Loading…
Two-sided residual refocusing for an acoustic lens-based photoacoustic imaging system
In photoacoustic (PA) cameras, an acoustic lens-based system can form a focused image of an object plane. A real-time C-scan PA image can be formed by simply time gating the transducer response. While most of the focusing action is performed by the lens, residual refocusing is needed to image multip...
Saved in:
Published in: | Physics in medicine & biology 2018-07, Vol.63 (13), p.13NT03-13NT03 |
---|---|
Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
cited_by | cdi_FETCH-LOGICAL-c466t-cbdc6f1a5e7b280c605648c59fe853e73076ae847e1f1019c7e4420ea77a23813 |
---|---|
cites | cdi_FETCH-LOGICAL-c466t-cbdc6f1a5e7b280c605648c59fe853e73076ae847e1f1019c7e4420ea77a23813 |
container_end_page | 13NT03 |
container_issue | 13 |
container_start_page | 13NT03 |
container_title | Physics in medicine & biology |
container_volume | 63 |
creator | Francis, Kalloor Joseph Chinni, Bhargava Channappayya, Sumohana S Pachamuthu, Rajalakshmi Dogra, Vikram S Rao, Navalgund |
description | In photoacoustic (PA) cameras, an acoustic lens-based system can form a focused image of an object plane. A real-time C-scan PA image can be formed by simply time gating the transducer response. While most of the focusing action is performed by the lens, residual refocusing is needed to image multiple depths with high resolution simultaneously. However, a refocusing algorithm for a PA camera has not been studied so far in the literature. In this work, we reformulate this residual refocusing problem for a PA camera into a two-sided wave propagation from a planar sensor array. One part of the problem deals with forward wave propagation while the other deals with time reversal. We have chosen a fast Fourier transform (FFT) based wave propagation model for the refocusing to maintain the real-time nature of the system. We have conducted point spread function (PSF) measurement experiments at multiple depths and refocused the signal using the proposed method. The full width at half maximum (FWHM), peak value and signal to noise ratio (SNR) of the refocused PSF is analyzed to quantify the effect of refocusing. We believe that using a two-dimensional transducer array combined with the proposed refocusing can lead to real-time volumetric imaging using a PA camera. |
doi_str_mv | 10.1088/1361-6560/aac8c5 |
format | article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1088_1361_6560_aac8c5</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2047282990</sourcerecordid><originalsourceid>FETCH-LOGICAL-c466t-cbdc6f1a5e7b280c605648c59fe853e73076ae847e1f1019c7e4420ea77a23813</originalsourceid><addsrcrecordid>eNp9kctL7TAQxoNc0eNj7-rSpQurk-bZjXARXyC6Oa5Dmk6PlbapTav435ty9OAFEQITMr_5MvMNIUcUTilofUaZpKkUEs6sddqJLbLYPP0hCwBG05wKsUv2QngGoFRnfIfsZrnmkiqxII_LN5-GusQyGTDGyTbxUnk3hbpbJZUfEtsl1vkpjLVLGuxCWtgQ8f7Jj36TqFu7mgvCexixPSDblW0CHn7GffJ4dbm8uEnvHq5vL_7dpY5LOaauKJ2sqBWoikyDkyAkj2PkFWrBUDFQ0qLmCmlFgeZOIecZoFXKZkxTtk_O17r9VLRYOuzGwTamH2I7w7vxtjb_Z7r6yaz8q5HAQeSzwPGnwOBfJgyjaevgsGlsh3EykwFXmc7yHCIKa9QNPoTo0eYbCmbehpmtN7P1Zr2NWPL3e3ubgi_7I3CyBmrfm2c_DV106ze94x_wvi2MZJGO534JzPRlxT4AS4ejgQ</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2047282990</pqid></control><display><type>article</type><title>Two-sided residual refocusing for an acoustic lens-based photoacoustic imaging system</title><source>Institute of Physics:Jisc Collections:IOP Publishing Read and Publish 2024-2025 (Reading List)</source><creator>Francis, Kalloor Joseph ; Chinni, Bhargava ; Channappayya, Sumohana S ; Pachamuthu, Rajalakshmi ; Dogra, Vikram S ; Rao, Navalgund</creator><creatorcontrib>Francis, Kalloor Joseph ; Chinni, Bhargava ; Channappayya, Sumohana S ; Pachamuthu, Rajalakshmi ; Dogra, Vikram S ; Rao, Navalgund</creatorcontrib><description>In photoacoustic (PA) cameras, an acoustic lens-based system can form a focused image of an object plane. A real-time C-scan PA image