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Optical properties of sol-gel coatings for fiberoptic sensors

Monika Lechna

*

, Iwona Holowacz, Agnieszka Ulatowska, Halina Podbielska Bio-Optics Group

Institute of Physics, Wrocław University of Technology, 50 370 Wrocław, Wybrzeze Wyspianskiego 27, Poland

Abstract

The sol-gel-derived materials can be exploited for the construction of various optoelectronic devices, including sensors optodes and theirs protecting layers, as well as other kinds of coatings.

Different types of materials were studied here: silica sol-gel matrices made from silica solutions with water or alcohol as solvents. The samples were prepared in form of single layer films. The films were deposited on glass surfaces. The porous structure of sol-gels layers was examined as well as the transmittance spectra were measured in visible and in UV region. The strong influence of the solvent on the material optical properties was stated. Alcohol based samples showed stable homogenous structure, with no cracking. From, the other hand the water based samples

demonstrate higher transmittance in visible region. The obtained results can serve as a basis for choosing the suitable layer when constructing optical sensors or coatings.

Keywords: sol-gel coatings, optical properties, solvents

1. Introduction

The sol-gel process allows to obtain glass-like materials with tailored specific features. In recent years the number of research have been conducted in order to create and to study this type of materials produced in room temperatures from liquid precursors [1, 2]. Sol-gel derived matrices can be potentially used in many applications in medicine [3], food production [4] or chemistry [5].

Theirs promising features can be exploited in computer technology [6], integrated systems with fiber optics [7], [8], lasers construction [9] and materials science [10]. The high quality materials for optical fibers [11], films and coatings [12], solid bulks [13] etc. can be produced, as well.

Since the non-melted sol-gels have generally porous structure, many compounds can be entrapped into the sol gel matrix. The applications include sensors, where sol-gels are used as a material for optodes of chemical optical sensors or biosensors [14], [15]. The sol-gel protective coatings can improve the performance of fiberoptic oxygen sensors [16] or it be exploited for construction of microoptodes [17].

For majority of the described applications it is necessary to have homogenous highly transparent materials with smooth surfaces. Therefore, it is important to examine the sol-gels optical properties and structure depending on the procedure of fabrication and compounds used as substrates. In this study the light transmission in silica sol-gel coatings, as well as their structure are examined.

*

Corresponding author: Halina Podbielska, Institute of Physics, Wrocław University of Technology, 50 370 Wroclaw,

Wybrzeze Wyspianskiego 27, tel +48 501436607, fax:*48 71 3283696, e-mail: podbiels@rainbow.if.pwr.wroc.pl

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2. Materials preparation

The chemistry of the sol-gel process comprises several steps that are well described in the literature [1], [2]. First, silicate precursor is mixed with solvent (water or alcohol) and catalyst and stirred for a few hours. This process leads to hydrolysis of the Si-O-R bonds. The sol-gel films in this study were prepared from the following precursors: TEOS – tetraethoxysilan (Aldrich) with addition of Triton X-100 (Aldrich). Triton plays here the role of detergent enabling better adhesion of coating to the base surface. As a solvent doubly distilled water or alcohol were used in

corresponding amounts, so thus to obtain the required R ratios. Molar ratio R is defined as a ratio of number of solvent moles to the number of precursor moles. The acid (HCl) was added in proper amounts to ensure the acid hydrolysis or the base (NaOH) for basis hydrolysis. All the precursors were mixed for 4 hours by means of magnetic stirrer with the speed 400/min at the room

temperature. The samples were prepared with the following molar ratios R: R=50, R=32, R=15, R=5 (see Tab.1).

Tab. 1

Molar ratios of produced samples and types of solvent

Sample No R Type of solvent

1. 5 Ethyl alcohol

2. 15 Ethyl alcohol

3. 15 Water

4. 32 Ethyl alcohol

5. 32 Water

6. 50 Ethyl alcohol

The microscopic ground plates were first washed in water with detergent and then, they were rinsed in doubly distilled water. Eventually, the glass plates were washed in ethyl alcohol.

After alcohol evaporation they were clean and dry. Liquid hydrolyzate was spread with clean glass rod on the surface of microscopic ground glass. The thickness of sol-gel layer as measured in interferometric microscope was equal to1 m5%.

