基于啁啾的超谐波成像

M. Danilouchkine, P. van Neer, G. Matte, M. Voormolen, M. Verweij, N. de Jong
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引用次数: 4

摘要

在医学超声中,生物组织的谐波图像通常是通过分析二次谐波波段的反射回波来获得的。一种被称为超谐波成像(SHI)的新模式针对的是3 - 5次谐波的组合。SHI有望产生增强的空间分辨率,从而提高超声图像的质量。另一方面,使用短成像脉冲获得的图像容易受到所谓的多轴向反射伪影的影响,这些伪影源于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影,但将帧率降低了2倍。在这项工作中,我们研究了在不影响帧速率的情况下使用chirp协议来执行SHI的可行性。啁啾协议使用交错相控阵换能器(44个元件在1 MHz调谐,44个元件在3.7 MHz调谐)与完全可编程的超声系统相结合来实现。换能器安装在一个装满水的水箱的侧面。采用中心频率为1mhz、带宽为40%的线性啁啾作为激励脉冲。利用水听器沿横向轴记录焦平面上的射频迹线,在超谐波波段上进行滤波,并与解码信号进行卷积以获得点扩展函数(psf)。采用矩形孔径的KZK方法模拟发射光束,获得解码信号。解码后的超谐波啁啾信噪比为35-40 dB。与2.5周1 MHz高斯离化正弦突发传输产生的3次谐波相比,超谐波啁啾信号在- 6 dB和- 20 dB电平的横向波束宽度分别是3次谐波的0.8倍和0.9倍。在轴向波束宽度方面,超谐波啁啾信号在−6 dB和−20 dB水平分别是三次谐波轴向波束宽度的0.9倍和0.8倍。超谐波啁啾PSF几乎没有成像伪影。基于信噪比测量,啁啾协议产生足够的动态范围。与三次谐波相比,PSF提高了空间分辨率。第一批体外图像显示出了希望,但解码脉冲需要改进。
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Superharmonic imaging based on chirps
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.
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