The lasers are sources of light with very special properties that emit light based on the stimulated emission of electromagnetic radiation. There is a great variety of laser applications but most of them are used only for specialised research [1] -[26] . The copper vapor lasers (CVLs) are one of the efficient sources of coherent light in visible region at 510.6 nm and 578.2 nm with high average output powers [27] . CVLs have wide applications in the research, medicine and industry and have been used extensively in high speed imaging, micro-machining, non-linear frequency conversion to the ultraviolet and photodynamic therapy. Moreover, they have considered as a powerful pumping source for dye lasers [27] - [31] , particularly by means of a master oscillator-power amplifier array, in order to satisfy higher output powers and beam quality simultaneously [32] [33] . The output power of CVL involved many factors and the type of buffer gas only had some influences on it. It could be finding that the fluctuations of the output power of CVL based on the type of buffer gas are not very slight. The buffer gas is employed in CVL tube to increase the output power and improve the laser performance [34] [35] . It provides a discharge medium before reaching the discharge tube to the temperature required for copper vapor production. The buffer gas is necessary to produce the population inversion mechanism via energy transfer of the gas, ions or electrons to the metal atoms. It shapes the electron-energy-distribution function through elastic collisions. It also protects the windows against contamination and transfers heat from tube axis to the walls. Addition of a buffer gas allows the impedance of the discharge tube to increase, thus leads to improving impedance matching by the excitation circuit [29] . In CVLs, the non-reactive inert gases with high excitation and ionization energies have been used as the buffer gases to minimize the influence of inelastic electron collisions on the electron energy distribution function. Among of the He, Ne, Ar, Kr, Xe and their mixtures gases, neon enables laser oscillation at the highest gas pressure and provides the highest output power [36] . The next best buffer gas to use is He, which gives longer and lower discharge current pulses [28] . Weak oscillations are also obtained with N₂ [37] , H₂ [38] , and CO₂ buffer gases [39] . Adding of H₂ to the Ne buffer gas in CVL greatly enhances its performance [38] [40] [41] . In our previous work, a CVL and a gold vapor laser were operated using air as a buffer gas to compare output power and the stability of the laser by the air and other gases [42] . Also, we used a pair of CVL in the oscillator-amplifier configuration for investigating the small-signal gain and the intensity saturation as the amplifying parameters, versus the pressure of various types of buffer gases. It is shown that the small- signal gain increases and the intensity saturation decreases with increase in the air pressure. Moreover, the values of these parameters are different for various gases used in the amplifier media [43] . The amplifying parameters, and then output power, and interval of operational pressure of CVL have been strongly affected by buffer gas. In this work, a CVL has been operated by using some different buffer gases such as the He, Ne and air. Some similar works have been studied generally, which investigated the effects of buffer gas pressure and some additive gases on CVL output characteristics. In this work, the behavior of the laser output power versus gas flow rate of these gases has been investigated to obtain the optimum conditions. It is shown that the gas flow rate is depending upon the type of buffer gas. However, abundance of the air and reduction of the system volume due to eliminating the gas handling as well as the economically benefits are the advantages of employing air as a buffer gas in CVL operation in some researches or educational cases. The rest of this paper is as follows. Section 2 describes the experimental setup. The obtained results and discussion are presented in Section 3. Finally, we conclude in Section 4.

The discharge tube of CVL has been made of Alumina with inner diameter of 16 mm and active medium length of 60 cm, surrounded by a fibrous alumina insulation covering with a Pyrex tube and an external stainless steel jacket. Two cylindrical electrodes made of molybdenum are employed for discharging. A couple of flat-flat resonator with reflectivity of 98% and 4% are considered as the back and front mirrors, respectively. The laser tube is coupled to the standard driven circuit as illustrated in Figure 1. The gas on the tube is excited by the discharge of a 1.65-nF main capacitor (C_s) through the TGI1-1000/25 Thyratron, which is cooled by air. A 0.68- nF peaking capacitor (C_p) is connected between the tube electrodes as well as the 0.15 mH inductance (L₂).

The laser output is measured by a Molectron^TM PM500D power meter. Precision needle valve is used to control the gas flow rate and a gauge is used to pressure measuring of buffer gas in the tube.

In our work, three gases, Ne, He, and air have been used as buffer gas individually, and the output powers are measured under same conditions, that is, the electrical input power is kept at 1.7 kW and the pulse repetition frequency is fixed at 20 kHz. The output power of 6, 4 and 1.9 W are obtained with Ne, He and air gases with the optimum pressure of 30, 20 and 3.8 torr, respectively. The laser output powers with these gases are measured versus gas flow rates, individually. The results are shown in Figure 2. It is finding that the laser output power increased by the gas flow rate, first, and after reaching to a maximum value, it reduces at higher flow rates. The maximum output power is achieved by using of Ne, and minimum one is obtained by air as buffer gas. The optimum values of gas flow rate of He and Ne are approximately 15 and 12 Lit/min, respectively, but this one is 23

Lit/min for air, which gives the maximum output powers. It is shown that the optimum value of air flow rate is more than that of other gases, due to existence of small percent of hydrogen in air which improve the output power of laser.

At low flow rate, the output power would be increased. The flow rate is maintained to permit the excited metal atoms to emit laser radiation by stimulated emission to a lower laser level in the discharge region and to remove the lower laser level atoms. Moreover, the impurities at a low flow rate would be removed. There is an optimum flow rate, which the maximum output power is obtained. By increasing of flow rate more than its optimal value, the output power is decreased, because of at higher flow rates, the electron energy function distribution and temperature rise across the length of the tube are altered, which affected on population inversion. It could be finding that the performance of CVL has strongly dependent on the type of buffer gas.

The type of buffer gas has been strongly influencing the output power of CVL. The results show that the gas flow rate is depending upon the type of gas. The optimum of air flow rate is higher than that of other conventional gases, due to the existence of the small percent of hydrogen in the air, which improves the output power of laser.

SaeidBehrouzinia,KamranKhorasani,SaeidMarjani,MasoudSabaghi,Mohammad EbrahimAeinehvand,SadeghMohammadpour, (2016) Experimental Study of Buffer Gas Flow Rate Effect on Output Power of a Copper Vapor Laser. Optics and Photonics Journal,06,24-28. doi: 10.4236/opj.2016.62004