共查询到20条相似文献,搜索用时 0 毫秒
1.
2.
Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to
generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 fs2 is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of
the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses
were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase
and cross-phase modulations, which occur simultaneously with four-wave mixing. 相似文献
3.
Generation of deep-ultraviolet femtosecond pulses by four-wave mixing through filamentation in neon gas was demonstrated. Fundamental (omega) and second-harmonic (2omega) pulses of 25 fs Ti:sapphire amplifier output were focused into neon gas, and 20 microJ pulses with the center wavelength of 260 nm were produced by a four-wave mixing process, 2omega+2omega-omega?3omega through an ~15 cm filament. Additionally, pulses with an energy of 2 microJ at 200 nm were generated, probably by a cascaded process, 3omega+2omega-omega?4omega. The 260 nm pulses were compressed by a grating-based compressor and characterized by a dispersion-free transient grating frequency-resolved optical gating. The estimated pulse width was 12 fs. 相似文献
4.
5.
Konorov SO Serebryannikov EE Zheltikov AM Zhou P Tarasevitch AP von der Linde D 《Optics letters》2004,29(13):1545-1547
Phase-matched parametric four-wave mixing in higher-order guided modes of a photonic crystal fiber is shown to result in an efficient decay of 40-fs 800-nm Ti:sapphire laser pump pulses into an anti-Stokes signal with a central wavelength around 590-600 nm and a Stokes signal centered at 1.25 microm. The photonic crystal fiber is designed in such a way as to minimize the group-velocity dispersion at the pump wavelength, phase match the parametric four-wave-mixing process, and reduce the group delay between the pump and the anti-Stokes pulses. The duration of the anti-Stokes pulse under these conditions, as shown by cross-correlation frequency-resolved optical gating measurements, is less than 200 fs. 相似文献
6.
H. Zhang Z. Zhou A. Lin J. Cheng H. Liu J. Si F. Chen X. Hou 《Applied physics. B, Lasers and optics》2012,108(3):487-491
We investigated the generation of cascaded four-wave mixing (CFWM) sidebands by using two crossing chirped femtosecond pulses with the same central wavelength in tellurite glass (Te glass). Sidebands of broadband spectra, which contained non-degenerate and degenerate CFWM signals, were obtained at different delay time between two input pulses. The CFWM sidebands observed on different sides of input beams were flexibly controlled by adjusting the delay time. 相似文献
7.
Four-wave mixing in the vicinity of a sodium doublet is reported. The three-level system allows collinear phase-matching. The FWM is resonantly enhanced by a high gain on the blue side of the D1 transition.Present address: LROL, Physics Department, Laval University, Quebec, Canada, G1K 7P4To whom correspondence should be addressed 相似文献
8.
Broadband (sometimes exceeding 1500 cm-1) red-shifted (with respect to the sodium 3S–3P transition frequency) conical emission has been observed with the pump wavelength
tuned in the range between 540 and 589 nm. Such broadband emission was attributed to the generation and amplification of light
at the Rabi sideband frequencies in the field of intense femtosecond laser pulses. It has been shown that the cone angle of
the emitted radiation is determined by the process of four-wave mixing under the conditions of longitudinal (Cherenkov-type)
phase matching.
PACS 42.65.Ky; 42.65.Re; 42.50.Hz 相似文献
9.
We exploit nondegenerate four-wave mixing to generate narrow-bandwidth visible light from blue to orange in microstructured optical fiber. The process is excited by nanosecond dual-wavelength pump pulses (532/1064 nm) produced by a frequency-doubled passively Q-switched Nd:YAG laser. A linearly polarized, fundamental mode signal wave is generated in the visible, accompanied by an idler wave in the near-infrared. The signal and idler wavelengths are adjustable by the design of the microstructure. 相似文献
10.
Jinyu Sun 《Optics Communications》2011,284(19):4745-4748
Noncollinear optical parametric up-conversion generation and amplification are realized in a thick β-barium borate (BBO) crystal, and a couple of visible femtosecond up-conversion laser pulses can be achieved by a femtosecond pulse at 800 nm as the pump sources. The theoretical and experimental results indicate that there exist phase-matching conditions for dual-color noncollinear parametric up-conversion generation and amplification, and their wavelengths can be tuned by rotating the BBO crystal. This parametric up-conversion generation and amplification can be attributed to three and five-wave mixing in a thick BBO crystal, and it shows the potential application on optical parametric chirped pulse amplification (OPCPA) to generate multi-color ultraviolet or visible femtosecond laser pulses pumped directly by femtosecond fundamental laser pulses without frequency-doubling or tripling. 相似文献
11.
12.
