排序方式: 共有64条查询结果,搜索用时 15 毫秒
21.
Shuxia Gao 《Optik》2010,121(23):2110-2112
We present an experimental study on supercontinuum generation by combining a clad-pumped Er/Yb co-doped fiber amplifier (EYDFA) and a highly nonlinear photonic crystal fiber (HNL-PCF). By using the nonlinear polarization rotation technique, a stable femtosecond optical pulse seed signal with a central wavelength of 1556.36 nm and a spectral line width of ∼5.6 nm has been obtained. Then, this pulsed seed signal is amplified by the EYDFA, the amplified pulse, which, with the broaden spectrum, propagates in the HNL-PCF. The 20 dB bandwidth of ∼520 nm from 1230 to 1750 nm is obtained. 相似文献
22.
Feroza Begum Yoshinori Namihira Tatsuya Kinjo Shubi Kaijage 《Optics Communications》2011,284(4):965-970
This paper presents a simple index-guiding square photonic crystal fiber (SPCF) where the core is surrounded by air holes with two different diameters. The proposed design is simulated through an efficient full-vector modal solver based on the finite difference method with anisotropic perfectly matched layers absorbing boundary condition. The nearly zero ultra-flattened dispersion SPCF with low confinement loss, small effective area as well as broadband supercontinuum (SC) spectra is targeted. Numerical results show that the designed SPCF has been achieved at a nearly zero ultra-flattened dispersion of 0 ± 0.25 ps/(nm·km) in a wavelength range of 1.38 μm to 1.89 μm (510 nm band) which covers E, S, C, L and U communication bands, a low confinement loss of less than 10−7 dB/m in a wavelength range of 1.3 μm to 2.0 μm and a wide SC spectrum (FWHM = 450 nm) by using picosecond pulses at a center wavelength of 1.55 μm. We then analyze the sensitivity of chromatic dispersion to small variations from the optimum value of specific structural parameters. The proposed index-guiding SPCF can be applicable in supercontinuum generation (SCG) covering such diverse fields as spectroscopy applications and telecommunication dense wavelength division multiplexing (DWDM) sources. 相似文献
23.
We present a new design study of ultra-flat near zero dispersion PCF with selectively liquid infiltration with all uniform air-holes in the cladding. The dependence of the individual parameters upon dispersion has been presented in detail. The study establishes that varying Λ influences the total dispersion, whereas d has the desired effect of modifying the dispersion slope, and varying nL modifies both. With the above study we could achieve near zero ultra-flat dispersion as small as 0 ± 0.41 ps/nm/km for broad wavelength range of 452 nm. The optimized near zero ultra-flat dispersion PCF has been targeted for smooth and flat broadband spectrum supercontinuum generation (SCG) for near Infrared (IR) applications. Broadband SC generations corresponding to three different designs of ultra-flat dispersion fiber have been carried out by using picoseconds pulse laser around the first zero dispersion wavelengths (ZDW). The numerical results show that FWHM of around 400 nm with less than a meter long fiber can be achieved with these fibers that cover most of the communication wavelength bands. The proposed design study will be applicable for applications in the field of tomography, Dense Wavelength Division Multiplexing (DWDM) system, spectroscopy, etc. 相似文献
24.
We theoretically investigate the high-order harmonic generation in helium atom driven by a nonlinear chirped laser pulse with few-cycle duration. By employing appropriate chirp to the driving pulse, an efficient electric field waveform of controlling quantum path for ultra-broadband supercontinuous harmonics is realized, and then an isolated sub-50 as pulse with bandwidth of 739 eV can be significantly obtained. 相似文献
25.
Spectral broadening of spectrum-sliced amplified spontaneous emission (SS-ASE) in highly nonlinear, dispersion-shifted fiber in different dispersion regimes is investigated experimentally. We find that, the spectral noise of the amplified SS-ASE pump from Er3+-doped fiber amplifier seeds the spectral broadening via four-wave mixing or modulation instability. Stimulated Raman scattering, red-shifted Raman solitons, and blue-shifted dispersion waves all enhance the broadening of the spectrum. The effect of the polarization state of pump on supercontinuum generation is also investigated, and it is found that, linear polarization is more efficient than random polarization for pumping supercontinuum. Supercontinuum with −10 dB bandwidth of 200 nm is generated by launching linearly polarized pump with 33.5 dB m power into anomalous dispersion regime near to zero dispersion wavelength of fiber. 相似文献
26.
Zhuan Wang Ching-yue Wang Yingkui Han Shiying Cao Zhigang Zhang Lu Chai 《Optics & Laser Technology》2006,38(8):641-644
A Ti:sapphire oscillator emitting an octave-spanning spectrum that ranges from 460 to 1000 nm is demonstrated. To our knowledge, it is the first time that a supercontinuum as a whole measured after the output coupler extending beyond 500 nm in the blue end is generated from a femtosecond Ti:sapphire oscillator. In the Ti:sapphire oscillator operating in self-Q-switched and self-mode locked mode, two chirped mirrors and a prism pair were used for dispersion compensation. These experimental results would open a new option for the construction of simple continuum sources. 相似文献
27.
