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1.
Recent developments in semiconductor disk lasers (SDLs) generating visible or ultraviolet light are reviewed. After an introduction on potential applications, we discuss how the combination of vertical‐emitting semiconductor GaAs‐based structures and intra‐cavity nonlinear conversion techniques can be successfully exploited to uniquely meet demands for continuous‐wave radiation in the visible and ultraviolet spectral range. To do so, an overview of the device operating principles and performance is presented highlighting the underlying material considerations, semiconductor structural designs, thermal management techniques and suitable cavity configurations. This summary is completed by a presentation of new developments in the field, with a particular focus on the trends towards miniaturization.  相似文献   

2.
We present experimental results on the interaction of pulsed laser radiation with ZnS-quantum-dot aqueous suspensions. We detect luminescence in the blue spectral range as well as narrow beams of X-ray radiation. We describe the experimental conditions of X-ray generation and discuss the triboluminescence as a possible mechanism of the emission.  相似文献   

3.
The paper concerns processing of optical images by means of tunable acousto-optic filters. Experimental and theoretical research showed that longitudinal chromatic aberrations cause a suffcient decay of the spatial resolution in the devices. It is shown that a proper choice of an optical cheme of an imager reduces the longitudinal aberrations all over the tuning range of the filters.  相似文献   

4.
The coupling of visible nanosecond laser pulses to metallic targets irradiated in vacuum is studied. The expressions of the vapour and plasma ignition times are obtained. Two cases for vapour breakdown in the plasma ignition process are considered. The first case is that 40 generations of new electrons are born in vapour generation time before plasma formation as assumed in the literature. The second case is that 10 generations of new electrons are born in vapour generation time. Molybdenum (Mo), niobium (Nb) and aluminium (Al) targets are considered for illustrations of our results. The expression of the plasma ignition time for the Al target is substantially different from that reported in the literature. The vapour and plasma ignition threshold laser intensities are calculated and compared with those reported in the literature. Reasons for disagreement are discussed. The plasma ignition threshold estimated in the second case is noted to be in good agreement with the reported experimental result.  相似文献   

5.
We present the first (to our best knowledge) femtosecond enhancement cavity in the visible wavelength range for ultraviolet frequency comb generation. The cavity is seeded at 518 nm by a frequency-doubled Yb fiber laser and operates at a peak intensity of 1.2×10(13) W/cm(2). High harmonics of up to the ninth order (~57 nm) are generated in an intracavity xenon gas jet. Intracavity high harmonic powers of several milliwatts for the third harmonic order and microwatts for the fifth harmonic order prove the potential of the "green cavity" as an efficient ultraviolet frequency comb source for future spectroscopic experiments. A limiting degradation effect of the cavity mirrors is avoided by operating at a constant oxygen background pressure.  相似文献   

6.
刘钧  杨书宁  高明 《应用光学》2014,35(2):215-220
设计了一种用来校准紫外与可见光光轴平行性的可调焦光学系统,调焦范围为70 m~。针对目前大多数校准系统无法进行调焦的问题,提出一种既能校准紫外与可见光光轴平行性又能对紫外部分进行调焦的方法。采用离轴卡塞格林系统作为初始结构进行设计,通过在传统的卡塞格林系统中加入调焦组和补偿组来实现调焦以及像差补偿,所设计的系统可以有效地解决紫外与可见光双光轴平行性失调的校准问题,提高紫外与可见光双光轴平行性校准效率,并且在不同视距下光学传递函数值及点列斑均接近衍射极限,能量集中度达到90%,整个视场的像质均匀,像面清晰,有利于后续的图像处理工作。  相似文献   

7.
Surface-relief gratings were directly fabricated onto a glass surface by UV-visible laser irradiation. The glass surface was pretreated by molten salt, including Ag ions. Periodic intensity modulation of the laser light was conducted with a phase mask or by an interference technique. A pattern generated by intensity modulation was precisely transcribed onto the glass surface and a surface-relief grating was formed. The period and depth of the grating were 0.5 to 10 microm and less than 0.8 microm, respectively. The cross-sectional profile of the grating was sinusoidal or triangular, with very smooth surface morphology.  相似文献   

