共查询到20条相似文献,搜索用时 15 毫秒
1.
Amit Pratap Singh Avinashi Kapoor K. N. Tripathi G. Ravindra Kumar 《Optics & Laser Technology》2002,34(1):1583-43
A comparative study of damage morphology in GaAs induced by s- , p- and linearly polarized laser light (1.064 μm, 35 ps) is presented. For linearly polarized light damage initiates in the form of pits. This material damage occurs below the surface. For s- or p-polarized light material damage involves only the surface layer. For larger fluences or number of pulses the differences are less marked and the damage morphology occurs in a similar manner either for linearly polarized or s- or p-polarized light. Ripples are formed when multiple irradiation is used due to interference between the front and back faces of the test sample. The spacing of these ripples is 3 μm, which is in good accordance with the reported work of Guosheng et al. (Phys. Rev. B 26 (1982) 5366). 相似文献
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Using generalized Ginzburg-Landau equations derived recently we solve the laser equations analytically for the case of spontaneous ultra-short laser pulses. The results are compared with previous computer solutions by Risken and Nummedal and very good agreement is found. 相似文献
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U. Chakravarty P. A. Naik J. A. Chakera A. Upadhyay P. D. Gupta 《Applied Physics A: Materials Science & Processing》2014,115(4):1457-1467
A simple technique, based on the interference principle, to obtain simultaneously the instantaneous electron density and temperature of ultra-short laser-excited semiconductor surface plasma is proposed and demonstrated. The interference of the incident laser and the surface plasmons forms nano-ripples on the surface. From the observed nano-ripple period, one can easily retrieve the density and temperature information. As a demonstration of the technique, the electron density and temperature are obtained for various band gap semiconductor materials based on the experimentally observed nano-ripples using 800 and 400 nm light in various ambient media and incident angles. The electron density estimated varied in the range of 2 $n_{\mathrm{c} }$ –10 $n_{\mathrm{c}}$ and the corresponding electron temperature in the range 10 $^{4}$ –10 $^{5}$ K, depending on the material band gap, the incident laser intensity, the ambient medium, the angle of incidence, and the laser wavelength. The information of the electron density and temperature is useful for choosing laser parameters (like fluence, wavelength, angle of incidence, ambient medium) and target materials (different band gap semiconductors) for obtaining a better size controllability of the nanostructure production. The information can also help one in obtaining essential plasma parameter inputs in the quest for understanding ultra-fast melting or understanding the pre-plasma conditions created by the pre-pulse of ultra-high intensity laser pulses. 相似文献
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Spatially localized femtosecond pulses have been produced by a combination of scanning near-field optical microscopy with ultrashort pulse lasers. With these pulses direct ablative writing on metal surfaces is demonstrated. Possible applications of this technique for nanostructuring, repair, and production of lithographic masks are discussed. 相似文献
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In this study, the surface morphology and structure of dentin after ablation by ultra-short pulses were evaluated using environmental scanning electron microscopy (ESEM) and atomic force microscopy (AFM). The dentin specimens examined were irradiated by a chirped-pulse-amplification (CPA) Ti:sapphire laser (800 nm) and the optimal conditions for producing various nanostructures were determined. Based on the ESEM results, it was possible to identify an energy density range as the ablation threshold for dentin. The laser-induced damage was characterized over the fluence range 1.3-2.1 J/cm2. The results demonstrate that by selecting suitable parameters one can obtain efficient dentin surface preparation without evidence of thermal damage, i.e., with minimized heat affected zones and reduced collateral damage, the latter being normally characterized by formation of microcracks, grain growth and recrystallization in the heat affected zones. 相似文献
6.
The nanostructures with dimensions (110–250 nm), much smaller than the wavelength of laser light, obtained on surfaces of
various semiconductors under the action of laser ablation by femtosecond pulses are studied. Nanostructures obtained at large
angles of incidence and under the action of interference of two femtosecond pulses on the surface of the samples are analyzed.
Original Russian Text ¢ R.A. Ganeev, T.Q. Jia, 2008, published in Optika i Spektroskopiya, 2008, Vol. 105, No. 1, pp. 154–159. 相似文献
7.
The particle size distribution, morphology and optical properties of the Au nanoparticle (NP) structures for surface enhanced
Raman signal (SERS) application are investigated in dependence on their preparation conditions. The structures are produced
from relatively thin Au films (10–20 nm) sputtered on fused silica glass substrate and irradiated with several pulses (6 ns)
of laser radiation at 266 nm and at fluencies in the range of 160–412 mJ/cm2. The SEM inspection reveals nearly homogeneously distributed, spherical gold particles. Their initial size distribution of
the range of 20–60 nm broadens towards larger particle diameters with prolonged irradiation. This is accompanied by an increase
in the uncovered surface of the glass substrate and no particle removal is observed. In the absorption profiles of the nanostructures,
the broad peak centred at 546 nm is ascribed to resonant absorption of surface plasmons (SPR). The peak position, halfwidth
and intensity depend on the shape, size and size distribution of the nanostructured particles in agreement with literature.