Generation of sub-two-cycle, microjoule pulses in the mid-infrared region is demonstrated. Fundamental and second-harmonic pulses of 25 fs Ti:sapphire amplifier output were focused into the air to produce extremely broadband mid-infrared pulses by four-wave difference-frequency generation through the filamentation. The full width at half-maximum of the spectral bandwidth reaches one octave (2.5-5.5 microm), which is sufficiently broad for sub-single-cycle pulse generation. The pulse width was estimated to be 13 fs, without any compressors, by cross-correlation frequency resolved optical gating. The output energy of more than a few microjoule is sufficient for spectroscopy. 相似文献
13.
The boundary problem for signal phase conjugation at nondegenerated four-wave mixing (FWM) is considered. In contrast to the statements of some authors it is shown that noncollinearity of the incident and the phase-conjugate waves occur. Expressions have been obtained for the deflection angle for a number of configurations of practical importance. Useful analogy between linear and nonlinear reflection at the FWM is noted. 相似文献
14.
Submillimeter-scale dispersion micromanagement (DMM) is used to generate coherent and stable femtosecond visible pulses in holey fibers as short as 10 mm. The longitudinal variation of the phase-matching conditions for Cerenkov radiation and four-wave mixing explains the results well. We have converted up to 20% of the total input energy to a low-noise solitary wave with a bandwidth up to 50 nm in the range 385-625 nm by using holey fibers with various DMM designs. 相似文献
15.
Broadband nonlinear-dispersive similariton (50 THz bandwidth; > 100 nm at 800 nm central wavelength) is generated in passive uniform fiber and characterized experimentally through the chirp measurement technique of spectral compression and frequency tuning in the sum-frequency generation process. The potential of similariton applications to the signal synthesis and analysis problems on the femtosecond time scale, especially for similariton-induced temporal lensing and similariton-based spectral interferometry, is discussed on the basis of our experiments. 相似文献
16.
Generation of high-energy femtosecond pulses in multimode-core Yb-fiber chirped-pulse amplification systems 总被引:1,自引:0,他引:1
220-fs pulses with energies of ~100microJ have been generated by use of two different configurations of diode-pumped Yb-fiber chirped-pulse amplification systems. Energy scaling was demonstrated with 25-microm -core diameter fibers, in which stable diffraction-limited output (M(2)~1.1) was achieved. A two-stage fiber-amplifier system produced average powers of up to 5.5 W at ~1- MHz pulse-repetition rate. A double-pass configuration provided 53-dB gain in a single Yb-fiber amplifier stage, thus eliminating the necessity for multiple amplification stages as well as the need for using polarization-preserving fibers. 相似文献
17.
S. O. Konorov E. E. Serebryannikov A. A. Ivanov D. A. Akimov M. V. Alfimov A. M. Zheltikov 《JETP Letters》2004,79(9):395-398
Hollow-core photonic-crystal fibers with a special dispersion profile are shown to allow phase-matched nonlinear optical interactions of isolated air-guided modes of high-intensity femtosecond laser pulses confined in the hollow fiber core. We present theoretical and experimental studies of the four-wave mixing of fundamental and second-harmonic pulses of a Cr:forsterite laser with an initial pulse duration of about 50 fs and an intensity on the order of 1014 W/cm2 in waveguide modes of a hollow photonic-crystal fiber with a core diameter of about 13μm. 相似文献
18.
We propose a method for exciting a surface polariton wave by nonlinear mixing of three evanescent waves. The nonlinear polarization and phase matching conditions are analyzed for diatomic cubic crystals and a numerical example is given for GaP showing that this scheme is possible. Furthermore, by consideration of the energy balance in the crystal, the gain coefficient for the surface wave and the intensity of the wave coupled to the vacuum are also calculated. 相似文献
19.
Fourier-transform-limited extreme-ultraviolet (XUV) radiation (bandwidth approximately < 300 MHz) tunable around 91 nm is produced by use of two-photon resonance-enhanced four-wave mixing on the Kr resonance at 94 093 cm(-1). Noncollinear phase matching ensures the generation of an XUV sum frequency 2 omega1 + omega2 that can be filtered from auxiliary laser beams and harmonics by an adjustable slit. Application of the generated XUV light is demonstrated in spectroscopic investigations of highly excited states in H2 and N2. 相似文献
20.
I. Blonskyi V. Kadan I. Dmitruk P. Korenyuk 《Applied physics. B, Lasers and optics》2012,107(3):649-652
It is demonstrated experimentally that the angle vs. wavelength dependence of the emission generated by multi-step four-wave mixing process seeded by stimulated Raman scattering in water under femtosecond Bessel beam excitation is determined by the longitudinal phase-matching from IR to near UV. It is shown that if on-axis phase velocity of the pump Bessel beam is equal to the phase velocity of the Stokes axial wave, then, similar to Cherenkov radiation, all the other anti-Stokes beams too acquire that axial velocity. 相似文献