Lu Jian-Yu
IEEE Trans Ultrason Ferroelectr Freq Control. 2024 Jan;71(1):153-171. doi: 10.1109/TUFFC.2023.3335883. Epub 2024 Jan 9.
High image resolution is desired in wave-related areas such as ultrasound, acoustics, optics, and electromagnetics. However, the spatial resolution of an imaging system is limited by the spatial frequency of the point spread function (PSF) of the system due to diffraction. In this article, the PSF is modulated in amplitude, phase, or both to increase the spatial frequency to reconstruct super-resolution images of objects or wave sources/fields, where the modulator can be a focused shear wave produced remotely by, for example, a radiation force from a focused Bessel beam or X-wave, or can be a small particle manipulated remotely by a radiation-force (such as acoustic and optical tweezers) or electrical and magnetic forces. A theory of the PSF-modulation method was developed, and computer simulations and experiments were conducted. The result of an ultrasound experiment shows that a pulse-echo (two-way) image reconstructed has a super-resolution (0.65 mm) as compared to the diffraction limit (2.65 mm) using a 0.5-mm-diameter modulator at 1.483-mm wavelength, and the signal-to-noise ratio (SNR) of the image was about 31 dB. If the minimal SNR of a "visible" image is 3, the resolution can be further increased to about 0.19 mm by decreasing the size of the modulator. Another ultrasound experiment shows that a wave source was imaged (one-way) at about 30-dB SNR using the same modulator size and wavelength above. The image clearly separated two 0.5-mm spaced lines, which gives a 7.26-fold higher resolution than that of the diffraction limit (3.63 mm). Although, in theory, the method has no limit on the highest achievable image resolution, in practice, the resolution is limited by noises. Also, a PSF-weighted super-resolution imaging method based on the PSF-modulation method was developed. This method is easier to implement but may have some limitations. Finally, the methods above can be applied to imaging systems of an arbitrary PSF and can produce 4-D super-resolution images. With a proper choice of a modulator (e.g., a quantum dot) and imaging system, nanoscale (a few nanometers) imaging is possible.
在超声、声学、光学和电磁学等与波相关的领域,需要高图像分辨率。然而,由于衍射,成像系统的空间分辨率受到系统点扩散函数(PSF)空间频率的限制。在本文中,对PSF进行幅度、相位或两者的调制,以提高空间频率,从而重建物体或波源/场的超分辨率图像,其中调制器可以是由例如聚焦贝塞尔光束或X波的辐射力远程产生的聚焦剪切波,或者可以是由辐射力(如声学和光学镊子)或电磁力远程操纵的小颗粒。开发了PSF调制方法的理论,并进行了计算机模拟和实验。超声实验结果表明,使用直径为0.5毫米的调制器,在波长为1.483毫米时,重建的脉冲回波(双向)图像与衍射极限(2.65毫米)相比具有超分辨率(0.65毫米),并且图像的信噪比(SNR)约为31分贝。如果“可见”图像的最小SNR为3,则通过减小调制器的尺寸,分辨率可进一步提高到约0.19毫米。另一个超声实验表明,使用上述相同的调制器尺寸和波长,以约30分贝的SNR对波源进行了成像(单向)。图像清晰地分离了两条间距为0.5毫米的线,其分辨率比衍射极限(3.63毫米)高7.26倍。虽然理论上该方法对可实现的最高图像分辨率没有限制,但在实际中,分辨率受到噪声的限制。此外,还开发了一种基于PSF调制方法的PSF加权超分辨率成像方法。该方法更易于实现,但可能有一些局限性。最后,上述方法可应用于任意PSF的成像系统,并可产生4D超分辨率图像。通过适当选择调制器(例如量子点)和成像系统,实现纳米级(几纳米)成像成为可能。