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Superharmonic imaging based on chirps

机译:基于线性调频的超谐波成像

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In medical ultrasound harmonic images of biological tissue are commonly obtained by analyzing the reflected echoes from the 2nd harmonic band. A new modality dubbed super-harmonic imaging (SHI) targets a combination of the 3rd–5th harmonics. SHI is expected to yield enhanced spatial resolution and thus to increase the quality of echographic images. On the other hand, those images obtained using short imaging pulses are susceptible to so-called multiple axial reflection artifacts, stemming from the troughs in between harmonics in the frequency domain. The recently proposed dual-pulse frequency compounding method suppresses these artifacts but reduces the frame rate by a factor of 2. In this work we research the feasibility of employing a chirp protocol to perform SHI without compromising the frame rate. The chirp protocol was implemented using an interleaved phased array transducer (44 elements tuned at 1 MHz, 44 elements at 3.7 MHz) in combination with a fully programmable ultrasound system. The transducer was mounted in the side of a water-filled tank. Linear chirps with a center frequency of 1 MHz and a bandwidth of 40% were used as excitation pulses. Radio frequency traces were recorded at the focal plane along the lateral axis using a hydrophone, filtered over the superharmonic band and convolved with a decoding signal to obtain point spread functions (PSFs). The decoding signal was acquired by simulating the emitted beam using the KZK method for a rectangular aperture. The decoded superharmonic chirp had an SNR of 35–40 dB. Comparing to a the 3rd harmonic produced by a 2.5 cycle 1 MHz Gaussian apodized sine burst transmission the lateral beam width of the superharmonic chirp signal is 0.8 and 0.9 times that of the 3rd harmonic at the −6 dB and −20 dB levels respectively. Regarding the axial beam width, the superharmonic chirp signal has 0.9 and 0.8 times the axial beam width --of the 3rd harmonic at the −6 dB and −20 dB levels respectively. The superharmonic chirp PSF is virtually free from imaging artifacts. Based on the SNR measurements the chirp protocol yields a sufficient dynamic range. The PSF has increased spatial resolution in comparison with the 3rd harmonic. The first in-vitro images show promise, but the decoding pulse requires improvement.
机译:在医学超声中,通常通过分析来自2 谐波带的反射回波来获得生物组织的谐波图像。一种被称为超谐波成像(SHI)的新模态以3 rd –5 th 谐波的组合为目标。预期SHI可以提高空间分辨率,从而提高回波图像的质量。另一方面,使用短成像脉冲获得的那些图像容易受到所谓的多个轴向反射伪像的影响,这些伪像源自频域中谐波之间的波谷。最近提出的双脉冲频率复合方法抑制了这些伪像,但是将帧速率降低了2倍。在这项工作中,我们研究了采用线性调频协议执行SHI而不损害帧速率的可行性。 an协议使用交错相控阵换能器(以1 MHz调谐的44个元件,以3.7 MHz调谐的44个元件)结合完全可编程的超声系统来实现。换能器安装在充满水的水箱的侧面。中心频率为1 MHz且带宽为40%的线性chi用作激励脉冲。使用水听器在焦平面上沿横轴记录射频轨迹,在超谐波频带上进行滤波,并与解码信号进行卷积以获得点扩展函数(PSF)。通过使用用于矩形孔径的KZK方法模拟发射光束来获取解码信号。解码的超谐波线性调频器的信噪比为35–40 dB。与2.5周期1 MHz高斯切趾正弦脉冲传输产生的3 rd 谐波相比,超谐波chi信号的横向波束宽度是3 rd 的0.8和0.9倍。 sup>分别在-6 dB和-20 dB的谐波。关于轴向波束宽度,超谐波线性调频信号的强度是轴向波束宽度的0.9和0.8倍- -- 分别在-6 dB和-20 dB的水平上的3 rd 谐波的幅度。超谐波线性调频PSF实际上没有成像伪影。基于SNR测量,线性调频协议产生足够的动态范围。与3 rd 谐波相比,PSF具有更高的空间分辨率。最初的体外图像显示出希望,但是解码脉冲需要改进。

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