8.
The ultraviolet upconversion luminescence of Tm3+ ions sensitized by Yb3+ ions in oxyfluoride glass when excited by a 975 nm diode laser was studied in this paper. One typical ultraviolet upconversion luminescence lines positioned at 362.3 nm was found. It can be attributed to the five-photon upconversion luminescence transition of 1D2 → 3H6. Several visible upconversion luminescence lines at 451.1 nm, (477.9 nm, 462.5 nm), 648.7 nm, (680.5 nm, 699.5 nm) and (777.5 nm, 800.7 nm) were found also, which results from the fluorescence transitions of five-photon 1D2 → 3F4, three-photon 1G4 → 3H6, three-photon 1G4 → 3F4, two-photon 3F3 → 3H6 and two-photon 3H4 → 3H6 of Tm3+ ion, respectively. The theoretical analysis suggests that the upconversion mechanism of the 362.3 nm 1D2 → 3H6 upconversion luminescence is the cross energy transfer of {3H4(Tm3+) → 3F4(Tm3+), 1G4(Tm3+) → 1D2(Tm3+)} and {1G4(Tm3+) → 3F4(Tm3+), 3H4(Tm3+) → 1D2(Tm3+)} between Tm3+ ions. In addition, the upconversion luminescence of 1G4 and 3H4 state results from the sequential energy transfer {2F5/2(Yb3+) → 2F7/2(Yb3+), 3H4(Tm3+) → 1G4(Tm3+)} and {2F5/2(Yb3+) → 2F7/2(Yb3+), 3F4(Tm3+) → 3F2(Tm3+)} from Yb3+ ions to Tm3+ions, respectively.  相似文献   

9.
A Langmuir probe was used as a diagnostic of the temporally evolving electron number densities within a low-temperature laser-ablated titanium plasma expanding in vacuum. Measurements were made following ablation by a KrF excimer laser (248 nm, F=30 ns) and a frequency-doubled Nd:YAG laser (532 nm, F=7.5 ns) for laser power densities between 85 MW cm-2 and 1130 MW cm-2 on target. Electron number density data were obtained from the saturation electron current region of the probe (I/V) characteristic. Peak electron number densities in the range 1.5᎒10 cm-3 to 1.5᎒13 cm-3 were measured, at a distance of 5 cm along the target normal, for the laser power range investigated. Above ablation threshold the temporally integrated electron flux increased linearly with incident power density for both ablation wavelengths. The ablation thresholds, in terms of peak power density within the laser spot on the target, were found to be 85ᆨ MW cm-2 for KrF ablation and 300ᇆ MW cm-2for 2P YAG ablation.  相似文献   

10.
11.
提出并建立了表面单分子膜在垂悬液滴面上的Raman图像取向的确定方法。对具有单以向性的分子,推导出全部Ranam散射活性矩阵元,计算并给制了Raman图像的光强分布以及确定分子取向的偏振光强比分布。  相似文献   

12.
We demonstrate a novel spectral-shearing interferometry setup for characterizing the temporal amplitude and phase of ultrashort optical pulses over an extremely wide wavelength region. By the mixing of two strongly chirped auxiliary pulses with the pulse to be characterized, two spectrally sheared replicas are generated, and their spectral interference is evaluated. We fully characterize 10-fs pulses in the visible region by sum-frequency mixing and 19-fs pulses in the ultraviolet region by difference-frequency mixing. The scheme is self-referencing and highly sensitive. The zero-additional-phase scheme does not alter the unknown pulses and yields the pulse shape at the interaction point of a spectroscopic experiment.  相似文献   

13.
The efficiencies of direct lidars operating at 355, 532, 1064 and 1540-nm radiation wavelengths for early forest fire detection were compared. For each wavelength, the range for reliable smoke-plume detection was estimated on the basis of a computer simulation plume using a one-dimensional “top-hat” gas dynamic model for the calculation of the backscattering and extinction-coefficient profiles within the plume. The agreement between the predicted signal-to-noise ratio (SNR) and experimental results for 532 and 1064-nm wavelength radiation is good. The decrease of the signal-to-noise ratio with distance is maximum for 355 nm and minimum for 1064 nm. At 1540 nm, the decay of SNR with distance is slightly faster, but the SNR is higher than for other wavelengths, leading to the highest detection efficiency for the same energy of the probing laser pulse. For a burning rate of 2 kg/s and a laser beam divergence of 2.5 mr, the maximum distance for reliable detection varies between 6 and 12 km, depending on the wavelength. Received: 15 May 2002 / Revised version: 13 September 2002 / Published online: 22 January 2003 RID="*" ID="*"Corresponding author. Fax: +351-21/841-8120, E-mail: rui.vilar@ist.utl.pt  相似文献   

