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1.
Experiments of the temperature effect on single bubble sonoluminescence (SBSL) are performed with a mixture of water and anti-freeze.Since experiments of constant pressure (keeping sound pressure constant) are not feasible for a wide temperature range,experiments of constant luminance (keeping light intensity stable),which reflect pure sensitivity of SBSL to temperature,are investigated.The results show that lower temperature needs less pressure to obtain the same light intensity,which means that lower temperature is better for SBSL.Numerical calculations show a qualitative agreement with experiments.  相似文献   

2.
路涛  安宇 《中国物理快报》2006,23(4):1019-1022
Considering the vapour effects, we calculate the shape instability of single-bubble sonoluminescence (SBSL) in the phase diagram of the amplitude of driving pressure versus ambient radius, i.e. the pa - R0 diagram. The numerical calculation shows that the results calculated by the present model are reliable, even some parameters, such as the binary diffusion constant and the thermal conductivity of the mixture of argon and water vapour inside the bubble, are roughly evaluated. It is found by numerical calculation that the shape stable area of a single argon bubble in those viscous liquids with low vapour pressure, such as oil of vitriol, glycerol and 1,2- propanediol, can be extended to a wider region. Combining with the calculation of the maximum temperature inside the bubble, we may predict that these areas are probably the stable region of SBSL.  相似文献   

3.
钱祖文 《中国物理》2001,10(7):636-638
The transient resonance of a sonoluminescence bubble has been analysed. When the bubble performs its transient resonance at the nth order harmonics of the standing waves in the liquid, the light intensity strongly depends on the amplitude of the driving pressure (proportional to its 2n power, with n=fr/f, where fr is Minnaert's linear resonant frequency of the bubble and f is the frequency of driving sound). The kinetic energy of a vibrating bubble becomes maximum approximately when it is in its equilibrium size. For example, when the ambient temperature of a bubble decreases from 34℃ to 4℃, a huge increase of the light intensity emitted by it can be explained. A suggestion was made that, within the limits permitted by the phase diagrams, as high an increase in driving pressure as possible could enhance the light intensity of sonoluminescence up to four orders of magnitude.  相似文献   

4.
陈岐岱  王龙 《中国物理快报》2004,21(9):1822-1824
Single transient cavitation bubble with luminescence has been generated in pure glycerin by using the ‘tube arrest‘ method. The analyses of high-speed photograph and light emission data suggest that the light emission would be a single bubble sonoluminescence. The luminescence pulse width is observed to vary from sub-nanosecond to about 30 ns. The width and intensity of luminescence pulses increases with the height of the liquid column height and decreases with the liquid temperature.  相似文献   

5.
The Raman–Nath diffraction in acousto–optic effect was studied theoretically and experimentally in the paper.Up to now,each order of diffracted light in Raman–Nath diffraction was still considered simply to be just frequency-shifted and to be a plane wave.However,we find that the phase and frequency shifts occur simultaneously and individually in Raman–Nath diffraction.The findings demonstrate that,in addition to the frequency shift,the optical phase of each order of diffracted light is also shifted by the sound wave and fluctuates with the sound wave and is related to the location in the acoustic field from which the diffracted light originates.As a result,the wavefront of each order of diffracted light is modulated to fluctuate spatially and temporally with the sound wave.Obviously,these findings are significant for applications of Raman–Nath diffraction in acousto–optic effect because the optical phase plays an important role in optical coherence technology.  相似文献   

6.
罗牧华  张秋菊 《中国物理 B》2011,20(8):85201-085201
The influence of time-dependent polarization on attosecond pulse generation from an overdense plasma surface driven by laser pulse is discussed analytically and numerically.The results show that the frequency of controlling pulse controls the number and interval of the generated attosecond pulse,that the generation moment of the attosecond pulse is dominated by the phase difference between the controlling and driving pulses,and that the amplitude of the controlling pulse affects the intensity of the attosecond pulse.Using the method of time-dependent polarization,a "single" ultra-strong attosecond pulse with duration τ≈ 8.6 as and intensity I ≈ 3.08 × 10 20 W·cm-2 can be generated.  相似文献   

7.
The effect of the absolute phase of the few-cycle driving laser field on the generation and measurement of highorder harmonic attosecond pulses is investigated theoretically.We find that the generated attosecond soft-x-ray pulse is locked to the oscillations of the driving laser field,but not to the envelope of the laser pulse,and the intensity ratio of two adjacent attosenond pulses is exponential as a function of the absolute phase.Based on these results,we propose a novel method to detect the absolute phase of the driving laser field by measuring the spatial distribution of the photoelectrons induced by the attosecond soft-x-ray pulse and the driving laser field.  相似文献   

8.
A truncated broadband parametric array with a primary frequency of 500 kHz and difference frequency range of 1 kHz to 30 kHz was designed as a sound source of the underwater acoustic material measurement system.By analyzing the theoretical calculation and actual measurement results in array directivity of the truncated broadband parametric source at typical frequencies,we observed that the curves of the two results were basically consistent,which proved that the calculation model was correct.Application of bell-shaped short-duration pulse to achieve broadband measurement for characteristics of underwater acoustic materials was beneficial to reduce the effects of diffraction from the panel edges.The measurement system was established for measuring the sound pressure reflection coefficients,sound pressure transmission coefficients and absorption coefficients of the large panel sample in the pressure vessel.The size of this tank is φ4 m×12 m,the maximum hydrostatic pressure is 4.5 MPa,and the corresponding measuring frequency range is from 1 kHz to 30 kHz.The measured curves had a good agreement with theoretical curves,which verified that the parametric source measurement method was feasible.Then,the sound absorption properties of the rubber plate sample were measured under different hydrostatic pressures.The studying results could show that the parametric source measurement method had the potential application in the limited space water,such as the pressure vessel.  相似文献   

9.
葛愉成 《中国物理快报》2008,25(4):1305-1308
Quantitative investigations are made for the laser-duration dependence of the emission properties of high-order harmonic generation (HHG). HHG emission properties produced by few-cycle lasers show some useful characteristics. The cutoff energy is less than that by laser for infinite duration. The single energy distribution pulse decreases much faster than its duration as the laser duration grows. A two-cycle laser with carrier-envelope phase of 0° can produce a single distribution pulse peaked at the laser carrier phase 1.22 rad and spanned 1.18 rad with the cutoff energy 2.9Up + Ip and a bandwidth 0.63Up, where Up is the ponderomotive potential of the laser field and Ip is the atomic ionization potential.  相似文献   

10.
李敏  米贤武 《中国物理 B》2009,18(12):5534-5538
This paper studies both the intraband polarization and terahertz emission of a semiconductor superlattice in combined dc and ac electric fields by using the superposition of two identical time delayed and phase shifted optical pulses. By adjusting the delay between these two optical pulses, our results show that the intraband polarization is sensitive to the time delay. The peak values appear again for the terahertz emission intensity due to the superposition of two optical pulses. The emission lines of terahertz blueshift and redshift in different ac electric fields and dynamic localization appears. The emission lines of THz only appear to blueshift when the biased superlattice is driven by a single optical pulse. Due to excitonic dynamic localization, the terahertz emission intensity decays with time in different dc and ac electric fields. These are features of this superlattice which distinguish it from a superlattice generated by a single optical pulse to drive it.  相似文献   

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