Real and imaginary components of the third-order nonlinearity of polyaniline dodecylbenzenesulfonic salt

M. Samoc; A. Samoc; B. Luther-Davies; J. Swiatkiewicz; C. Q. Jin; J. W. White

doi:10.1364/OL.20.002478

Optics Letters
Vol. 20,
Issue 24,
pp. 2478-2480
(1995)
•https://doi.org/10.1364/OL.20.002478

Real and imaginary components of the third-order nonlinearity of polyaniline dodecylbenzenesulfonic salt

M. Samoc, A. Samoc, B. Luther-Davies, J. Swiatkiewicz, C. Q. Jin, and J. W. White

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M. Samoc, A. Samoc, B. Luther-Davies, J. Swiatkiewicz, C. Q. Jin, and J. W. White, "Real and imaginary components of the third-order nonlinearity of polyaniline dodecylbenzenesulfonic salt," Opt. Lett. 20, 2478-2480 (1995)

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Abstract

The third-order optical nonlinearity of a salt form of polyaniline has been measured at 527, 800, and 1054 nm. The dominant nonlinear response has been found to be bleaching of the material absorption, leading to high negative values of the imaginary part of the nonlinearity.

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Wavelength (nm)	Absorption Coefficient α (cm⁻¹)	Re(n₂) (cm²/W)	Im(n₂) (cm²/W)	β (cm/W)	\|Re(n₂)/α\| (cm³/W)
527	1370	5.9 × 10⁻¹³	−2.9 × 10⁻¹³	−6.8 × 10⁻⁸	4.3 × 10⁻¹⁶
800	5600	−1.4 × 10⁻¹²	−1.3 × 10⁻¹²	−2.1 × 10⁻⁷	2.5 × 10⁻¹⁶
1054	2300	−1.7 × 10⁻¹²	−3.5 × 10⁻¹³	−4.2 × 10⁻⁸	7.4 × 10⁻¹⁶

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