Author Affiliations
1Laboratory of Micro⁃Nano Optoelectronic Materials and Devices, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China2Science and Technology on Electro⁃Optical Information Security Control Laboratory, Academy of Opto⁃Electronics, China Electronics Technology Group Corporation, Tianjin 300308, Chinashow less
Fig. 1. Principle diagram of ideal optical limiter
Fig. 2. Research status of optical limiting
[4] Fig. 3. Optical limiting properties of graphene. (a)(b) Nonlinear transmittance and scattering signal of graphene dispersions versus incident laser energy density
[22]; (c)(d) open aperture
Z-scan curves of graphene NMP dispersions under action of nanosecond pulse laser
[23]; high-magnification (e) SEM and (f) TEM images of etched graphene
[24]; (g) open aperture
Z-scan curves of different materials
[24]; (h) normalized transmittance versus incident laser fluence
[24] Fig. 4. Optical limiting properties of different nanostructured graphene dispersions under action of 532 nm and 1064 nm nanosecond lasers
[25]. (a)(b) Normalized transmittance; (c)(d) scattering signals
Fig. 5. Nonlinear optical properties and mechanisms of MoX
2 dispersions. (a)(b) open aperture
Z-scan results of MoX
2 dispersions under action of femtosecond laser
[33] ; (c)(d) normalized transmittance (solid circles) and scattering signals (open circles) of TMDCs suspensions
[34]; (e) mechanism diagram of all-optical modulation
[35]; (f) mechanism diagram of SA and NLS of nanosheet dispersions
[35] Fig. 6. Nonlinear optical properties of TMDCs. (a) Two-photon absorption property of monolayer MoS
2 under action of near-infrared femtosecond laser
[36]; (b) SA property of multilayer MoS
2[36] ; (c) two-photon absorption coefficients of cm-scaled few-layered WS
2 under 1030 nm laser irradiation
[37]; (d) four two-photon absorption saturation models
[38]; (e)(f) self-focusing and defocusing behaviors of monolayer and bulk WS
2 [39] Fig. 7. Optical limiting properties of MoS
2 composite materials under 532 nm and 1064 nm laser irradiation. (a)(b) Output fluence versus input fluence for MoS
2/PMMA composite materials
[40]; (c)(d) normalized transmittance versus input laser intensity for MoS
2 composite materials
[41] Fig. 8. Nonlinear optical properties of BP nanosheets. (a)--(c)
Z scan results under action of 1064, 532, 355 nm lasers
[48]; (d) normalized transmittance versus input laser intensity for each wavelength
[48]; (e) optical modulation properties of BP dispersions
[49]; (f) modulation depths under different pump fluences
[49]; (g) open aperture
Z-scan results and corresponding (h) scattering signals
[49] Laser protectiontechnology | Advantage | Issue to be addressed |
---|
Notch filter | Multi-time scale, low protection threshold, high damage threshold, and large laser repetition rate | Narrow-band spectral range of ~10 nm, single wavelength, and low linear transmittance | Phase change material | Being effective for laser heating, high damage threshold, near infrared wavelength, and broadband spectral range of 0.5--10 μm | Long recovery time and low linear transmittance under laser operation | Optical limiting | Short response time, continuous broadband spectral range,low protection threshold, and being soft | Being unable to resist thermal ablation of continuous wave laser | Liquid crystal | Large electro-optic coefficient and low driving voltage | Long response time |
|
Table 1. Summarization of several laser protection technologies