# Ag Nanoparticles: Experimental Study of  Sign Identification of Nonlinear Refractive Index by  Moiré Deflectometry and Z-Scan Methods

Authors: Adeleh Granmayeh Rad; Khosro Madanipour; Ata Koohian
Journal: ISRN Nanomaterials
 (2013)

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## Abstract

Two different methods are presented for the sign identification of nonlinear refractive index (n2) of Ag colloidal nanoparticles which are based on nonscanning Moiré deflectometry and Z-scan. In the Moiré deflectometry setup, two lasers are used, one is used as pump laser which causes thermal nonlinear effects in the sample, and the second one is used as the probe laser for monitoring these effects by Moiré deflectometry system. By observing the deflected Moiré fringes, we can determine the sign of nonlinear refractive index in real time, and there would be no need for calibration or complicated calculations. The second technique for sign identification is Z-scan. In this technique, a CW 532 nm second harmonic Nd:YAG laser with a beam power of 55 mW is used as the excitation source. Results show that the nonlinear refractive index is negative for Ag nanoparticles in pure water by both methods.


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## Body

## 1. Introduction

Measurements of nonlinear optical parameters of colloidal metallic nano-particles have drawn a lot of attentions because of their fast nonlinear optical response and high nonlinearity ability [1]. Colloidal metallic solutions are frequently used in the design of optical instruments and photonic limiters because of their photoinduced nonlinear properties [2, 3]. There are two standard and usual methods for sign identification of nonlinear refractive index of nanoparticles, Z-scan [4–7] and Moiré deflectometry techniques [8–13]. In Z-scan method, the refractive index and the sign are found by drawing the diagram of the z dependence of the transmitted beam intensity but in Moiré deflectometry technique, these are found by observing the Moiré fringes patterns [14]. It has also been shown that Moiré method is simpler and more robust than other methods [15]. In recent years, sign identification of third nonlinear refractive index of materials by Moiré deflectometry technique is found by observing size of Moiré fringes and Moiré fringes spacing curves [16, 17]. This technique avoids the requirement of highly calibrated detectors, but still, the need to use a scanner that is highly sensitive to movements exists. In our recent work, we have proposed a novel Moiré deflectometry technique that not only avoids the use of highly sensitive calibrated detectors but also omits the need for scanner [18].The presented methods in this paper which are based on scanning (Z-scan) and nonscanning (Moiré deflectometry) techniques have been used to identify the sign of the nonlinear refractive index of Ag nano-particles suspended in water.


## 2. Experimental

### 2.1. Material Processing

The samples of Ag nano-particles for this study were fabricated by the laser ablation method. The synthesis procedure has been detailed elsewhere [19]. The average size of fabricated nano-particles is ~20 nm and is obtained through the transmission electron microscopy (TEM) technique, Figure 1. The linear absorption spectra of Ag nanoparticles are shown in Figure 2. Absorption peak happens at near 400 nm.Figure 1
Image of silver nanoparticles fabricated during laser ablation technique by method of transmission electron microscopy.Figure 2
Absorption spectra of Ag nanoparticles.


### 2.2. Moiré Deflectometry Method

In this technique a Gaussian laser beam with a high intensity as a pump beam is emitted to the sample (Laser2). This beam causes nonlinear effects in the sample which will lead to changes in the refractive index in the sample environment. An expanded beam of low intensity will be emitted perpendicularly on the pump beam (Laser1). The sign of nonlinear refractive index is determined only usign the probe beam without any further calculation. The block diagram of the experiment for Moiré deflectometry method is depicted in Figure3.Figure 3
The experimental setup of Moiré deflectometry for sign identifying nonlinear refractive index, (a): Laser1 (probe laser); 15 mW He-Ne laser, Laser2 (pump laser); 47 mW green laser, F; filter, SF; spatial filter, G1, G2; grating, L1, L2, and L3; lenses with the focal lengths of f1=50 mm, f2=150 mm, and f3=250 mm, S sample, P; the pinhole, CCD; the camera, Com; the computer.The intensity-dependent refractive indexn, is defined as [20]:
(1)n=n0+Δn=n0+n2I,
where n0 is the first refractive index, n2 is the second order of refractive index, and I is the intensity of the incident pump beam which causes nonlinear effects. The difference between refractive index of interaction zone and other area of sample creates a cylindrical lens which is shown in Figure 4.Interaction zone between guide laser beam and nonlinear environment. (a) A convex lens as a result of positive refractive index. (b) A concave lens as a result of negative refractive index.
(a)
(b)According to lens-makers formula, the focal length of this lens can be written as [21]:
(2)1f=(n-n0)[1R1-1R2],
where R1 and R2 are the first and second radius of lens, respectively, and are equal to the pump laser beam radius R. By usign (1) and (2), the focal length of cylindrical lens created by the nonlinear effects will be
(3)f=R2n2I.
Equation (3) shows that concave or convex lenses are generated as a result of negative or positive nonlinear refractive indexes of sample, respectively. Convergence or divergence of probe beam illuminated on the generated cylindrical lens will determine the sign of nonlinear refractive index. The convergence of the beam corresponds to positive (n2>0) and divergence of the beam corresponds to negative (n2<0) nonlinear refractive index [18].


