Advertisement

Nonlinear optical properties of sodium copper chlorophyllin in aqueous solution

Abstract

Background

Sodium copper chlorophyllin (SCC), as one of the derivatives of chlorophyll – with its inherent green features; good stability for heat, light, acids and alkalies; unique antimicrobial capability; and particular deodori zation performance – is widely applied in some fields such as the food industry, medicine and health care, daily cosmetic industry etc. SCC, as one of the metal porphyrins, has attracted much attention because of its unique electronic band structure and photon conversion performance. To promote the application of SCC in materials science; energy research and photonics, such as fast optical communications; and its use in nonlinear optical materials, solar photovoltaic cells, all-optical switches, optical limiters and saturable absorbers, great efforts should be dedicated to studying its nonlinear optical (NLO) properties.

Methods

In this study, the absorption spectra and NLO properties of SCC in aqueous solution at different concentrations were measured. The Z-scan technique was used to determine NLO properties.

Results

The results indicated that the absorption spectra of SCC exhibit 2 characteristic absorption peaks located at the wavelengths 405 and 630 nm, and the values of the peaks increase with increasing SCC concentration. The results also showed that SCC exhibits reverse saturation absorption and negative nonlinear refraction (self-defocusing).

Conclusions

It can be seen that SCC has good optical nonlinearity which will be convenient for applications in materials science, energy research and photonics.

J Appl Biomater Funct Mater 2017; 15(Suppl. 1): e19 - e24

Article Type: ORIGINAL RESEARCH ARTICLE

DOI:10.5301/jabfm.5000350

OPEN ACCESS ARTICLE

Authors

Jiangting Li, Yufeng Peng, Xueyun Han, Shaoshuai Guo, Kunning Liang, Minggao Zhang

Article History

Disclosures

Financial support: The authors would like to acknowledge support from the National Natural Science Foundation of China (grant 61077037), the Foundation and Advanced Technology Research Project of Henan Province (102300413214) and the Key Scientific and Technological Research Project of Henan Province (122102310032).
Conflict of interest: None of the authors has any financial interest related to this study to disclose.

This article is available as full text PDF.

Download any of the following attachments:

Introduction

Underwater laser communication (1-2-3-4-5-6), underwater laser imaging (7-8-9-10) and deep-sea exploration (11-12-13-14-15) and precision underwater positioning systems (16) have attracted much attention, along with the development of blue and green laser technology. Seawater is a very complex multicomponent aqueous solution. There are abundant dissolved ions in seawater such as sodium, chloride, magnesium, sulfate and calcium. Along with the increasing of coastal area developments, chlorophyll-a concentration is usually used as an important parameter in evaluating water quality, nutrition status and extent of organic pollution. Awad (17) performed sea water chlorophyll measurements in a coastal area using Hyperion satellite hyperspectral images. The vertical variability of chlorophyll-a in the Kara Sea regions in autumn was studied by Demidov and Mosharov (18). Wang et al (19) and Fu et al (20) investigated temporospatial distribution variations of chlorophyll in the South China Sea and China Bohai Sea, respectively. The distributions of chlorophyll concentration in the Japan Sea (21), the Adriatic Sea (22), the Red Sea (23) and Chukchi Sea (24) have been estimated by others.

Chlorophyll absorbs light most strongly in the blue portion of the electromagnetic spectrum, followed by the red portion. Conversely, it is a poor absorber of green and near-green portions of the spectrum, which it reflects. The maximum absorption peak of an aqueous solution is obtained to make clear the attenuation mechanism of laser beam propagation in underwater blue-green laser communication systems.

At the same time, liquid laser has received considerable attention owing to its high damage threshold and low stress birefringence. Among the various liquid laser solvents, most of the inorganic solvents are difficult to use due to their high toxicity and strong corrosiveness, while organic solvents are of great interest due to their nontoxicity and low cost. Sodium copper chlorophyllin (SCC) is a class of organic solvents. SCC, as one of the derivatives of chlorophyll – with its inherent green features; good stability for heat, light, acids and alkalies, unique antimicrobial capability, and particular deodorization performance – is widely applied in some fields such as the food industry (25, 26), medicine and health care (27, 28), daily cosmetic industry (29), etc. SCC is used as a green dye for food, toothpaste, detergents and cosmetics, and it is applicable to luminescence chemistry and spectrophotometric analysis as well as to organic synthesis and as a polymerization catalyst. SCC, as one of metal porphyrins, has attracted much attention because of its unique electronic band structure and photon conversion performance. To promote the application of SCC in materials science, energy research and photonics, such as fast optical communications, and its use in nonlinear optical materials (30-31-32), solar photovoltaic cells (33, 34), all-optical switches, optical limiters and saturable absorbers, great efforts should be dedicated to studying its nonlinear optical (NLO) properties.

