{"title":"选择低频率的径向调制成像在20mhz","authors":"F. Yu, F. Villanueva, Xucai Chen","doi":"10.1109/ULTSYM.2010.5935981","DOIUrl":null,"url":null,"abstract":"Background: Radial modulation (RM) is a promising dual band approach for high frequency microbubble (MB) imaging. A low frequency (LF) ultrasound pulse is used to manipulate the MB radius while a synchronized high frequency (HF) pulse successively measures MB backscatter in compressed and expanded states. RM signal amplitude has been shown to increase with LF signal amplitude, but is ultimately limited by the infiltration of LF harmonics into the HF bandwidth at higher LF pressure. The ideal LF for maximizing RM signal remains controversial, and frequencies at and below resonance have been reported. This study was designed to investigate the modulation frequency and amplitude that maximize RM signal. Methods: Lipid-encapsulated perfluorocarbon MB (3.54 ± 1.76 µm) were circulated in a 6 mm diameter cellulose tube. A 20 MHz single element transducer was concentrically housed in the center of hollow 1 and 2.25 MHz transducers and the resulting confocal pressure fields were calibrated with a hydrophone. During insonation of the circulating MB, 50 independent HF line pairs were recorded while varying LF pressure from 0.02 to 0.4 mechanical index (MI). The RM signal was defined as the mean HF backscatter power difference between the low and high pressure phases of the modulating LF, normalized by the high pressure HF backscatter power. Radio-frequency signal and spectra were also analyzed for LF harmonics. Results: Simulation and experimental data for this MB suspension both predicted higher RM at resonance frequency for the same MI. However, our experimental data demonstrate that the RM reaches a 60% maximum that is the same for both frequencies and is reached at 0.1 < MI < 0.15. This plateau just precedes the appearance of LF harmonics in the HF bandwidth when MI > 0.15. Also, we show that RM allows high resolution single MB specific imaging with very efficient tissue suppression. Conclusions: Our results suggest that a MI in the 0.1–0.15 range produced the same maximal RM amplitude in the studied MB population for both LF studied. LF harmonics were negligible at these pressure levels. These findings should help with the development of high frequency molecular imaging.","PeriodicalId":6437,"journal":{"name":"2010 IEEE International Ultrasonics Symposium","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2010-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"The selection of the low frequency for radial modulation imaging at 20 MHz\",\"authors\":\"F. Yu, F. Villanueva, Xucai Chen\",\"doi\":\"10.1109/ULTSYM.2010.5935981\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Background: Radial modulation (RM) is a promising dual band approach for high frequency microbubble (MB) imaging. A low frequency (LF) ultrasound pulse is used to manipulate the MB radius while a synchronized high frequency (HF) pulse successively measures MB backscatter in compressed and expanded states. RM signal amplitude has been shown to increase with LF signal amplitude, but is ultimately limited by the infiltration of LF harmonics into the HF bandwidth at higher LF pressure. The ideal LF for maximizing RM signal remains controversial, and frequencies at and below resonance have been reported. This study was designed to investigate the modulation frequency and amplitude that maximize RM signal. Methods: Lipid-encapsulated perfluorocarbon MB (3.54 ± 1.76 µm) were circulated in a 6 mm diameter cellulose tube. A 20 MHz single element transducer was concentrically housed in the center of hollow 1 and 2.25 MHz transducers and the resulting confocal pressure fields were calibrated with a hydrophone. During insonation of the circulating MB, 50 independent HF line pairs were recorded while varying LF pressure from 0.02 to 0.4 mechanical index (MI). The RM signal