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We report a coregistered ultrasound and photoacoustic imaging protocol for the transvaginal imaging of ovarian/adnexal lesions. The protocol may be valuable to other translational photoacoustic imaging studies, especially those using commercial ultrasound arrays for the detection of photoacoustic signals and standard delay-and-sum beamforming algorithms for imaging.
Ovarian cancer remains the deadliest of all the gynecological malignancies due to the lack of reliable screening tools for early detection and diagnosis. Photoacoustic imaging or tomography (PAT) is an emerging imaging modality that can provide the total hemoglobin concentration (relative scale, rHbT) and blood oxygen saturation (%sO2) of ovarian/adnexal lesions, which are important parameters for cancer diagnosis. Combined with coregistered ultrasound (US), PAT has demonstrated great potential for detecting ovarian cancers and for accurately diagnosing ovarian lesions for effective risk assessment and the reduction of unnecessary surgeries of benign lesions. However, PAT imaging protocols in clinical applications, to our knowledge, largely vary among different studies. Here, we report a transvaginal ovarian cancer imaging protocol that can be beneficial to other clinical studies, especially those using commercial ultrasound arrays for the detection of photoacoustic signals and standard delay-and-sum beamforming algorithms for imaging.
Photoacoustic imaging or tomography (PAT) is a hybrid imaging modality that measures the optical absorption distribution at US resolution and depths far beyond the tissue optical diffusion limit (~1 mm). In PAT, a nanosecond laser pulse is used to excite biological tissue, causing a transient temperature rise due to optical absorption. This leads to an initial pressure rise, and the resultant photoacoustic waves are measured by US transducers. Multispectral PAT involves the use of either a tunable laser or multiple lasers operating at different wavelengths to illuminate the tissue, thereby enabling the reconstruction of optical absorption maps at multiple wavelengths.....
All the research performed was approved by the Washington University Institutional Review Board.
1. System configuration: Optical illumination (Figure 1)
Here, we show examples of malignant and normal ovarian lesions imaged by USPAT. Figure 3 shows a 50 year old premenopausal woman with bilateral multicystic adnexal masses revealed by contrast-enhanced CT. Figure 3A shows the US image of the left adnexa with the ROI marking the suspicious solid nodule inside the cystic lesion. Figure 3B shows the PAT rHbT map superimposed onto the US and shown in red. The rHbT showed extensive diffus.......
Optical illumination
The number of fibers used is based on two factors: light illumination uniformity and system complexity. It is critical to have a uniform light illumination pattern at the skin surface to avoid hot spots. It is also important to keep the system simple and robust with a minimal number of fibers. The use of four separate fibers has previously been shown to be optimal for creating uniform illumination at depths of several millimeters and beyond. Additionally, the light coupling to .......
This work was supported by the NCI (R01CA151570, R01CA237664). The authors thank the entire GYN oncology group led by Dr. Mathew Powell for helping with recruiting patients, radiologists Drs. Cary Siegel, William Middleton, and Malak Itnai for helping with the US studies, and the pathologist Dr. Ian Hagemann for helping with the pathology interpretation of the data. The authors gratefully acknowledge the efforts of Megan Luther and the GYN study coordinators in coordinating the study schedules, identifying patients for the study, and obtaining informed consent.
....Name | Company | Catalog Number | Comments |
Clinical US imaging system | Alpinion Medical Systems | EC-12R | Fully programmable clinical US system |
Dielectric mirror | Thorlabs | BB1-E03 | Used to reflect light along the optical path |
Endocavity US transducer | Alpinion Medical Systems | EC3-10 | Transvaginal ultrasound probe |
Laser power meter | Coherent | LabMax TOP | Used to measure laser energy |
Multi-mode optical fiber | Thorlabs | FP1000ERT | Couple laser light to the endocavity ultrasound probe |
Non-polarizing beam splitter plate | Thorlabs | BSW11 | For splitting laser beam into sensors to measure energy |
Plano-concave lens | Thorlabs | LC1715 | For laser beam expansion |
Plano-convex lens | Thorlabs | LA1484-B | For laser beam collimation |
Plano-convex lens | Thorlabs | LA1433-B | Used to focus light into four optical fibers |
Polarizing beam splitter cube | Thorlabs | PBS252 | For splitting laser beam into four beams |
Protective probe shealth | Custom 3D printed | Hold and protect the four optical fibers at the tip of the ultrasound probe | |
Right angle prism mirror | Thorlabs | MRA25-E03 | Used to reflect light along the optical path |
Tunable laser system | Symphotic TII | LS-2145-LT50PC | Light source for multispectral PAT |
USPAT control software | Custom developed in C++ | Controls acquisition parameters of the ultrasound machine and the laser wavelength | |
USPAT image display software | Custom developed in C++ | Displays the US/PAT B-scans and sO2/rHbT maps in real time |
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