Defining the unknowns of sonoluminescence

被引:453
作者
Barber, BP
Hiller, RA
Lofstedt, R
Putterman, SJ
Weninger, KR
机构
[1] UNIV CALIF LOS ANGELES, DEPT PHYS, LOS ANGELES, CA 90095 USA
[2] UNIV CALIF SANTA BARBARA, INST THEORET PHYS, SANTA BARBARA, CA 93106 USA
来源
PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS | 1997年 / 281卷 / 02期
基金
美国国家科学基金会;
关键词
sonoluminescence; bubble dynamics; Bremsstrahlung;
D O I
10.1016/S0370-1573(96)00050-6
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
As the intensity of a standing sound wave is increased the pulsations of a bubble of gas trapped at a velocity node attain sufficient amplitude so as to emit picosecond hashes of light with a broadband spectrum that increases into the ultraviolet. The acoustic resonator can be tuned so that the flashes of light occur with a clocklike regularity: one flash for each cycle of sound with a jitter in the time between flashes that is also measured in picoseconds. This phenomenon (sonoluminescence or ''SL'') is remarkable because it is the only means of generating picosecond flashes of light that does not use a laser and the input acoustic energy density must be concentrated by twelve orders of magnitude in order to produce light. Light scattering measurements indicate that the bubble wall is collapsing at more than 4 times the ambient speed of sound in the gas just prior to the light emitting moment when the gas has been compressed to a density determined by its van der Waals, hard core. Experiments indicate that the collapse is remarkably spherical, water is the best fluid for SL, some noble gas is essential for stable SL, and that the light intensity increases as the ambient temperature is lowered. In the extremely stable experimental configuration consisting of an air bubble in water, measurements indicate that the bubble chooses an ambient radius that is not explained by mass diffusion. Experiments have not yet been able to map out the complete spectrum because above 6 eV it is obscured by the cutoff imposed by water, and furthermore experiments have only determined an upper bound on the hash widths. In addition to the above puzzles, the theory for the light emitting mechanism is still open. The scenario of a supersonic bubble collapse launching an imploding shock wave which ionizes the bubble contents so as to cause it to emit Bremsstrahlung radiation is the best candidate theory but it has not been shown how to extract from it the richness of this phenomenon. Most exciting is the issue of whether SL is a classical effect or whether Planck's constant should be invoked to explain how energy which enters a medium at the macroscopic scale holds together and focuses so as to be emitted at the microscopic scale.
引用
收藏
页码:65 / 143
页数:79
相关论文
共 128 条
[1]  
[Anonymous], ECHOCARDIOGRAPHY
[3]   SHAPE OSCILLATIONS OF BUBBLES IN WATER DRIVEN BY MODULATED ULTRASONIC RADIATION PRESSURE - OBSERVATIONS AND DETECTION WITH SCATTERED LASER-LIGHT [J].
ASAKI, TJ ;
MARSTON, PL ;
TRINH, EH .
JOURNAL OF THE ACOUSTICAL SOCIETY OF AMERICA, 1993, 93 (02) :706-713
[4]  
Barber B., 1991, J ACOUST SOC AM, V89, P1885
[5]   RESOLVING THE PICOSECOND CHARACTERISTICS OF SYNCHRONOUS SONOLUMINESCENCE [J].
BARBER, BP ;
HILLER, R ;
ARISAKA, K ;
FETTERMAN, H ;
PUTTERMAN, S .
JOURNAL OF THE ACOUSTICAL SOCIETY OF AMERICA, 1992, 91 (05) :3061-3063
[6]   OBSERVATION OF SYNCHRONOUS PICOSECOND SONOLUMINESCENCE [J].
BARBER, BP ;
PUTTERMAN, SJ .
NATURE, 1991, 352 (6333) :318-320
[7]   OBSERVATION OF A NEW PHASE OF SONOLUMINESCENCE AT LOW PARTIAL PRESSURES [J].
BARBER, BP ;
WENINGER, K ;
LOFSTEDT, R ;
PUTTERMAN, S .
PHYSICAL REVIEW LETTERS, 1995, 74 (26) :5276-5279
[8]   SENSITIVITY OF SONOLUMINESCENCE TO EXPERIMENTAL PARAMETERS [J].
BARBER, BP ;
WU, CC ;
LOFSTEDT, R ;
ROBERTS, PH ;
PUTTERMAN, SJ .
PHYSICAL REVIEW LETTERS, 1994, 72 (09) :1380-1383
[9]   LIGHT-SCATTERING MEASUREMENTS OF THE REPETITIVE SUPERSONIC IMPLOSION OF A SONOLUMINESCING BUBBLE [J].
BARBER, BP ;
PUTTERMAN, SJ .
PHYSICAL REVIEW LETTERS, 1992, 69 (26) :3839-3842
[10]  
BARBER BP, 1997, IN PRESS T ROY SOC