At present, 4-wave mixing, elliptic polarization, nonlinear interferometry, self-diffraction, beam distortion and the Z-scan technique are available for investigating NLO properties. The Z-scan technique has been used as a convenient and effective method to explore the properties of NLO, as proposed by Sheik-Bahae in 1989. It is a simple, highly sensitive method that is widely used to determine NLO properties.

In this study, the absorption properties of an SCC aqueous solution in the light wavelengths of 300 to 800 nm were measured. Meanwhile, NLO properties of SCC in aqueous solution were studied. We used the Z-scan method to measure the NLO properties of SCC in aqueous solution with a laser irradiation at a wavelength of 355 nm.

Methods

SCC is a highly stable and water-soluble derivative of chlorophyll; its chemical formula is C34H31CuN4Na3O6 (Fig. 1). It is formed by replacing the central magnesium atom by a copper atom and is then saponified by dissolving in ethanol containing NaOH. SCC was chosen for our study (Chemical Abstracts Service [CAS] number: 11006-34-1, pH 9.5~10.7). It was provided by Shanghai Jinsui Biological Technology Co. Ltd. and prepared by dissolving it in pure water (resistivity of 18 MΩ × cm at a temperature of 25°C). Eight samples (Tab. I) of different concentrations of SCC solution were prepared. Each concentration was measured 3 times, and the measurement data were averaged to reduce experimental error.

Different concentrations of sodium copper chlorophyllin solution

Number 1 2 3 4 5 6 7 8
ppm = parts per million.
Concentration 0 ppm 0.625 ppm 1.25 ppm 2.5 ppm 3.75 ppm 5 ppm 7.5 ppm 10 ppm

Sodium copper chlorophyllin chemical structure.

Absorption spectra of the different concentrations in the range from 300 to 800 nm were recorded using a Cary 5000 spectrophotometer of the Australian (maximum absorbance: 8 Abs, photometric range: 175-3,300 nm; Agilent Scientific Technology Co. Ltd).

A schematic diagram of the experimental setup used for the Z-scan measurements is shown in Figure 2. The excitation laser source was a pulsed Nd:YAG laser with Gaussian beam profile at a wavelength of 355 nm. The beam splitters BS1 and BS2 were used to reflect part of the incident and transmitted laser beam onto the detectors D1 and D2. The laser input power was measured by the detector D1, while the transmitted laser power and the transmitted laser power through the aperture were measured by the detectors D2 and D3, respectively. The sample was a 10-mm quartz cell containing the SCC solution. The experiment was implemented by scanning the sample across the focus of the lens along the z-axis direction using a translation stage. Because all of the power transmitted through the sample was collected by D2, D2/D1 is called the open-aperture Z-scan. Because a part of the laser beam transmitted through the aperture was obtained by D3, D3/D1 is called the closed-aperture Z-scan.

Z-scan experimental setup. BS1 and BS2 are the beam splitters; L indicates the lens; A, the aperture; and D1, D2 and D3 are the detectors.

Figure 3A B shows the experimental setup for detecting optical power limiting behavior. Two 450-nm and 532-nm semiconductor lasers were pump and detector, respectively. The laser beam was focused by a convex lens of focal length 5 cm and passed through the sample, which was a 100-mm quartz cell containing SCC solution. The experiment was carried out with a modular multifunction grating spectrometer (WGD-8) provided by Tianjin Gangdong Scientific Technology Co. Ltd. An optical variable attenuator of the rotary-vane type was placed behind the sample. A Charge Coupled Device (CCD) (LS-2000 laser beam analyzer) provided by Beijing Wuke Photoelectric Technology Co. Ltd was used to measure the laser spot. A natrium lamp was used to calibrate the setup.

(A,B) Experimental apparatus setup. A = aperture; CCD = Charge Coupled Device(LS-2000 laser beam analyzer); L = lens; M = Mirror; S = sample; V = variable attenuator (rotary-vane type).

