Quantitative Optimization of Handheld Probe External Pressure on Dermatological Microvasculature Using Optical Coherence Tomography-Based Angiography
Optical Coherence Tomography (OCT)-based angiography (OCTA) is a high-resolution, high-speed, and non-invasive imaging method that can provide vascular mapping of subcutaneous tissue up to approximately 2 mm. In dermatology applications of OCTA, handheld probes are always designed with a piece of tr...
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| Published in | Micromachines (Basel) Vol. 15; no. 9; p. 1128 |
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| Main Authors | , , , , , |
| Format | Journal Article |
| Language | English |
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01.09.2024
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| ISSN | 2072-666X 2072-666X |
| DOI | 10.3390/mi15091128 |
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| Abstract | Optical Coherence Tomography (OCT)-based angiography (OCTA) is a high-resolution, high-speed, and non-invasive imaging method that can provide vascular mapping of subcutaneous tissue up to approximately 2 mm. In dermatology applications of OCTA, handheld probes are always designed with a piece of transparent but solid contact window placed at the end of the probe to directly contact the skin for achieving better focusing between the light source and the tissue, reducing noise caused by minor movements. The pressure between the contact window and the skin is usually uncontrollable, and high external pressure affects the quality of microvascular imaging by compressing the vessels and obstructing the underlying blood flow. Therefore, it is necessary to determine a pressure range to ensure that the vessels can be fully imaged in high-quality images. In this paper, two pressure sensors were added to the existing handheld OCT probe, and the imaging probe was fixed to a metal stand and adjusted vertically to change the pressure between the probe and the tested skin site, a gradient of roughly 4 kPa (with 1–2 kPa error) increase was applied in each experiment, and the impact of pressure to the vessel was calculated. The experiment involved a total of five subjects, three areas of which were scanned (palm, back of the hand, and forearm). The vessel density was calculated to evaluate the impact of external pressure on angiography. In addition, PSNR was calculated to ensure that the quality of different tests was at a similar level. The angiography showed the highest density (about 10%) when the pressure between the contact window on the probe and the test area was between 3 and 5 kPa. As the pressure increased, the vascular density decreased, and the rate of decrease varied in different test areas. After fitting all the data points according to the different sites, the slope of the fitted line, i.e., the rate of decrease in density per unit value of pressure, was found to be 4.05% at the palm site, 6.93% at the back of the hand, and 4.55% at the forearm site. This experiment demonstrates that the pressure between the skin and contact window is a significant parameter that cannot be ignored. It is recommended that in future OCTA data collection processes and probe designs, the impact of pressure on the experiment be considered. |
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| AbstractList | Optical Coherence Tomography (OCT)-based angiography (OCTA) is a high-resolution, high-speed, and non-invasive imaging method that can provide vascular mapping of subcutaneous tissue up to approximately 2 mm. In dermatology applications of OCTA, handheld probes are always designed with a piece of transparent but solid contact window placed at the end of the probe to directly contact the skin for achieving better focusing between the light source and the tissue, reducing noise caused by minor movements. The pressure between the contact window and the skin is usually uncontrollable, and high external pressure affects the quality of microvascular imaging by compressing the vessels and obstructing the underlying blood flow. Therefore, it is necessary to determine a pressure range to ensure that the vessels can be fully imaged in high-quality images. In this paper, two pressure sensors were added to the existing handheld OCT probe, and the imaging probe was fixed to a metal stand and adjusted vertically to change the pressure between the probe and the tested skin