was defined as the mean HF backscatter power difference between the low and high pressure phases of the modulating LF, normalized by the high pressure HF backscatter power. Radio-frequency signal and spectra were also analyzed for LF harmonics. Results: Simulation and experimental data for this MB suspension both predicted higher RM at resonance frequency for the same MI. However, our experimental data demonstrate that the RM reaches a 60% maximum that is the same for both frequencies and is reached at 0.1 < MI < 0.15. This plateau just precedes the appearance of LF harmonics in the HF bandwidth when MI > 0.15. Also, we show that RM allows high resolution single MB specific imaging with very efficient tissue suppression. Conclusions: Our results suggest that a MI in the 0.1–0.15 range produced the same maximal RM amplitude in the studied MB population for both LF studied. LF harmonics were negligible at these pressure levels. 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引用次数: 2
摘要
背景:径向调制(RM)是一种很有前途的用于高频微泡成像的双波段方法。使用低频(LF)超声脉冲来控制MB半径,同时使用同步的高频(HF)脉冲依次测量压缩和扩展状态下的MB背散射。RM信号幅值随低频信号幅值的增加而增加,但最终受到低频谐波在高低频压力下渗入高频带宽的限制。最大化RM信号的理想LF仍然存在争议,共振和低于共振的频率已被报道。本研究旨在探讨调制频率和幅度,最大限度地提高了RM信号。方法:脂质包封的全氟碳MB(3.54±1.76µm)在直径6 mm的纤维素管中循环。将一个20 MHz的单元件换能器同心放置在空心1和2.25 MHz换能器的中心,用水听器校准所得的共聚焦压力场。在循环MB超声期间,记录了50对独立的HF线对,同时将LF压力从0.02到0.4机械指数(MI)变化。RM信号定义为调制LF的低压相位和高压相位之间的平均HF反向散射功率差,经高压HF反向散射功率归一化。对射频信号和频谱进行了低频谐波分析。结果:该MB悬架的模拟和实验数据都预测了相同MI的共振频率下更高的RM。然而,我们的实验数据表明,两个频率下RM达到60%的最大值,并且在0.1 < MI < 0.15时达到。当MI > 0.15时,该平台恰好先于高频带宽中低频谐波的出现。此外,我们表明RM允许高分辨率单个MB特异性成像,具有非常有效的组织抑制。结论:我们的研究结果表明,0.1-0.15范围内的MI在两种LF研究的MB人群中产生相同的最大RM振幅。在这些压力水平下,低频谐波可以忽略不计。这些发现将有助于高频分子成像技术的发展。
The selection of the low frequency for radial modulation imaging at 20 MHz
Background: Radial modulation (RM) is a promising dual band approach for high frequency microbubble (MB) imaging. A low frequency (LF) ultrasound pulse is used to manipulate the MB radius while a synchronized high frequency (HF) pulse successively measures MB backscatter in compressed and expanded states. RM signal amplitude has been shown to increase with LF signal amplitude, but is ultimately limited by the infiltration of LF harmonics into the HF bandwidth at higher LF pressure. The ideal LF for maximizing RM signal remains controversial, and frequencies at and below resonance have been reported. This study was designed to investigate the modulation frequency and amplitude that maximize RM signal. Methods: Lipid-encapsulated perfluorocarbon MB (3.54 ± 1.76 µm) were circulated in a 6 mm diameter cellulose tube. A 20 MHz single element transducer was concentrically housed in the center of hollow 1 and 2.25 MHz transducers and the resulting confocal pressure fields were calibrated with a hydrophone. During insonation of the circulating MB, 50 independent HF line pairs were recorded while varying LF pressure from 0.02 to 0.4 mechanical index (MI). The RM signal was defined as the mean HF backscatter power difference between the low and high pressure phases of the modulating LF, normalized by the high pressure HF backscatter power. Radio-frequency signal and spectra were also analyzed for LF harmonics. Results: Simulation and experimental data for this MB suspension both predicted higher RM at resonance frequency for the same MI. However, our experimental data demonstrate that the RM reaches a 60% maximum that is the same for both frequencies and is reached at 0.1 < MI < 0.15. This plateau just precedes the appearance of LF harmonics in the HF bandwidth when MI > 0.15. Also, we show that RM allows high resolution single MB specific imaging with very efficient tissue suppression. Conclusions: Our results suggest that a MI in the 0.1–0.15 range produced the same maximal RM amplitude in the studied MB population for both LF studied. LF harmonics were negligible at these pressure levels. These findings should help with the development of high frequency molecular imaging.