Poster Session, Thursday, June 17Theme F686 - N1123Comparison of The Dispersion Properties of The Solid-Core <strong>Photonic</strong> Crystal Fibers with a FixedDiameter of Holes and The Fixed Pitch Length at Wavelength Region of 0.8-2 mHalime Demir 1* and Sedat Özsoy 11 Department of Physics,Faculty of Science and Arts, Erciyes University, Kayseri 38039, TurkeyAbstract— In this work, for a solid core photonic crystal fiber with the triangular lattice, the dispersion of fundamental modeis exam<strong>in</strong>ed at wavelength region of 0.8-2 m. The silica core is constituted by remov<strong>in</strong>g the 7 air hole. The cladd<strong>in</strong>gconsists of the two dimensional silica-air photonic crystal with the 4-r<strong>in</strong>g of air holes. The dispersion properties were<strong>in</strong>vestigated for different values of d/, first with fixed and then with fixed d. Here, d and represent the diameter of airholes and the pitch length, respectively. The results obta<strong>in</strong>ed are then compared and it is concluded that, for a dispersiontailor<strong>in</strong>g, the configurations with fixed diameter are more effective than for fixed pitch length.In recent years, the photonic crystal fibers (PCFs) have asignificant <strong>in</strong>terest due to their unique structures and newproperties [1-6]. Generally, photonic crystal fibers consist ofan arrangement of air holes <strong>in</strong> the cladd<strong>in</strong>g extend<strong>in</strong>g thewhole length of the fiber. <strong>Photonic</strong> crystal fibers arecategorized <strong>in</strong>to two groups accord<strong>in</strong>g to light guid<strong>in</strong>gmechanism. One is the <strong>in</strong>dex guid<strong>in</strong>g photonic crystal fiberand the other is the photonic band gap PCF. In the <strong>in</strong>dexguid<strong>in</strong>g PCF s , the core region is solid and the light is conf<strong>in</strong>ed<strong>in</strong> the central core as <strong>in</strong> the conventional fibers. The photoniccrystal fiber consists of the pure silica fiber with an array ofthe air-holes along the length of the fiber. The core isconstituted by remov<strong>in</strong>g the central hole from the structure.The higher effective refractive <strong>in</strong>dex of the surround<strong>in</strong>g holesforms cladd<strong>in</strong>g <strong>in</strong> which lead<strong>in</strong>g the <strong>in</strong>dex guid<strong>in</strong>g mechanismanalogous to total <strong>in</strong>ternal reflection. Consequently, the lightguid<strong>in</strong>g can be expla<strong>in</strong>ed by the total <strong>in</strong>ternal reflection whichis also the way light is guided <strong>in</strong> step <strong>in</strong>dex fibers.PCFs have been shown to posses many importantproperties as the s<strong>in</strong>gle mode operation over wide range ofwavelength, the highly tunable dispersion, the propagation ofhigh power densities without excit<strong>in</strong>g unwanted nonl<strong>in</strong>eareffects and the high birefr<strong>in</strong>gence. These properties have thepractical importance <strong>in</strong> design of sophisticated broadbandoptical telecommunication networks [7] and active sensorsystems [8]. In optical communication, dispersion plays asignificant role because it determ<strong>in</strong>es the <strong>in</strong>formation carry<strong>in</strong>gcapacity of the fiber. Thus, it becomes necessary to know thedispersion properties of an optical fiber.In this work, the dispersion properties of solid-corephotonic crystal fibers with d/= 0.1-0.9 ratios are analyzedfor both the fixed diameter (d=0.84 m) and the fixed pitch(=4 m) at 0.8-2.0 m wavelength range.The cross-section of fiber used <strong>in</strong> the dispersioncalculations is shown <strong>in</strong> Fig.1. Here is the pitch length and dis the diameter of air- holes. The fiber core is silica and it isformed by remov<strong>in</strong>g 7 air-holes from the structure. Thecladd<strong>in</strong>g is the two dimensional photonic crystal with 4-r<strong>in</strong>gsof the triangular lattice air-holes <strong>in</strong> the silica matrix.Fig. 1.The cross- section of the solid core PCFconsidered. is the pitch length and d isthe diameter of air-holes.The dispersion D is given as follow<strong>in</strong>g [9]:2λ d neffD = −2c dλn is the effective <strong>in</strong>dex of guided mode andeffλ is the freespace wavelength. Firstly, for the fixed pitch length = 4.2m, the dispersion properties are <strong>in</strong>vestigated by vary<strong>in</strong>g thediameters of air-holes for the d/ values of (0.1, 0.3, 0.5, 0.7,0.9). Later, a similar <strong>in</strong>vestigation is executed for the fixeddiameter of air-hole with d=0.84 m, by vary<strong>in</strong>g the pitchlength correspond<strong>in</strong>g to the same d/ values.The variations of the d/ ratios for a given wavelengthaffect the dispersion <strong>in</strong> a considerable manner. The variationof the d/ ratios also changes the zero-dispersion wavelengthwith<strong>in</strong> a large wavelength range comparatively. In the case offixed pitch, the variation of the d/ ratios does not affect thedispersion and zero-dispersion wavelength severely. As aresult, for a dispersion tailor<strong>in</strong>g, the configurations with fixeddiameter are more effective.*Correspond<strong>in</strong>g author: halimedemir@erciyes.edu.tr[1] J. C. Knight, T. A. Birks, P. St. J. Russell and D. M. Atk<strong>in</strong>, Opt. Lett. 21,1547-1549 (1996).[2] J. C. Knight, Nature 424, 847-851 (2003).[3] Arismar Cerqueira S. Jr., F. Luan et al., Opt. Express 14, 926-931 (2006).[4] T. A. Birks., J. C. Knight, , P. S. J. Russell., Opt. Lett. 22, 961-963 (1997).[5] A. Ortigosa-Blanch et al., Opt. Lett. 25, 1325-1327 (2000).[6] W. J. Wadsworth et al., J. Opt. Soc. Am. B 19, 2148-2155 (2002).[7] M. D. Nielsen, J. Folkenberg, N. Martensen and A. Bjarklev, OpticsExpress 12, 430-435 (2004).[8] S. Konorov , A. Zheltikov and M. Scalora, Optics Express 13, 3454-3459(2005).[9] J. K. Ranka and R. S. W<strong>in</strong>deler, Opt.& Photon. News, 20-25 (2000).d6th Nanoscience and Nanotechnology Conference, zmir, 2010 618
PP mPP vs.P =P,PP (1)P andPoster Session, Thursday, June 17Theme F686 - N1123Influence of Anneal<strong>in</strong>g Conditions on Optical Properties of ZnO Th<strong>in</strong> Films111111UDerya BaharUP P*, Göknil BabürP P, S<strong>in</strong>an DikenP P, Tuba Aye TermeliP P, Banu ErdoanP P, Sava SönmezoluPPand Güven ÇankayaP1PDepartment of Physics, Faculty of Arts and Science, Gaziosmanpaa University, Tokat 60250, TurkeyAbstract-ZnO th<strong>in</strong> films were deposited on soda lime glass substrates by sol–gel sp<strong>in</strong>-coat<strong>in</strong>g technique. The optical properties of ZnO th<strong>in</strong> filmsare <strong>in</strong>vestigated for different anneal<strong>in</strong>g temperatures. The optical band gaps of th<strong>in</strong> film are found to vary with anneal<strong>in</strong>g temperatures. Theobta<strong>in</strong>ed films are also transparent <strong>in</strong> the UV- visible region1Z<strong>in</strong>c oxide (ZnO) as a wide-band-gap semiconductor hasattracted much attention <strong>in</strong> current semiconductor research,due to its superior optical properties. In addition, ZnO is aversatile semiconductor material, which has attracted attentionfor its wide range of applications, such as th<strong>in</strong> films, solarcells, lum<strong>in</strong>escent, electrical and acoustic devices andchemical sensors [1-2].In this paper, we report the <strong>in</strong>vestigation of ZnO th<strong>in</strong> filmsprepared by sol-gel sp<strong>in</strong> coat<strong>in</strong>g process us<strong>in</strong>g z<strong>in</strong>c acetate(ZnAc). The optical characterization is <strong>in</strong>vestigated fordifferent anneal<strong>in</strong>g temperatures us<strong>in</strong>g Perk<strong>in</strong> Elmer Lambda35 UV-<strong>VI</strong>S Spectrometer at room temperature.Transmittance (%)100806040200200 400 600 800 1000 1200Wavelenght (nm)200 C 0300 C 0400 C 0500 C 0Figure 1. UV–<strong>VI</strong>S spectra of the ZnO th<strong>in</strong> film for varioustemperatures.In order to prepare a ZnO solution, first, 3.35gr z<strong>in</strong>c acetate(Zn(CHR3RCOO)R2R·2HR2RO, Merck), used as a precursor, wasdissolved <strong>in</strong> 50 ml ethanol [CR2RHR6RO, Merck] and stirred for 50m<strong>in</strong> at 60 P PC <strong>in</strong> a magnetic mixture. Then, 5 ml glacial aceticacide [CR2RHR4ROR2R, Merck] and 1.5 ml hydrochloride acid (HCl,Merck) were