2006
DOI: 10.1088/1742-6596/38/1/023
|View full text |Cite
|
Sign up to set email alerts
|

Large Resonant Third-order Optical Nonlinearity of CdSe Nanocrystal Quantum Dots

Abstract: Resonant third-order nonlinear optical susceptibility and hyperpolarizability of CdSe nanocrystal quantum dots were revealed to be ~2.6×10-20-2.7×10-19 m 2 /V 2 and ~2.2×10-40 m 5 /V 2 by using nanosecond degenerate four-wave mixing at 532 nm. The large nonlinearity of the CdSe nanocrystals is attributed to the resonant excitation and multiple nonlinear optical processes.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4

Citation Types

0
19
0

Year Published

2006
2006
2016
2016

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 21 publications
(19 citation statements)
references
References 6 publications
0
19
0
Order By: Relevance
“…In this article, we present the third-order optical nonlinearities and hyperpolarizabilities of CdS NCs as a function of the concentrations of NCs using polarization-resolved degenerate four-wave mixing (DFWM). The polarization-resolved DFWM involves the comparison of the parallel polarized DFWM and the perpendicularly polarized DFWM, and is usually used to measure different χ (3) ijkl components (where ijkl = x, y, z) and the electronic, molecular reorientation, and thermal contribution to the thirdorder nonlinearity. When the pump and probe laser beams are linearly polarized at 0 o and 90 o , respectively, the intensity distribution of the interaction region is uniform, in other words, there are no intensity modulations because the two laser beams can not interfere with each other.…”
Section: Introductionmentioning
confidence: 99%
See 3 more Smart Citations
“…In this article, we present the third-order optical nonlinearities and hyperpolarizabilities of CdS NCs as a function of the concentrations of NCs using polarization-resolved degenerate four-wave mixing (DFWM). The polarization-resolved DFWM involves the comparison of the parallel polarized DFWM and the perpendicularly polarized DFWM, and is usually used to measure different χ (3) ijkl components (where ijkl = x, y, z) and the electronic, molecular reorientation, and thermal contribution to the thirdorder nonlinearity. When the pump and probe laser beams are linearly polarized at 0 o and 90 o , respectively, the intensity distribution of the interaction region is uniform, in other words, there are no intensity modulations because the two laser beams can not interfere with each other.…”
Section: Introductionmentioning
confidence: 99%
“…toluene ) is assumed to be an addition of the effective third-order susceptibility of CdS NCs (χ NCs_eff ) and that of toluene (χ (3) toluene ) contributions in the dilute approximation [3]. The effective third-order susceptibilities of CdS NCs include the dielectric effect of NCs and toluene.…”
Section: Introductionmentioning
confidence: 99%
See 2 more Smart Citations
“…One QD material is CdSe, which has unique properties such as a stronger extinction coefficient, narrower band gap [29] , higher quantum confinement effect, higher optical gain, broader absorption profile, better photochemical stability [30] , and larger Stokes shift [30,31] compared to bulk semiconductors. A CdSe QD exhibits resonant non-linearity in slow times scales, which induces huge optical non-linearity, an important feature for generating Q-switched pulsed lasers [32] . The CdSe produced by the QD method has significant advantages over other reinforcements due to the high surface area to volume ratio and the small size distribution.…”
mentioning
confidence: 99%