3. Transmission properties of sol-gel coatings

The measurements of transmittance spectra in UV and in visible region were performed by means of Perkins-Elmer spectrophotometer. First, the transmittance of the sol-gel materials prepared with alcohol as a solvent was measured (Fig.1). It was found that the spectral properties depend on the molar ratio R. The lowest transmittance was observed for the samples prepared with the molar ratio R=5, the highest one was for the sample prepared with the molar ratio R=50.

However, the materials prepared with the molar ratio R=15, R=32 showed comparable high transmission in visible spectrum.

In Fig. 2 the comparison of transmission in sol-gel coatings with molar ratio R=32 prepared

with alcohol and water solvent is presented. Analyzing the diagrams, one can see that alcohol

based samples show higher transmittance than these prepared on water. For R=15 the same

behavior is observed, however in this case the difference is less significant (see Fig. 3).

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40 50 60 70 80 90 100

350 450 550 650 750 850

Wavelength [nm ]

T ra n sm is si o n [ % ]

molar ratio R=15 molar ratio R=32 molar ratio R=5 molar ratio R=50

Fig. 1. The influence of different molar ratios R on transmission spectra in sol-gel coatings prepared with alcohol as solvent.

40 50 60 70 80 90 100

350 450 550 650 750 850

Wavelength [nm ]

T ra n sm is si o n [ % ]

molar ratio R32-w ater molar ratio R32-alcohol

Fig. 2. The influence of the solvent on transmission spectra for the sample with molar ratio R=32.

40 50 60 70 80 90 100

350 450 550 650 750 850

Wavelength [nm]

T ra n sm is si o n [ % ]

molar ratio R15 -w ater molar ratio R15-alcohol

Fig. 3. The influence of the solvent on transmission spectra for the sample with molar ratio

R=15.

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Fig. 4. The influence of the type of hydrolysis on transmission spectra for the sample with molar ratio R=32.

Figure 4 demonstrates the transmittance spectra of the samples prepared on the way of base as well as acid hydrolysis. Both coatings were alcohol based and prepared with molar ration R=32.

The acid catalyzed samples show higher transmission than the base catalyzed ones.

4. Structural examination

In this study the surface of sol-gel coatings was examined by means of optical microscope. The microscopic image was recorded by the CCD camera and observed on the computer monitor. The Fly Video Life View frame grabber was used for image capturing. Some of the results are presented iFig. 4.

A B

Fig.4. The microscopic picture of the surface of the sol-gel layers prepared with the molar ratio R=32 (A) and R=5 (B) with alcohol as a solvent.

The surface of the layer prepared with molar ratio R=32 is smooth, no cracking are seen (one can see only small artifacts caused probably by dust particles). The sample made with R=5 is

1,5 mm 1,5 mm

0 20 40 60 80 100

350 400 450 500 550 600 650 700 750 800 Wavelength [nm]

T ra n sm is si o n [ % ]

sol-gel "acid" sol-gel "base"

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non-homogenic, one can observe a lot of scratches and cracking on the surface.

In the next, the microstructure of the sol-gel materials was studied by means of the mercury porosimetry (instrument type: Pascal 440). The structural variables used to characterize the pores in the sample, such as the pore volume, total porosity, specific surface area, pore distribution, and average pore diameter were determined. Because the alcohol-based sol-gels with molar ratio R=32 revealed the highest transmission in the visible range, the porosity examination were performed for these samples. Two types of samples were examined. The one was produced on the way of acid hydrolysis (with HCL as catalyzator) and the other one produced during the base type of

hydrolysis catalyzed by NaOH.

The experimental results demonstrating the pores radius and distribution are shown in Fig.5a and Fig.5b.

A B

Fig. 5. Pore size distribution in sol-gel material prepared in the way of base (A) and acid- hydrolysis (B) with the molar ratio R=32 and with alcohol as a solvent.

The samples prepared on the way of acid hydrolysis demonstrate more inhomogeneous

distribution of pore size within the material. In this case micropores (few nm radius) as well as meso- and macropores are observed. These materials have microporous structure with the agglomerates organized into larger clusters approaching 1 m. In contrary, base hydrolysis leads to the creation of material with more homogenous pores distribution. No meso- and macropores are observed. However, the total porosity in acid catalyzed samples is equal to 2,4802%, and in base hydrolyzed material the porosity is 29,2246%. Average pore diameter in case of acid

hydrolysis was 4,4345nm, while for base hydrolyzed samples it was 6, 4969nm, what is the direct result of the total porosity measured.

5. Conclusion

In this paper the silica single-layer sol-gel coatings produced from TEOS (Tetraethoxysilan) have been examined. The influences of the type of solvent and molar ratios R on sol-gel films

transmission properties were discussed in this work. The transmittance depends on molar ratio.