added <strong>in</strong> the solution, and the f<strong>in</strong>al solution wassubjected to the magnetic mixture for 2 h. Here, glacial aceticacid and hydrochloride acid were used as an <strong>in</strong>hibitor to slowdown the z<strong>in</strong>c acetate fast hydrolysis. Prior to the coat<strong>in</strong>gprocess, the glass was washed with water, ultrasonicallycleaned <strong>in</strong> ethanol for 20 m<strong>in</strong>, and <strong>in</strong> acetone for 20 m<strong>in</strong>,respectively. The deposition was carried out at a sp<strong>in</strong>n<strong>in</strong>gspeed of 3000 rpm for 30 s. The sp<strong>in</strong> coat<strong>in</strong>g procedure was0 0 0cont<strong>in</strong>uously repeated five times at 200P PC, 300P PC, 400P PC and0500P PC anneal<strong>in</strong>g temperatures on glass substrate.Fig. 1 shows the UV–<strong>VI</strong>S spectra ZnO th<strong>in</strong> films fordifferent anneal<strong>in</strong>g temperatures <strong>in</strong> wavelength range 300–1100nm. The transmission of the th<strong>in</strong> films of z<strong>in</strong>c oxidedecreases with the <strong>in</strong>crease <strong>in</strong> anneal<strong>in</strong>g temperature. This canbe l<strong>in</strong>ked with the <strong>in</strong>crease <strong>in</strong> the gra<strong>in</strong> size, and <strong>in</strong>dicat<strong>in</strong>g itshigh surface roughness and <strong>in</strong>homogeneity [3].(h v) 2 (eV/m) 220161284200 C 0 , E g= 3.84 eV300 C 0 , E g= 3.74 eV400 C 0 , E g= 3.67 eV500 C 0 , E g = 3.58 eV02.4 2.8 3.2 3.6 4Photon energy (eV)Figure 2. UV–<strong>VI</strong>S spectra of the ZnO th<strong>in</strong> film for varioustemperatures.The optical band gap of the film was calculated by thefollow<strong>in</strong>g relation [4]:(hv) = A (hv - ERgR) P7where A is an energy-<strong>in</strong>dependent constant between 10P8 -110PP, Eg is the optical band gap and r is a constant, whichdeterm<strong>in</strong>es type of optical transition, r = 1/2, 2, 3/2 or 3 forallowed direct, allowed <strong>in</strong>direct, forbidden direct andforbidden <strong>in</strong>direct electronic transitions, respectively [4]. The1/rr(hv)P hv curves were plotted for different r values andthe best fit was obta<strong>in</strong>ed for r = ½. The film at variousanneal<strong>in</strong>g temperatures shows a direct allowed transition. Theoptical band gap was determ<strong>in</strong>ed by extrapolat<strong>in</strong>g the l<strong>in</strong>ear2portion of the plots to (hv)P 0. The optical band gaps of theth<strong>in</strong> film were found to be 3.84, 3.74, 3.67 and 3.58 eV at 200 °C,300 °C, 400 °C and 500 °C anneal<strong>in</strong>g temperature, respectively.The thicknesses of ZnO film were also determ<strong>in</strong>ed fromtransmittance measurements <strong>in</strong> Fig.1 and found to be 1361, 692,939 and 660 nm, respectively. The optical band gap decreaseswith the <strong>in</strong>creas<strong>in</strong>g anneal<strong>in</strong>g temperatures. The decrease <strong>in</strong>the optical band gap is attributed to the lower<strong>in</strong>g of the<strong>in</strong>teratomic spac<strong>in</strong>g, which may be associated with a decrease<strong>in</strong> the amplitude of atomic oscillations around theirequilibrium positions [5].In summary, the analysis of the transmission spectra showsthat ZnO th<strong>in</strong> films are transparent <strong>in</strong> the UV-visible regionirrespective of the anneal<strong>in</strong>g temperatures. This work waspartially supported by the Scientific Research Commission ofGaziosmanpaa University (Project No: 2009/29).*Correspond<strong>in</strong>g author: HTbhr_dry@hotmail.comT[1] Y. Chen, D.M. Bagnall, Z. Zhu, T. Sekiuchi, K. Park, K. Hiraga,T. Tao, S. Koyama, M.Y. Shen, T. Goto, J. Cryst. Growth 181 (1997)165.[2] S. Saito, M. Miyayama, K. Koumoto, H. Yanagida, J. Am. Ceram.Soc. 68 (1985) 40–43[3] K. Liu, X. Wu, B. Wang, Q. Liu, Mater. Res. Bull. 37 (2002)2255.[4] J. Tauc, Mater. Res. Bull. 5 (1970) 721.[5] S. Sönmezolu, G. Çankaya,P PN. Ser<strong>in</strong>, T. Ser<strong>in</strong>, Int. Conf. onNanomaterials and Nanosystems, 10-13 August 2009, p. 129.6th Nanoscience and Nanotechnology Conference, zmir, 2010 619
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