The Key Laboratory of Biomedical Information Engineering of Ministry of Education, Department of Biomedical Engineering, School of Life Science and Technology, Xi'an Jiaotong University, Xi'an 710049, PR China.
Ultrason Sonochem. 2012 Mar;19(2):257-63. doi: 10.1016/j.ultsonch.2011.07.007. Epub 2011 Jul 26.
An intensified charge coupled device (ICCD) camera was used to observe the spatial distribution of sonoluminescence (SL) and sonochemiluminescence (SCL) generated by cavitation bubbles in a 1.2 MHz focused ultrasound (FU) field in order to investigate the mechanisms of acoustic cavitation under different sonication conditions for FU therapeutic applications. It was found that SL emissions were located in the post-focal region. When the intensity of SL and SCL increased as the power rose, the growth of SCL was much higher than that of SL. In the post-focal region, the SCL emissions moved along specific paths and formed branch-like streamers. At the beginning of the ultrasound irradiation, cavitation bubbles generated SCL in both the pre-focal and the post-focal region. When the electrical power or the sonication time increased, the SCL in the post-focal region increased and became higher than that in the pre-focal region. The intensity of SCL in the focal region is usually the weakest because of "oversaturation". The spatial distribution of SCL near a tissue boundary differed from that obtained in free fields. It organized into special structures under different acoustic amplitudes. When the electrical power was relatively low, the SCL emission was conical shape which suggested a standing wave formation at the tissue-fluid boundary. When the electrical power exceeded a certain threshold, only a bright spot could be captured in the focus. The cavitation bubbles which centralized in the focus concentrated energy and hindered the formation of standing waves. With rising electrical power at high levels, besides a bright spot in the focus, there were some irregular light spots in pre-focal region, which indicated some cavitation bubbles or small bubble clusters achieved the threshold of SCL and induced the reaction with the luminol solution.
采用增强型电荷耦合器件(ICCD)相机观察了在 1.2MHz 聚焦超声(FU)场中声空化气泡产生的声致发光(SL)和化学发光(SCL)的空间分布,以研究不同超声条件下声空化的机制,为 FU 治疗应用提供依据。结果发现,SL 发射位于焦后区。当强度随着功率的增加而增加时,SCL 的增长远高于 SL。在焦后区,SCL 发射沿着特定的路径移动,并形成分支状的流光。在超声辐射开始时,空化气泡在焦前区和焦后区都产生了 SCL。当电功率或超声时间增加时,焦后区的 SCL 增加,并且高于焦前区的 SCL。由于“过饱和”,焦区的 SCL 强度通常最弱。在组织边界附近,SCL 的空间分布与自由场中获得的分布不同。在不同的声幅下,它组织成特殊的结构。当电功率较低时,SCL 发射呈圆锥形,表明在组织-流体边界处形成驻波。当电功率超过一定阈值时,只能在焦点捕获一个亮点。集中在焦点的空化气泡集中能量并阻碍驻波的形成。随着电功率的升高,除了焦点处的亮点外,焦前区还有一些不规则的亮点,这表明一些空化气泡或小气泡簇达到了 SCL 的阈值,并引发了与鲁米诺溶液的反应。