Results and discussion

Structural characteristics

With the aim of determining a complete list of the interplanar spacing for SCC, the crystalline structural characteristics were measured. The X-ray diffraction (XRD) patterns of the SCC are shown in Figure 4. The SCC lattice interplanar spacing was d = 2.82386 Å at 31.750˚ and d = 1.99533 Å at 45.482˚.

X-ray diffraction (XRD) of sodium copper chlorophyllin (SCC).

Absorption properties

Absorption spectra of SCC in aqueous solution for different concentrations are shown in Figure 5. The figure shows that the absorption spectra of SCC exhibited 2 characteristic absorption peaks, which were located at wavelengths of 405 and 630 nm. Judging from the figure, we can also see that the values of the peaks increase with increasing SCC concentration.

Absorption spectra of the different concentrations of sodium copper chlorophyllin (SCC) solution; ppm = parts per million.

In the case of the visible range, the transitions which result in the absorption of electromagnetic radiation in this region of the spectrum are transitions between electronic energy levels. All samples showed absorption spectra characterized by the presence of both Soret and Q peaks. The highly conjugated nature of the SCC macrocycle shows intense absorption in the Soret band (B), which appeared in the wavelength range of 360-490 nm, and the Q-band in the range 500-720 nm. The peaks in visible range have generally been interpreted in terms of a π–π* transition type from the highest occupied molecular orbital (HOMO) to the excited lowest unoccupied molecular orbital (LUMO).

Nonlinear optical effect

The open-aperture and closed-aperture Z-scan transmittance curves of SCC in aqueous solution at different concentrations were measured and are shown in Figure 6A and B respectively. The open-aperture Z-scan normalized transmittance curve was characterized by a valley that indicated nonlinear absorption (reverse saturable absorption). The closed-aperture Z-scan normalized transmittance curve was characterized by a peak followed by a valley. This means that the sign of the nonlinear refractive index of the SCC was negative (n2<0) – namely, a self-defocusing effect. This was due to the thermal lensing effect – i.e., the sample acted as a lens, leading to the variation of its refractive index (n) with temperature (T). The open-aperture Z-scan data show nonlinear absorption, while the closed-aperture Z-scan data show both nonlinear absorption and nonlinear refraction. Therefore, the closed-aperture Z-scan transmittance data were divided by the open-aperture Z-scan transmittance data. The pure nonlinear refraction Z-scan normalized transmittance curves for SCC in aqueous solution at different concentrations were thus obtained, and these are shown in Figure 6C.

Normalized transmittance curves for sodium copper chlorophyllin (SCC) solution at different concentrations. (A) Open-aperture Z-scan. (B) Closed-aperture Z-scan. (C) Pure nonlinear refraction. ppm = parts per million.

Optical power limiting behavior

Figure 7A and B shows the optical power limiting behavior of different concentrations SCC. The laser transmittance and spot radius, respectively, were plotted as a function of the laser input luminous intensity, varying over the range 0-4.5 × 106 w/cm2. It can clearly be seen that the transmittance varied in a linear fashion with increasing laser input luminous intensity (at low concentrations). The transmittance initially varied linearly with increasing laser input luminous intensity (at low luminous intensity), but the transmittance started to diminish at high luminous intensity (at high concentrations). Spot radius was just the opposite.

(A) Transmission spectra of different concentrations of sodium copper chlorophyllin (SCC) solution under different excitations. (B) Spot radius of different concentrations of SCC solution under different excitations; ppm = parts per million.

The optical power limiting behavior, based on the nonlinear refraction (self-defocusing) of the sample (SCC), evidently depended on the concentrations of the SCC and increased with increasing SCC concentrations.

Conclusion

We studied the absorption spectra and the NLO properties of SCC in aqueous solution at different concentrations. It was demonstrated that absorption features of SCC in the visible range included 2 absorbance peaks and 1 transmission band, which were molecular properties and were invariant with concentration. We used the Z-scan technique to measure NLO properties. We found that the absorption spectra of SCC exhibited 2 characteristic absorption peaks, which were located at wavelengths of 405 and 630 nm, and the values of the peaks increased with increasing SCC concentration. The experimental results showed that SCC was characterized by reverse saturation absorption and negative nonlinear refraction (self-defocusing). The values of the optical parameters increased in a linear fashion as SCC concentration increased. It could be seen that SCC has good optical nonlinearity and is a promising material for potential applications in nonlinear optical devices.

