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. 2023 May 16:14:1150416.
doi: 10.3389/fimmu.2023.1150416. eCollection 2023.

Noninvasive mechanical destruction of liver tissue and tissue decellularisation by pressure-modulated shockwave histotripsy

Affiliations

Noninvasive mechanical destruction of liver tissue and tissue decellularisation by pressure-modulated shockwave histotripsy

Ki Joo Pahk et al. Front Immunol. .

Abstract

Introduction: Boiling histotripsy (BH) is a promising High Intensity Focused Ultrasound (HIFU) technique that can be used to mechanically fractionate solid tumours at the HIFU focus noninvasively, promoting tumour immunity. Because of the occurrence of shock scattering phenomenon during BH process, the treatment accuracy of BH is, however, somewhat limited. To induce more localised and selective tissue destruction, the concept of pressure modulation has recently been proposed in our previous in vitro tissue phantom study. The aim of the present study was therefore to investigate whether this newly developed histotripsy approach termed pressure-modulated shockwave histotripsy (PSH) can be used to induce localised mechanical tissue fractionation in in vivo animal model.

Methods: In the present study, 8 Sprague Dawley rats underwent the PSH treatment and were sacrificed immediately after the exposure for morphological and histological analyses (paraffin embedded liver tissue sections were stained with H&E and MT). Partially exteriorised rat's left lateral liver lobe in vivo was exposed to a 2.0 MHz HIFU transducer with peak positive (P +) and negative (P -) pressures of 89.1 MPa and -14.6 MPa, a pulse length of 5 to 34 ms, a pressure modulation time at 4 ms where P + and P - decreased to 29.9 MPa and - 9.6 MPa, a pulse repetition frequency of 1 Hz, a duty cycle of 1% and number of pulses of 1 to 20. Three lesions were produced on each animal. For comparison, the same exposure condition but no pressure modulation was also employed to create a number of lesions in the liver.

Results and discussion: Experimental results showed that a partial mechanical destruction of liver tissue in the form of an oval in the absence of thermal damage was clearly observed at the HIFU focus after the PSH exposure. With a single pulse length of 7 ms, a PSH lesion created in the liver was measured to be a length of 1.04 ± 0.04 mm and a width of 0.87 ± 0.21 mm which was 2.37 times in length (p = 0.027) and 1.35 times in width (p = 0.1295) smaller than a lesion produced by no pressure modulation approach (e.g., BH). It was also observed that the length of a PSH lesion gradually grew towards the opposite direction to the HIFU source along the axial direction with the PSH pulse length, eventually leading to the generation of an elongated lesion in the liver. In addition, our experimental results demonstrated the feasibility of inducing partial decellularisation effect where liver tissue was partially destructed with intact extracellular matrix (i.e., intact fibrillar collagen) with the shortest PSH pulse length. Taken together, these results suggest that PSH could be used to induce a highly localised tissue fractionation with a desired degree of mechanical damage from complete tissue fractionation to tissue decellularisation through controlling the dynamics of boiling bubbles without inducing the shock scattering effect.

Keywords: boiling histotripsy; cavitation; high intensity focused ultrasound; immunotherapy; pressure-modulated shockwave histotripsy; tissue decellularisation; tumour destruction.

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Conflict of interest statement

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Figures

Figure 1
Figure 1
HIFU experimental setup used in the present study. Photographs of (A) exteriorised liver prior to HIFU exposure and (B) during the exposure. (C) Pressure modulated acoustic waveforms at the HIFU focus used in the PSH approach. PSH, pressure-modulated shockwave histotripsy.
Figure 2
Figure 2
Morphological and histological observations of freshly created PSH or BH lesions in the liver in vivo. A cross-sectioned PSH lesion produced by (A) 1 pulse, (B) 10 pulses, and (C) 20 pulses with a pulse length of 7 ms, P ,1+ of 89.1 MPa, P ,1– of – 14.6 MPa, P ,2+ of 29.9 MPa, P ,2– of – 9.6 MPa, tm of 4 ms, 1 Hz PRF and 1% DC. (Ai) A photograph of three cross-sectioned PSH lesions after the exposure. (Aii) Formalin-preserved section of (Ai). (Aiii, Bii, Cii) are the corresponding H&E stained liver tissues indicated in (Aii, Bi, Ci), respectively. (Biii, Ciii) are higher magnification of the areas indicated by the yellow squares in (Bii, Cii) respectively. Formalin-preserved cross-sectioned BH lesions produced by (Di) 1 pulse and (Ei) 10 pulses with a pulse length of 7 ms, P + of 89.1 MPa, P of – 14.6 MPa, 1 Hz PRF and 1% DC. (Dii, Eii) are the corresponding H&E stained liver tissues indicated in (Di, Ei). The HIFU beam propagates from top to bottom.
Figure 3
Figure 3
Histological examination of PSH lesions produced in the liver in vivo by a single PSH pulse with P ,1+ of 89.1 MPa, P ,1– of – 14.6 MPa, P ,2+ of 29.9 MPa, P ,2– of – 9.6 MPa at HIFU focus and tm of 4 ms. H&E stained cross-sectioned PSH lesion induced by (Ai) a 5-ms long PSH pulse, (Bi) a 7-ms long PSH pulse, (Ci) a 10-ms long PSH pulse, (Di) a 14-ms long PSH pulse, (Ei) a 24-ms long PSH pulse, and (Fi) 34-ms long PSH pulse. Corresponding MT stained cross-sectioned PSH lesions of (A–F, i) are shown in (Aiii, Biii, Civ, Diii, Eiii, f-iii) respectively. (Aii,iv, Bii,iv, Cii,iii,v,vi, Dii,iv, Eii,iv, Fii,iv) are higher magnifications of the areas indicated by the squares in (Ai, Aiii, Bi, Biii, Ci, Civ, Di, Diii, Ei, Eiii, Fi, Fiii), respectively. The HIFU beam propagates from top to bottom.
Figure 4
Figure 4
Histological observation of cross-sectioned MT-stained treated liver tissue. (A) untreated liver tissue. Treated liver tissue with a single (B) 5 ms long PSH pulse, (C) 7 ms long PSH pulse and (D) 10 ms long PSH pulse. Red arrows indicate the decellularised liver scaffold. The raw MT-stained image of (D) is obtained from Figure 3Cv .

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Grants and funding

This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIT) (No. NRF-2021R1C1C1008240) and a grant from Kyung Hee University in 2022 (KHU-20220903). This work was supported by KOREA HYDRO & NUCLEAR POWER CO., LTD (No. 22-Tech-10). The funder, KOREA HYDRO & NUCLEAR POWER CO., LTD, was not involved in the study design, collection, analysis, interpretation of data, the writing of this article or the decision to submit it for publication.

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