14.
Broadband tunability in the yellow-red region is obtained by use of intracavity type II second-harmonic generation of gain-switched Cr:forsterite lasers in KTiOPO(4) . An operating wavelength range of 67 nm, from 587 to 654 nm, is obtained. Second-harmonic energy of almost 1 mJ is achieved at a peak wavelength of 620 nm. A measured factor-of-34 enhancement in acceptance angle is obtained with broadband harmonic generation. Frequency doubling is optimized with respect to the Cr:forsterite pump and laser parameters.  相似文献   

15.
This paper reports the micromachining of fused quartz and Pyrex glass by laser-induced plasma-assisted ablation (LIPAA) using a conventional nanosecond laser at wavelengths 266 nm, 532 nm, and 1064 nm, respectively. High-quality surface structuring can be achieved at each of these wavelengths. The micrograting formed has periods of 14 7m at 266 nm, 20 7m at 532 nm, and 30 7m at 1064 nm, respectively. The ablation rate using a 266 nm laser is much larger than that at longer wavelengths. The ablation thresholds of laser fluence are 0.7 J/cm2 for 266 nm, 1.5 J/cm2 for 532 nm and 3.7 J/cm2 for 1064 nm, respectively. The 532 nm and 1064 nm lasers enable hole drilling in 0.5 and 2.0-mm thick fused quartz and Pyrex glass substrates of about 0.7-0.8 mm in diameter. However, the less destructive through channel can be only formed in Pyrex glass by using a 532 nm laser.  相似文献   

16.
17.
Single-crystal specular reflectance spectra of three polarizations of (TMTSF)2ClO4 in the visible and ultraviolet regions and their Kramers-Kronig-transformed absorption spectra are reported. Earlier reports of visible transitions are confirmed with the addition of integrated intensities, and several new transitions are reported quantitatively in the ultraviolet.  相似文献   

18.
The influence of different evaporation process parameters on the optical properties and constants of thin Sb2O3 films in the ultraviolet and visible region from 250 to 800 nm has been investigated. The most dominant parameters, namely the substrate temperature, rate of evaporation, and ambient oxygen pressure used during the deposition process and the post-annealing temperatures were optimised which resulted in low loss, dense and homogeneous Sb2O3 films. The optical constants and band gaps of these films were evaluated using their interference modulated transmittance spectra in case of both homogeneous and inhomogeneous conditions. Optimized films have been successfully used in developing multilayer high reflecting coatings for Fabry-Perot etalons along with the cryolite (Na3AlF6) films.  相似文献   

19.
Evidences of ultraviolet visible spectra of hydrogen sulfide scavenging trans-crotonaldehyde (TCA) induced by hydrogen peroxide through mitochondria were probed for the first time. TCA was induced by hydrogen peroxide through mitochondria. When sodium hydrosulfide as hydrogen sulfide donor, comparison with control, ultraviolet visible spectra of TCA decrease were clear. Hydrogen sulfide released by garlic was detected by ultraviolet visible spectroscopy. When garlic as hydrogen sulfide donors, the ultraviolet visible spectra of TCA decrease were very obvious. The findings are strongly recommended that garlic as safe, stable, and controllable hydrogen sulfide donor become a promising drug which is worthy of further study.  相似文献   

20.
Ma CY  Xu JY  Liu XJ 《Ultrasonics》2006,44(Z1):e375-e378
The degradation of Acid Orange 7 in aqueous solution has been investigated under the irradiation of ultrasound and visible light respectively and simultaneously. We have observed that the maximum removal percentage K increases from 4% to 35% when the ultrasonic frequency f and power P change from f=20 KHz and P=3 W to f=1 MHz and P=40 W. On the other hand, the K-value is approximately 3% under the irradiation of visible light at 632 nm and 100 mW/mm(2). Under the simultaneous irradiation of ultrasound (1 MHz, 40 W) and visible light (632 nm, 100 mW/mm(2)), the K-value reaches to approximately 65%, indicating a synergistic effect of ultrasound and visible light irradiations. A simple model based on the band gap theory and cavitation theory is proposed to explain the synergistic phenomenon.  相似文献   

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