Disclosures

Financial support: The authors would like to acknowledge support from the National Natural Science Foundation of China (grant 61077037), the Foundation and Advanced Technology Research Project of Henan Province (102300413214) and the Key Scientific and Technological Research Project of Henan Province (122102310032).
Conflict of interest: None of the authors has any financial interest related to this study to disclose.
References
  • 1. Woodward B Sari H Underwater speech communications with a modulated laser. Appl Phys B 2008 91 1 189 194 Google Scholar
  • 2. Baiden G Bissiri Y Masoti A Paving the way for a future underwater omni-directional wireless optical communication systems. Ocean Eng 2009 36 9-10 633 640 Google Scholar
  • 3. Johnson LJ Green RJ Leeson MS Underwater optical wireless communications: depth dependent variations in attenuation. Appl Opt 2013 52 33 7867 7873 Google Scholar
  • 4. Rashed ANZ Sharshar HA Performance evaluation of short range underwater optical wireless communications for different ocean water types. Wirel Pers Commun 2013 72 1 693 708 Google Scholar
  • 5. Oubei HM Li C Park KH Ng TK Alouini MS Ooi BS 2.3 Gbit/s underwater wireless optical communications using directly modulated 520 nm laser diode. Opt Express 2015 23 16 20743 20748 Google Scholar
  • 6. Oubei HM Duran JR Janjua B et al. 4.8 Gbit/s 16-QAM-OFDM transmission based on compact 450-nm laser for underwater wireless optical communication. Opt Express 2015 23 18 23302 23309 Google Scholar
  • 7. Maccarone A McCarthy A Ren X et al. Underwater depth imaging using time-correlated single-photon counting. Opt Express 2015 23 26 33911 33926 Google Scholar
  • 8. Massot-Campos M Oliver-Codina G Optical sensors and methods for underwater 3D reconstruction. Sensors (Basel) 2015 15 12 31525 31557 Google Scholar
  • 9. He DM Underwater laser-illuminated range-gated imaging scaled by 22.5 cm ns-1 with serial targets. J Ocean Univ China 2004 3 2 208 219 Google Scholar
  • 10. Youwei H Fengmei C Weiqi J Su Q Underwater pulsed laser range-gated imaging model and its effect on image degradation and restoration. Opt Eng 2013 53 6 061608 Google Scholar
  • 11. Brewer PG Malby G Pasteris JD et al. Development of a laser Raman spectrometer for deep-ocean science. Deep Sea Res Part I Oceanogr Res Pap 2004 51 5 739 753 Google Scholar
  • 12. Coble PG Characterization of marine and terrestrial DOM in seawater using excitation-emission matrix spectroscopy. Mar Chem 1996 51 4 325 346 Google Scholar
  • 13. Thornton B Takahashi T Sato T et al. Development of a deep-sea laser-induced breakdown spectrometer for in situ multi-element chemical analysis. Deep Sea Res Part I Oceanogr Res Pap 2015 95 20 36 Google Scholar
  • 14. Angel SM Bonvallet J Lawrence-Snyder M Pearman WF Register J Underwater measurements using laser induced breakdown spectroscopy. J Anal At Spectrom 2016 31 1 328 336 Google Scholar
  • 15. Dunlop KM Kuhnz LA Ruhl HA et al. An evaluation of deep-sea benthic megafauna length measurements obtained with laser and stereo camera methods. Deep Sea Res Part I Oceanogr Res Pap 2015 96 38 48 Google Scholar
  • 16. White SN Kirkwood W Sherman A et al. Development and deployment of a precision underwater positioning system for in situ laser Raman spectroscopy in the deep ocean. Deep Sea Res Part I Oceanogr Res Pap 2005 52 12 2376 2389 Google Scholar
  • 17. Awad M Sea water chlorophyll-a estimation using hyperspectral images and supervised Artificial Neural Network. Ecol Inform 2014 24 60 68 Google Scholar
  • 18. Demidov AB Mosharov SA Vertical distribution of primary production and chlorophyll a in the Kara Sea. Oceanology (Mosc) 2015 55 4 521 534 Google Scholar