### 2.3. Z-Scan Method

We used the Z-scan method as the second method to investigate sign identification of nonlinear refractive index of silver nano-particles. The experimental setup is shown in Figure5. In Z-scan method, the scanning starts from a distance far away from the focus (negative z), and when the sample is brought closer to the focus, the beam irradiance increases leading to self-lens effect in the sample. In negative nonlinearity, a negative self-lens effect occurs prior to focus which tends to collimate the beam and reduces the diffraction leading to a smaller beam at the aperture and an increased transmittance. As the sample crosses the focal plane to the right (positive z), the diffraction of the beam will, change and the aperture transmittance will be reduced due to the same self-defocusign effect. Therefore, prefocal transmittance maximum (peak) and postfocal transmittance minimum (valley) are the representatives of the negative sign of nonlinear refractive index as shown by the peak-valley configuration. Following the same analogy, the Z-scan signature of a positive nonlinearity will give rise to an opposite valley-peak configuration. Figure 6 depicts these two configurations. Z-scan method requires sensitive and calibrated detector which makes the accuracy of measurements dependent on the accuracy of detector’s response.Figure 5
The experimental setup for measuring optical nonlinearity by use of the Z-scan technique, and D1 and D2 are detectors for beam intensity detection.Figure 6
Z-scan theoretical curves of the transmittance as a function ofz.


## 2.1. Material Processing

The samples of Ag nano-particles for this study were fabricated by the laser ablation method. The synthesis procedure has been detailed elsewhere [19]. The average size of fabricated nano-particles is ~20 nm and is obtained through the transmission electron microscopy (TEM) technique, Figure 1. The linear absorption spectra of Ag nanoparticles are shown in Figure 2. Absorption peak happens at near 400 nm.Figure 1
Image of silver nanoparticles fabricated during laser ablation technique by method of transmission electron microscopy.Figure 2
Absorption spectra of Ag nanoparticles.


## 2.2. Moiré Deflectometry Method

In this technique a Gaussian laser beam with a high intensity as a pump beam is emitted to the sample (Laser2). This beam causes nonlinear effects in the sample which will lead to changes in the refractive index in the sample environment. An expanded beam of low intensity will be emitted perpendicularly on the pump beam (Laser1). The sign of nonlinear refractive index is determined only usign the probe beam without any further calculation. The block diagram of the experiment for Moiré deflectometry method is depicted in Figure3.Figure 3
The experimental setup of Moiré deflectometry for sign identifying nonlinear refractive index, (a): Laser1 (probe laser); 15 mW He-Ne laser, Laser2 (pump laser); 47 mW green laser, F; filter, SF; spatial filter, G1, G2; grating, L1, L2, and L3; lenses with the focal lengths of f1=50 mm, f2=150 mm, and f3=250 mm, S sample, P; the pinhole, CCD; the camera, Com; the computer.The intensity-dependent refractive indexn, is defined as [20]:
(1)n=n0+Δn=n0+n2I,
where n0 is the first refractive index, n2 is the second order of refractive index, and I is the intensity of the incident pump beam which causes nonlinear effects. The difference between refractive index of interaction zone and other area of sample creates a cylindrical lens which is shown in Figure 4.Interaction zone between guide laser beam and nonlinear environment. (a) A convex lens as a result of positive refractive index. (b) A concave lens as a result of negative refractive index.
(a)
(b)According to lens-makers formula, the focal length of this lens can be written as [21]:
(2)1f=(n-n0)[1R1-1R2],
where R1 and R2 are the first and second radius of lens, respectively, and are equal to the pump laser beam radius R. By usign (1) and (2), the focal length of cylindrical lens created by the nonlinear effects will be
(3)f=R2n2I.
Equation (3) shows that concave or convex lenses are generated as a result of negative or positive nonlinear refractive indexes of sample, respectively. Convergence or divergence of probe beam illuminated on the generated cylindrical lens will determine the sign of nonlinear refractive index. The convergence of the beam corresponds to positive (n2>0) and divergence of the beam corresponds to negative (n2<0) nonlinear refractive index [18].