site, a gradient of roughly 4 kPa (with 1–2 kPa error) increase was applied in each experiment, and the impact of pressure to the vessel was calculated. The experiment involved a total of five subjects, three areas of which were scanned (palm, back of the hand, and forearm). The vessel density was calculated to evaluate the impact of external pressure on angiography. In addition, PSNR was calculated to ensure that the quality of different tests was at a similar level. The angiography showed the highest density (about 10%) when the pressure between the contact window on the probe and the test area was between 3 and 5 kPa. As the pressure increased, the vascular density decreased, and the rate of decrease varied in different test areas. After fitting all the data points according to the different sites, the slope of the fitted line, i.e., the rate of decrease in density per unit value of pressure, was found to be 4.05% at the palm site, 6.93% at the back of the hand, and 4.55% at the forearm site. This experiment demonstrates that the pressure between the skin and contact window is a significant parameter that cannot be ignored. It is recommended that in future OCTA data collection processes and probe designs, the impact of pressure on the experiment be considered. Optical Coherence Tomography (OCT)-based angiography (OCTA) is a high-resolution, high-speed, and non-invasive imaging method that can provide vascular mapping of subcutaneous tissue up to approximately 2 mm. In dermatology applications of OCTA, handheld probes are always designed with a piece of transparent but solid contact window placed at the end of the probe to directly contact the skin for achieving better focusing between the light source and the tissue, reducing noise caused by minor movements. The pressure between the contact window and the skin is usually uncontrollable, and high external pressure affects the quality of microvascular imaging by compressing the vessels and obstructing the underlying blood flow. Therefore, it is necessary to determine a pressure range to ensure that the vessels can be fully imaged in high-quality images. In this paper, two pressure sensors were added to the existing handheld OCT probe, and the imaging probe was fixed to a metal stand and adjusted vertically to change the pressure between the probe and the tested skin site, a gradient of roughly 4 kPa (with 1-2 kPa error) increase was applied in each experiment, and the impact of pressure to the vessel was calculated. The experiment involved a total of five subjects, three areas of which were scanned (palm, back of the hand, and forearm). The vessel density was calculated to evaluate the impact of external pressure on angiography. In addition, PSNR was calculated to ensure that the quality of different tests was at a similar level. The angiography showed the highest density (about 10%) when the pressure between the contact window on the probe and the test area was between 3 and 5 kPa. As the pressure increased, the vascular density decreased, and the rate of decrease varied in different test areas. After fitting all the data points according to the different sites, the slope of the fitted line, i.e., the rate of decrease in density per unit value of pressure, was found to be 4.05% at the palm site, 6.93% at the back of the hand, and 4.55% at the forearm site. This experiment demonstrates that the pressure between the skin and contact window is a significant parameter that cannot be ignored. It is recommended that in future OCTA data collection processes and probe designs, the impact of pressure on the experiment be considered.Optical Coherence Tomography (OCT)-based angiography (OCTA) is a high-resolution, high-speed, and non-invasive imaging method that can provide vascular mapping of subcutaneous tissue up to approximately 2 mm. In dermatology applications of OCTA, handheld probes are always designed with a piece of transparent but solid contact window placed at the end of the probe to directly contact the skin for achieving better focusing between the light source and the tissue, reducing noise caused by minor movements. The pressure between the contact window and the skin is usually uncontrollable, and high external pressure affects the quality of microvascular imaging by compressing the vessels and obstructing the underlying blood flow. Therefore, it is necessary to determine a pressure range to ensure that the