  • 19. Wang S Li S Hu J Geng B Experiments in optimizing simulations of the subsurface chlorophyll maximum in the South China Sea. J Mar Syst 2016 156 1 15 Google Scholar
  • 20. Fu Y Xu S Liu J Temporal-spatial variations and developing trends of chlorophyll-a in the Bohai Sea, China. Estuar Coast Shelf Sci 2016 173 49 56 Google Scholar
  • 21. Andreev AG Interannual variations of sea water parameters and chlorophyll-a concentration in the Japan Sea in autumn. Russ Meteorol Hydrol 2014 39 8 542 549 Google Scholar
  • 22. Mélin F Vantrepotte V Clerici M et al. Multi-sensor satellite time series of optical properties and chlorophyll-a concentration in the Adriatic Sea. Prog Oceanogr 2011 91 3 229 244 Google Scholar
  • 23. Brewin RJ Raitsos DE DallOlmo G et al. Regional ocean-colour chlorophyll algorithms for the Red Sea. Remote Sens Environ 2015 165 64 85 Google Scholar
  • 24. Brown ZW Lowry KE Palmer MA et al. Characterizing the subsurface chlorophyll a maximum in the Chukchi Sea and Canada Basin. Deep Sea Res Part II Top Stud Oceanogr 2015 118 88 104 Google Scholar
  • 25. López-Carballo G Hernández-Muñoz P Gavara R Ocio MJ Photoactivated chlorophyllin-based gelatin films and coatings to prevent microbial contamination of food products. Int J Food Microbiol 2008 126 1-2 65 70 Google Scholar
  • 26. Ferruzzi MG Schwartz SJ Thermal degradation of commercial grade sodium copper chlorophyllin. J Agric Food Chem 2005 53 18 7098 7102 Google Scholar
  • 27. Domijan AM Gajski G Jovanović I M Gerić Garaj-Vrhovac V In vitro genotoxicity of mycotoxins ochratoxin A and fumonisin B(1) could be prevented by sodium copper chlorophyllinimplication to their genotoxic mechanism. Food Chem 2015 170 455 462 Google Scholar
  • 28. Cope RB Loehr C Dashwood R Kerkvliet NI Ultraviolet radiation-induced non-melanoma skin cancer in the Crl:SKH1:hr-BR hairless mouse: augmentation of tumor multiplicity by chlorophyllin and protection by indole-3-carbinol. Photochem Photobiol Sci 2006 5 5 499 507 Google Scholar
  • 29. Hou X Yang R Xu H Yang Y Adsorption kinetic and thermodynamic studies of silk dyed with sodium copper chlorophyllin. Ind Eng Chem Res 2012 51 25 8341 8347 Google Scholar
  • 30. Farag AA Mansour AM Ammar AH Rafea MA Farid AM Electrical conductivity, dielectric properties and optical absorption of organic based nanocrystalline sodium copper chlorophyllin for photodiode application. J Alloys Compd 2012 513 404 413 Google Scholar
  • 31. Farag AA Optical absorption of sodium copper chlorophyllin thin films in UV-vis-NIR region. Spectrochim Acta A Mol Biomol Spectrosc 2006 65 3-4 667 672 Google Scholar
  • 32. Aydin ME Farag AA Abdel-Rafea M Ammar AH Yakuphanoglu F Device characterization of organic nanostructure based on sodium copper chlorophyllin (SCC). Synth Met 2012 161 23-24 2700 2707 Google Scholar
  • 33. Calogero G Citro I Crupi C Di Marco G Absorption spectra and photovoltaic characterization of chlorophyllins as sensitizers for dye-sensitized solar cells. Spectrochim Acta A Mol Biomol Spectrosc 2014 132 477 484 Google Scholar
  • 34. Tennakone K Kumara G Wijayantha KG Kottegoda IR Perera VP Aponsu GM A nanoporous solid-state photovoltaic cell sensitized with copper chlorophyllin. J Photochem Photobiol Chem 1997 108 2-3 175 177 Google Scholar

Authors

Affiliations

  • College of Electronic and Electric Engineering, Henan Normal University, Xinxiang - PR China
  • Henan Engineering Laboratory of Optoelectronic Technology and Advanced Manufacturing, Xinxiang - PR China
  • Henan Key Discipline Open Laboratory of Electromagnetic Wave Detecting, Xinxiang - PR China

Article usage statistics

The blue line displays unique views in the time frame indicated.
The yellow line displays unique downloads.
Views and downloads are counted only once per session.

No supplementary material is available for this article.