## 2.3. Z-Scan Method

We used the Z-scan method as the second method to investigate sign identification of nonlinear refractive index of silver nano-particles. The experimental setup is shown in Figure5. In Z-scan method, the scanning starts from a distance far away from the focus (negative z), and when the sample is brought closer to the focus, the beam irradiance increases leading to self-lens effect in the sample. In negative nonlinearity, a negative self-lens effect occurs prior to focus which tends to collimate the beam and reduces the diffraction leading to a smaller beam at the aperture and an increased transmittance. As the sample crosses the focal plane to the right (positive z), the diffraction of the beam will, change and the aperture transmittance will be reduced due to the same self-defocusign effect. Therefore, prefocal transmittance maximum (peak) and postfocal transmittance minimum (valley) are the representatives of the negative sign of nonlinear refractive index as shown by the peak-valley configuration. Following the same analogy, the Z-scan signature of a positive nonlinearity will give rise to an opposite valley-peak configuration. Figure 6 depicts these two configurations. Z-scan method requires sensitive and calibrated detector which makes the accuracy of measurements dependent on the accuracy of detector’s response.Figure 5
The experimental setup for measuring optical nonlinearity by use of the Z-scan technique, and D1 and D2 are detectors for beam intensity detection.Figure 6
Z-scan theoretical curves of the transmittance as a function ofz.


## 3. Experimental Results and Discussions

We have examined the Moiré deflectometry technique for measuring the nonlinear refractive index in colloidal Ag nano-particles. To identify the sign of nonlinear refractive index of the sample, the experiment was set up as shown in Figure3; a 15 mW He-Ne laser beam has been used as a probe beam, which has been expanded and collimated by lenses L1, L2 and a spatial filter. This beam will then pass the nano-particles, which is in a Quartz cell with 10 mm thickness. As the laser beam passes through grating G1 and G2, Moiré fringe patterns are projected on a CCD camera by lens L3 and recorded by a computer. A 47 mW second harmonic Nd:YAG laser is used as pump laser, and the beam is emitted to the sample. After generating the thermal gradient in the colloidal nano-particles, the deflection of Moiré fringes will appear [18]. By choosign the appropriate coordinates as shown in Figures 7 to 8 and rotating the grating along the Z axes, we can observe the effect of rotation of the first grating on the Moiré fringe patterns. As shown in Figure 9, the deflected Moiré fringes were determined for Ag nano-particles. By changing direction of first grating angle, the deflected Moiré fringes change patterns as shown in Figures 9(b) and 9(c). Finally, by knowing the direction of deflected Moiré fringes and the direction of rotation of first grating angle, the sign of nonlinear refractive index of Ag nano-particles was found to be negative.(a) The experimental setup forn2<0, θG1>0, (b) deflection of Moiré pattern; the red dashed lines show the movement of the grating vector image, in which Gi is grating, L is lens, and di and dm are the pitches of grating and Moiré fringes, respectively.
(a)
(b)(a) The experimental setup forn2<0, θG1<0, (b) deflection of Moiré pattern; the red dash lines show the movement of the grating vector image, in which Gi is grating, L is lens, and di and dm are the pitches of grating and Moiré fringes, respectively.
(a)
(b)The deflection of Moiré fringes patterns of Ag nano-particles caused by producing refractive index gradient, (a) the Moiré fringes before deflection, (b) the Moiré fringes after deflection,θG1>0, and (c) the Moiré fringes after deflection, θG1<0.
(a)
(b)
(c)Figure4 shows the schematic setup for close-aperture Z-scan experiment. The excitation source was a second harmonic Nd:YAG laser with a beam power of 55 mW and was focused onto the sample by a lens with 10 cm focal length, and the beam waist radius (w0) was measured to be 14.7 μm, and the corresponding Rayleigh length was 1.32 mm. The thickness of the quartz cell containing the sample was 1 mm, which was less than the Rayleigh length of the laser beam. Prefocal transmittance maximum (peak), followed by a post-focal transmittance minimum (valley) for Ag nano-particles, is shown in Figure 10.Figure 10
Z-scan normalized transmittance with close aperture of colloidal Ag nanoparticles. The solid curve is the theoretical fit to the data.


## 4. Conclusion

As shown in this paper, two different methods can be used to identify the sign of thermal nonlinear refractive index, caused by the interaction of a laser beam with the colloidal silver nano-particles in water solution.The proposed Moiré deflectometry technique is a nonscanning method, and the sign of refractive index can be achieved immediately and in real time. By observing the deflection of Moiré fringes, the sign of nonlinear refractive index can be determined. This method is simple, fast, and not sensitive to environment noise and vibration. Also, it does not need calibration or analysis of fringe patterns. Furthermore, the closed aperture of Z-scan technique was used to identify the sign of refractive index of colloidal Ag nano-particles. The Moire deflectometry and Z-scan methods showed that the sign of nonlinear refractive index of colloidal Ag nanoparticles is negative.



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*Source: 327575-2013-10-21.xml*