Darren D. Hudson Eric C. Mägi Alexander C. JudgeStephen A. Dekker Benjamin J. Eggleton 《Optics Communications》2012,285(23):4660-4669
In this review we consider the basic elements of tapering chalcogenide optical fibers for the generation of extreme spectral broadening through supercontinuum generation. Creating tapered nanofiber devices in chalcogenide fiber, which has an intrinsic nonlinearity that is two orders of magnitude higher than silica, has resulted in the demonstration of octave-spanning spectra using record low power. We first present a brief theoretical understanding of the tapering process that follows from the basic principle of mass conservation, and a geometric construction tool for the visualization of the shape of tapered fibers. This is followed by a theoretical treatment of dispersion engineering and supercontinuum generation in a chalcogenide nanofiber. In the final section, we cover the experimental implementation of the chalcogenide nanofiber and demonstrate an octave-spanning spectrum created with 150 W of peak power. 相似文献
28.
29.
All normal dispersion (ANDi) and highly nonlinear chalcogenide glass photonic crystal fiber (PCF) is proposed and numerically investigated for a broad, coherent and ultra-flat mid-infrared supercontinuum generation. The proposed PCF consists of a solid core made of Ga8Sb32S60 glass surrounded by seven rings of air holes arranged in a triangular lattice. We show by employing the finite difference frequency domain (FDFD) method that the Ga8Sb32S60 PCF dispersion properties can be engineered by carefully adjusting the air holes diameter in the cladding region and ANDi regime is achieved over the entire range of wavelengths with a zero chromatic dispersion around 4.5?μm. Moreover, we demonstrate that injecting 50?fs width and 20?kW peak power laser pulses (corresponding to a pulse energy of 1.06?nJ) at a pump wavelength of 4.5?μm into a 1?cm long ANDi Ga8Sb32S60 PCF generates a broad, flat-top and perfectly coherent SC spectrum extending from 1.65?μm to 9.24?μm at the 20?dB spectral flatness. These results make the proposed Ga8Sb32S60 PCF an excellent candidate for various important mid-infrared region applications including mid-infrared spectroscopy, medical imaging, optical coherence tomography and materials characterization. 相似文献
30.
HUANG Yi;WU Kan;XIAO Zeyu;LI Tieying;CAI Minglu;CHEN Jianping 《光子学报》2023,52(5):284-291
Optical frequency comb is a kind of multi-wavelength laser source with uniform and coherent frequency lines. Recently, the application of optical frequency comb in different fields has been expanding, such as spectroscopy, atomic clock, optical communication and microwave photonics. In the past decades, there are three main methods to generate optical frequency comb: firstly, optical frequency comb is generated by model locked lasers with a fixed repetition frequency. However, this method is limited by the model locked lasers, and it has small adjustable range and inflexibility. Secondly, optical frequency comb is generated on micro ring or cavity with great Kerr nonlinearity on chip, and the micro ring and cavity are easily affected by temperature in this method. Third, optical frequency comb is generated by electro-optic modulation using electro-optic effect. This method is generally used to generate optical frequency comb outside the chip due to the limitation of electro-optic modulator. Supercontinuum traditionally is generated by inputting MHz femtosecond pulse into a highly nonlinear waveguide to broaden its spectrum. Recently, lithium niobate materials stand out among many materials because of its strong linear electro-optic effect and high modulation bandwidth. With the integrated lithium niobate modulator, ultra-low optical loss, high modulation bandwidth and low RF drive voltage can be achieved simultaneously. Moreover, integrated lithium niobate has become an ideal platform in nonlinear optics because of its large second-order nonlinear index and high third-order nonlinearity. In this paper, we use the push-pull Mach Zehnder modulation and a cascade phase modulator integrated on the lithium niobate platform to generate optical frequency comb, and then let the signal go through a dispersion compensation module to compress the time domain waveform into a femtosecond pulse. At last, the signal is input into the lithium niobite waveguide which has great second-order nonlinear and third-order nonlinear to generate the second harmonic in the waveguide. Then the second harmonic interferes with the fundamental wave to generate a supercontinuum spectrum. In this paper, our mathematical model includes both second-order and third-order nonlinear, and the process of generating the second harmonic and supercontinuum spectrum is simulated in numerical simulation. Firstly, we use the cascade lithium niobite to generate a pulse with 180 fs pulse width and 126.4 pJ energy. Then this femtosecond pulse is input into the lithium niobite waveguide to generate the supercontinuum spectrum by the nonlinear effect of lithium niobite. We analyze the spectrum evolution under different energy of input pulse. In the simulation, we discuss the appearance of dispersion wave in the process of supercontinuum. Then we make a simulation on smaller modulation depth in order to get a wider pulse signal, and observe the effect of different input energies on supercontinuum broadening under this modulation depth. Comparing the energy required for the supercontinuum broadening of the optical spectrum with the modulation depth of 21π and 28π, it can be found that the wider the pulse width is, the narrower the 10 dB bandwidth of the spectrum is, the higher the energy required to generate the supercontinuum spectrum is. Moreover, when the modulation depth is 21π, the spectral width is about 75% of the modulation depth of 28π, and the pulse width is about 1.25 times of the modulation depth of 28π. However, after passing through the same section of waveguide, the supercontinuum spectrum also needs about 3 times of the energy when the modulation depth is 28π. Therefore, we believe that the pulse width, namely the width of the spectrum, has a greater impact on the supercontinuum broadening of the signal spectrum than the energy of the input pulse. This work lists the pulse width, spectrum width and input energy of input pulse when the supercontinuum spectrum is generated in different modulation depths. At last, we also observe the relationship between the pulse width and input energy in a figure, and conclude that the input energy will increase approximately square with the decreasing of pulse width. 相似文献