vessels can be fully imaged in high-quality images. In this paper, two pressure sensors were added to the existing handheld OCT probe, and the imaging probe was fixed to a metal stand and adjusted vertically to change the pressure between the probe and the tested skin site, a gradient of roughly 4 kPa (with 1-2 kPa error) increase was applied in each experiment, and the impact of pressure to the vessel was calculated. The experiment involved a total of five subjects, three areas of which were scanned (palm, back of the hand, and forearm). The vessel density was calculated to evaluate the impact of external pressure on angiography. In addition, PSNR was calculated to ensure that the quality of different tests was at a similar level. The angiography showed the highest density (about 10%) when the pressure between the contact window on the probe and the test area was between 3 and 5 kPa. As the pressure increased, the vascular density decreased, and the rate of decrease varied in different test areas. After fitting all the data points according to the different sites, the slope of the fitted line, i.e., the rate of decrease in density per unit value of pressure, was found to be 4.05% at the palm site, 6.93% at the back of the hand, and 4.55% at the forearm site. This experiment demonstrates that the pressure between the skin and contact window is a significant parameter that cannot be ignored. It is recommended that in future OCTA data collection processes and probe designs, the impact of pressure on the experiment be considered. |
| Audience | Academic |
| Author | Liao, Jinpeng Zhang, Yilong Zhang, Tianyu Gu, Jiacheng Huang, Zhihong Li, Chunhui |
| AuthorAffiliation | 2 Centre for Medical Engineering and Technology (CMET), School of Science and Engineering, University of Dundee, Dundee DD1 4HN, UK; y.z.z.z.h.zhang@dundee.ac.uk 1 School of Physics, Engineering and Technology, University of York, York YO10 5DD, UK; xgq516@york.ac.uk (J.G.); tqq517@york.ac.uk (J.L.); t.x.zhang@dundee.ac.uk (T.Z.); zhihong.huang@york.ac.uk (Z.H.) |
| AuthorAffiliation_xml | – name: 2 Centre for Medical Engineering and Technology (CMET), School of Science and Engineering, University of Dundee, Dundee DD1 4HN, UK; y.z.z.z.h.zhang@dundee.ac.uk – name: 1 School of Physics, Engineering and Technology, University of York, York YO10 5DD, UK; xgq516@york.ac.uk (J.G.); tqq517@york.ac.uk (J.L.); t.x.zhang@dundee.ac.uk (T.Z.); zhihong.huang@york.ac.uk (Z.H.) |
| Author_xml | – sequence: 1 givenname: Jiacheng surname: Gu fullname: Gu, Jiacheng – sequence: 2 givenname: Jinpeng orcidid: 0000-0001-6287-8079 surname: Liao fullname: Liao, Jinpeng – sequence: 3 givenname: Tianyu orcidid: 0000-0002-4297-2727 surname: Zhang fullname: Zhang, Tianyu – sequence: 4 givenname: Yilong surname: Zhang fullname: Zhang, Yilong – sequence: 5 givenname: Zhihong orcidid: 0000-0003-4569-5400 surname: Huang fullname: Huang, Zhihong – sequence: 6 givenname: Chunhui orcidid: 0000-0003-2186-5137 surname: Li fullname: Li, Chunhui |
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| Cites_doi | 10.1146/annurev.med.56.082103.104649 10.1161/CIRCRESAHA.118.313058 10.1111/jdv.18123 10.1002/jbio.202100152 10.1364/BOE.10.002847 10.1016/j.mvr.2014.09.007 10.1146/annurev-physiol-030212-183802 10.1161/01.CIR.29.6.847 10.1007/s13555-017-0175-4 10.1016/S0741-5214(99)70154-0 10.1364/BOE.10.005755 10.1186/s40942-015-0005-8 10.1111/eci.12493 10.1007/s00417-019-04553-2 10.1038/jidsymp.2011.5 10.3126/ajms.v14i11.52938 10.3390/app13010378 10.1364/OL.41.002330 10.1117/1.JBO.19.5.056003 10.1364/OE.16.015149 10.1364/BOE.486933 10.1002/lsm.22788 10.1364/OL.497080 10.1007/s00421-008-0697-7 10.1109/TIP.2003.819861 10.1111/j.1468-3083.2006.01629.x 10.1152/jappl.1948.1.3.234 |
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| SubjectTerms | Angiography Blood Blood flow Blood vessels Contact pressure Data collection Data points Density Dermatology External pressure Forearm Image compression Image quality Light sources Mean square errors Medical imaging OCTA Optical Coherence Tomography Pressure sensors Sensors Signal to noise ratio Skin Technology application Tomography vessel density |
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| Title | Quantitative Optimization of Handheld Probe External Pressure on Dermatological Microvasculature Using Optical Coherence Tomography-Based Angiography |
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