Design of a broadband infrared absorber based on multiple layers of black phosphorus nanoribbons

Hamed Khalilzadeh; Amir Habibzadeh-Sharif; Niloufar Anvarhaghighi

doi:10.1364/JOSAB.444851

Journal of the Optical Society of America B
Vol. 38,
Issue 12,
pp. 3920-3928
(2021)
•https://doi.org/10.1364/JOSAB.444851

Design of a broadband infrared absorber based on multiple layers of black phosphorus nanoribbons

Hamed Khalilzadeh, Amir Habibzadeh-Sharif, and Niloufar Anvarhaghighi

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Hamed Khalilzadeh, Amir Habibzadeh-Sharif, and Niloufar Anvarhaghighi, "Design of a broadband infrared absorber based on multiple layers of black phosphorus nanoribbons," J. Opt. Soc. Am. B 38, 3920-3928 (2021)

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- Physical Optics
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About this Article
History
- Original Manuscript: September 30, 2021
- Revised Manuscript: November 1, 2021
- Manuscript Accepted: November 4, 2021
- Published: December 1, 2021

Abstract

A polarization-sensitive broadband plasmonic absorber consists of multiple black phosphorus (BP)/dielectric layers stacking on an Ag reflector has been proposed theoretically and demonstrated numerically for infrared (IR) regime. The optimum geometrical parameters have been achieved by parametric sweep analyses with regard to the fabrication considerations and miniaturization of the absorber structure. So a high absorption (above 85%) with relatively broad bandwidth of 5.24 µm corresponding to the relative bandwidth of 42.12% has been achieved for the designed periodic structure with optimum unit cell dimensions of ${0.5}\;\unicode{x00B5}{\rm m} \times {1.755}\;\unicode{x00B5}{\rm m}$. The electromagnetic loss in the BP material is the foundation of absorption performance in the designed absorber. The proposed anisotropic broadband IR absorber may have great potential in many areas of photonics.

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Data underlying the results presented in this paper are not publicly available at this time but may be obtained from the authors upon reasonable request.

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Ref.	BW (µm)	RBW (%)	Min ABS (%)	Max ABS (%)	Materials	Polarization	Unit Cell Size ( $µ m^{3}$ ) $P_{x} \times P_{y} \times H$
[39]	1.56 [5.75 7.31]	—	85	99	Al, ${M g F}_{2}$ , Al, ${A l}_{2} O_{3}$ , Al, Si	Independent	$2.4 \times 2.4 \times 0.4$
[40]	2.4 [3.4 5.8]	—	80	99	Al, Dielectric, Al	Dependent	$1.4 \times 1.4 \times 0.8$
[41]	2 [10.5 12.5]	—	80	99	SiC, Dielectric, Ag	Dependent	2D: $3 \times 30$
[42]	4.1[8.1 12.2]	—	90	100	a-Si, Al, Si	Independent	$2 \times 2 \times 800$
[43]	6 [8, 14]	—	85	$> 90$	Ti, Ge, Ti	Independent	$1.4 \times 1.4 \times 0.62$
[44]	1 [10, 11]	—	80	$> 90$	SiC, ${B a F}_{2}$	Dependent	2D: $5 \times 4$
[45]	7.3 [7 14.3]	—	80	$> 90$	Au, InP, Au	Dependent	2D: $2.4 \times 1.28$
[46]	4 [8, 12]	—	80	$> 99$	${I n A s}_{d o p e d}$ , InAs, ${I n A s}_{d o p e d}$	Dependent	2D: $2 \times 0.38$
[47]	4.8 [3.52 8.32]	81	80	$> 90$	Ni, Si, W	Independent	$1 \times 1 \times 0.43$
[48]	4.5 [7.7-12.2]	45	90	$> 95$	Au, ${A l}_{2} O_{3}$ , ZnS, Au	Independent	$6.76 \times 6.76 \times 0.79$
	8.5 [5.2 13.7]	90	80				$9.2 \times 9.2 \times 1.56$
[49]	2.01 (TE) [17.11 19.12]	11.1 (TE)	90	99	BP, ${A l}_{2} O_{3}$ , Metal	Dependent	$0.25 \times 0.25 \times 1.95$
	2.91 (TM) [13.71 16.62]	19.2 (TM)
[50]	3	—	85	100	BP, Dielectric, Au	Dependent	$0.2 \times 0.2 \times 2.6$
This work	5.27 [9.79 15.06]	42.41	85	$\approx 100$	BP, ${A l}_{2} O_{3}$ , Ag	Dependent	2D: $0.5 \times 1.755$

Hamed Khalilzadeh	https://orcid.org/0000-0001-6564-7583
Amir Habibzadeh-Sharif	https://orcid.org/0000-0002-2661-3708
Niloufar Anvarhaghighi	https://orcid.org/0000-0002-4639-4928

Abstract

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Journal of the Optical Society of America B