From peak intensities of the Raman spectra recorded for Rhodamine 6G in the range of 300–1800 cm−1, the relative signal enhancement by factor between 20 and 603 for individual peaks is estimated. The results confirm that
the obtained structures can be applied for SERS measurements and sensing. 相似文献
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We have measured the absolute dissociation probability of SF6 gas irradiated by CO2 laser pulses varying in duration from 0.5 nsec to 100 nsec. We find a threshold for dissociation of ? 1.4 J/cm2, independent of pulse duration. For fixed energy density, the dissociation probability increases as the pulse duration decreases, but not nearly to the degree expected from theory. We have also determined the dissociation probability in the ν2 + ν6 combination band and find it to be 103 times less than in the ν3 band, in contradiction to some conclusions recently reported by Ambartzumian et al. The dissociation mechanism takes place without collisions, and if collisions occur, they tend to be detrimental to the dissociation rate. 相似文献
10.
We demonstrate an optical limiter for ultra-short (∼100-fs) laser pulses. The device has a dynamic range (= damage energy/onset-of-limiting
energy) of more than 10000 and an onset-of-limiting energy of only ∼10 nJ. The output-pulse energy is kept below 1.3 μJ. The
limiting mechanism is based on two-photon absorption and refractive nonlinearities in a 20-mm piece of ZnSe. We discuss the
importance of the different nonlinearities, damage issues, and guidelines for the construction of the device.
Received: 20 December 2001 / Revised version: 25 March 2002 / Published online: 8 May 2002 相似文献
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本文数值计算了超短脉冲(脉冲持续时间为两个光学周期)的高次谐波发射功率谱.研究结果表明,超短脉冲谐波谱的截止频率不再符合IP 3.17UP的截止规则(IP为原子电离势,UP为有质动力能).对此,本文采用"三步"模型给出了合理解释,并用小波变换验证了结果的正确性. 相似文献
13.
Masatoshi Ohnishi Hirokazu Shikata Masaaki Sakakura Yasuhiko Shimotsuma Kiyotaka Miura Kazuyuki Hirao 《Applied Physics A: Materials Science & Processing》2010,98(1):123-127
Micro machining of a polyimide film with ultra-short pulsed laser was demonstrated. A through-hole with a diameter of less than 10 μm could be produced by optimizing the pulse duration, repetition rate, and number of shots. Thermal damage around the through-hole can be made negligibly small when the pulse duration was shorter than 140 fs. We also found that the minimum shot number needed for the creation of a through-hole becomes smaller as the repetition rate of laser shot increases. On the basis of the optimum irradiation condition, we demonstrated laser cutting of a polyimide film without thermal damage and copper filling in through-holes with diameters of 9 μm by a plating process. 相似文献
14.
Lu Xue Jianjun Yang Yang Yang Yishan Wang Xiaonong Zhu 《Applied Physics A: Materials Science & Processing》2012,109(2):357-365
Formation of periodic subwavelength ripples on a metallic tungsten surface is investigated through a line-scribing method under the irradiation of 800?nm, 50 fs to 8 ps ultra-short laser pulses. The distinctive features of the induced ripple structures are described in detail with different laser parameters. Experimental measurements reveal that with gradual decrease of the laser fluence, the pulse duration or the scanning speed, the ripple period is inclined to reduce but the ripple depth tends to become pronounced. Theoretical analyses suggest that the transient dielectric function change of the tungsten surface mainly originates from the nonequilibrium distribution of electrons due to the d-band transitions. A sandwich-like physical model of air?Cplasma?Ctarget is proposed and the excitation of a surface plasmon polaritonic (SPP) wave is supposed to occur on the interface between the metallic target and the electron plasma layer. Formation of ripples can be eventually attributed to the laser?CSPP interference. Theoretical interpretations are consistent with the experimental observations. 相似文献
15.
J.R. Vázquez de Aldana L. Plaja I.J. Sola L. Roso 《Applied physics. B, Lasers and optics》2007,88(1):5-11
We demonstrate the possibility of imprinting a controlled ultra-fast time-varying ellipticity on few-cycle laser pulses through
the non-linear propagation in a thin anisotropic crystal. The method is based on the self- and cross-phase modulation induced
by the third-order (Kerr) non-linearity when the pulse propagates through the crystal. The feasibility of this technique is
demonstrated through the numerical integration of the Maxwell equations, showing the possibility of producing a sub-half-cycle
temporal gate of linear polarization. In comparison with alternative approaches, our method results in a polarization gate
with higher efficiency, and also it can be controlled by changing the polarization axis of the laser pulse at the entrance
of the crystal. We finally demonstrate the efficiency of this scheme in the generation of single attosecond pulses.
PACS 42.81.Gs; 42.65.Re; 32.80.Wr 相似文献
16.
H. Strehlow 《Applied Physics A: Materials Science & Processing》1997,65(4-5):355-360
Received: 5 June 1997/Accepted: 13 June 1997 相似文献
17.
The damage morphology of germanium surfaces using femtosecond laser pulses of various fluences and number of pulses is reported. The single pulse damage threshold in the present experiment was 9.7±4.0×10−13 W/cm2. The experimental threshold value was compared with theory, considering the damage threshold as the melting threshold. The cooling rate calculated on the basis of present results is 2.4×1015°C/s. Recrystallization was the common feature of the damage morphology. For fluences greater than the single pulse damage-threshold micropits and spherical grains of micron size were formed in the damaged surface. Ablation (surface removal) was also observed at higher fluences (at two or three times of damage threshold value). The damage morphology, induced by multiple pulses, was unaffected for linear and circular polarization. 相似文献
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Highly-chirped dissipative solitons of the cubic-quintic Ginzburg-Landau equation found in this work may provide a roadmap to design passively mode-locked laser oscillators that generate pulses of extremely high energy. We provide a region in the space of the system parameters where high-energy dissipative solitons are found, along with their typical spectral and temporal features. 相似文献