The highest one was stated in case of the samples prepared with alcohol and molar ratio R=32.

When analyzing the type of catalizator it was proved that HCL catalyzed hydrolysis leads to production of more transparent samples than NaOH catalyzed process. This can be explained by

0 10 20 30 40 50

1 10 100 1000

Pore Radius [nm]

R el at iv e p o re v o l. [ % ]

0 10 20 30 40 50

1 10 100 1000

Pore Radius [nm]

R el at iv e p o re v o l. [ % ]

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the presence of sodium in the layer. So, while adding some dopants, one can influence the spectroscopic properties of the prepared coatings.

The structural microscopic analysis allowed to prove that the most homogenous material is in the case of the samples prepared with alcohol and molar ratio R=32. However, porosimetry

examination lead to the conclusion that base catalyzed process results in more equal pores distribution. So, the lower transmission in this case was most probably due to the catalizator type used in experiment.

Acknowledgements

The support of the Polish State Committee for Scientific Research KBN, Grant No. 8 T11E 029 15 is gratefully acknowledged.

References

[1] Klein L. C. (ed.): Sol-Gel Optics:Procesing and Applications, Kluwer Academic Publishers, Boston, 1994.

[2] Brinker C.J., Scherer G.W.: Sol-Gel Science, Academic Press, San Diego, Ca, 1999.

[3] V.Glezer and O.Lev: Sol-Gel Vanadium Pentaoxide Glucose Biosensor, Journal of American Chemical Society 115, (1993), pp. 2533-2534.

[4] S.S.Park, J.D.Mackenzie, Thickness and microstructure effects on alcohol sensing of tin oxide thin films, Thin Solid Films 274, (1996), pp.154-159.

[5] R.Zusman, C.Rottman, M.Ottolenghi and D.Avnir, Doped sol-gel glasses as chemical sensors, Journal of Non-CrystallineSolids 122, (1990), pp. 107-109.

[6] Y. Mitsuhashi, A. Matsuda, Y. Matsuno, Sol-gel technology for optical disk application, SPIE Proc. 1758, (1992), pp. 105-112.

[7] B.D.MacCraith, C.M.McDonagh, G.O`Keeffe, A.K.McEvoy, T.Butler, F.R.Sheridan, Sol-gel coatings for optical chemical sensors and biosensors, Sensors & Actuators B29, (1995), pp.51-57.

[8] R.Blue, G.Stewart, Fibre-optic evanescent wave pH sensing with dye doped sol-gel films, International Journal of Optoelectronics 10, (1995), pp.211-222.

[9] R.Gvishi, G.Ruland, P.N.Prasad, New Laser Medium: Dye-Doped Sol-Gel Fiber, Optics Communications 126, (1996), pp. 66-72.

[10] E.Traversa, New ceramic materials for chemical sensors, Journal of Intelligent Material Systems and Structures 6, (1995), pp. 860-869.

[11] F.Kirkbir, S.R.Chaudhuri, Optical fibers from sol-gel derived germania-silica glasses, SPIE Proc. 1758, (1992), pp.160-172.

[12] H.G.Floch, P.F.Belleville, A scratch-resistant single-layer antireflective coating by a low temperature sol-gel route, SPIE Proc. 1758, (1992), pp.135-149.

[13] L.L.Hench, G.P.LaTorre, S.Donovan, J.Marotta, E.Valliere, Properties of gel-silica optical

matrices with 4.5-nm and 9.0-nm pores, SPIE Proc. 1758, (1992), pp.94-104.

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[14] M.K.Krihak, M.R.Shahriari, Highly sensitive, all solid state fiber optic oxygen sensor based on the sol-gel coating technique, Electronics Letters 32, (1996), pp. 240-242.

[15] B.C.Dave, B.Dunn, J.Selverstone Valentine and J.I.Zink, Sol-Gel Encapsulation Methods for Biosensors, Anal.Chem. 66, (1994), pp. 1120A-1127A.

[16] D. Andrzejewski, H. Podbielska, A. Ulatowska, Sol gel protective layer for fiberoptic chemical microsensors, Opt. Appl. vol. XXX, No.4 2000, 503-508, (2000).

[17] D. Andrzejewski, H. Podbielska, Examination of various shape of sol-gel optodes for indirect

fiberoptic sensors, OPTIK 112, 2001, in press.

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