due to its good optical properties, particularly when compared to traditional silicate glass, for instance.…”
Section: Introductionmentioning
confidence: 99%
“…Third-order optical nonlinearities (TONL) of glass materials have been extensively studied, mainly due to their possible applications in telecommunications as ultrafast optical switches, modulators, and electro-optical devices [1][2][3][4]. Among several formed glass lattices, TeO 2 -based glass is receiving special attention due to its good optical properties, particularly when compared to traditional silicate glass, for instance.…”
Section: Introductionmentioning
confidence: 99%
“…The same kind of nonlinear results (i.e., SA in OA Z-scan mode and negative nonlinear refraction in CA Z-scan mode) were reported by Chen et al [39] recently and they reported their investigations on transparent glasses matrix with glass composition of 60Bi 2 O 3 -30B 2 O 3 -10TiO 2 in which they measured the NLO properties by adopting Z-scan technique at 750 nm using 200 fs laser pulses and a repetition rate of 76 MHz. The 2PA coefficients (α 2 ) of Au-NP-doped glasses of present investigation are found to be one order of magnitude greater than that of Na 2 O-CaO-B 2 O 3 -SiO 2 bulk glasses embedded with CuO quantum dots (α 2 = 1.56 × 10 −12 m/W at 1550 nm) [32] and that of gold NP-doped heavy metal oxide glasses (α 2 varied from 0.6 × 10 −12 m/W to 0.9 × 10 −12 m/W for the wavelengths in the range of 500 nm to 580 nm) [22]. The coefficients are comparable to that of sodium borosilicate glasses doped with copper quantum dots (α 2 = 2.10 × 10 −11 m/W at 1550 nm) [21] and lower than that of silver-doped oxyfluoride glasses (α 2 ranges from 1.1 × 10 −9 m/W to 24.8 × 10 −9 m/W at the wavelengths from 445 nm to 660 nm of NPs sizes 3 nm and 17 nm) [39].…”
Section: Resultsmentioning
confidence: 99%
“…Zhong et al [21] reported reverse saturable absorption (RSA) in copper NPdoped sodium borosilicate glasses at 800 nm with fs-pulse excitation. Furthermore, by studying the temporal dynamics of HMO glasses embedded with Au-NPs using Kerr gate measurements at 780 nm using 120 fs pulses, Almedia et al [22] have found that the response time was 220 fs (which was faster than the pulse duration). However, there are very few reports on the comparison of NLO properties using different wavelengths in glasses.…”
Section: Introductionmentioning
confidence: 99%
“…Such experiments were performed in a 700 µm thick sample. A complete description of Z-scan and OKG setups used here can be found in [20].…”
Section: Methodsmentioning
confidence: 99%