can be formed by simply time gating the transducer response. While most of the focusing action is performed by the lens, residual refocusing is needed to image multiple depths with high resolution simultaneously. However, a refocusing algorithm for a PA camera has not been studied so far in the literature. In this work, we reformulate this residual refocusing problem for a PA camera into a two-sided wave propagation from a planar sensor array. One part of the problem deals with forward wave propagation while the other deals with time reversal. We have chosen a fast Fourier transform (FFT) based wave propagation model for the refocusing to maintain the real-time nature of the system. We have conducted point spread function (PSF) measurement experiments at multiple depths and refocused the signal using the proposed method. The full width at half maximum (FWHM), peak value and signal to noise ratio (SNR) of the refocused PSF is analyzed to quantify the effect of refocusing. We believe that using a two-dimensional transducer array combined with the proposed refocusing can lead to real-time volumetric imaging using a PA camera.</description><identifier>ISSN: 0031-9155</identifier><identifier>ISSN: 1361-6560</identifier><identifier>EISSN: 1361-6560</identifier><identifier>DOI: 10.1088/1361-6560/aac8c5</identifier><identifier>PMID: 29846175</identifier><identifier>CODEN: PHMBA7</identifier><language>eng</language><publisher>England: IOP Publishing</publisher><subject>acoustic lens ; ex vivo ; photoacoustic imaging ; refocusing</subject><ispartof>Physics in medicine & biology, 2018-07, Vol.63 (13), p.13NT03-13NT03</ispartof><rights>2018 Institute of Physics and Engineering in Medicine</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c466t-cbdc6f1a5e7b280c605648c59fe853e73076ae847e1f1019c7e4420ea77a23813</citedby><cites>FETCH-LOGICAL-c466t-cbdc6f1a5e7b280c605648c59fe853e73076ae847e1f1019c7e4420ea77a23813</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,27901,27902</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/29846175$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Francis, Kalloor Joseph</creatorcontrib><creatorcontrib>Chinni, Bhargava</creatorcontrib><creatorcontrib>Channappayya, Sumohana S</creatorcontrib><creatorcontrib>Pachamuthu, Rajalakshmi</creatorcontrib><creatorcontrib>Dogra, Vikram S</creatorcontrib><creatorcontrib>Rao, Navalgund</creatorcontrib><title>Two-sided residual refocusing for an acoustic lens-based photoacoustic imaging system</title><title>Physics in medicine & biology</title><addtitle>PMB</addtitle><addtitle>Phys. Med. Biol</addtitle><description>In photoacoustic (PA) cameras, an acoustic lens-based system can form a focused image of an object plane. A real-time C-scan PA image can be formed by simply time gating the transducer response. While most of the focusing action is performed by the lens, residual refocusing is needed to image multiple depths with high resolution simultaneously. However, a refocusing algorithm for a PA camera has not been studied so far in the literature. In this work, we reformulate this residual refocusing problem for a PA camera into a two-sided wave propagation from a planar sensor array. One part of the problem deals with forward wave propagation while the other deals with time reversal. We have chosen a fast Fourier transform (FFT) based wave propagation model for the refocusing to maintain the real-time nature of the system. We have conducted point spread function (PSF) measurement experiments at multiple depths and refocused the signal using the proposed method. The full width at half maximum (FWHM), peak value and signal to noise ratio (SNR) of the refocused PSF is analyzed to quantify the effect of refocusing. We believe that using a two-dimensional transducer array combined with the proposed refocusing can lead to real-time volumetric imaging using a PA camera.</description><subject>acoustic lens</subject><subject>ex vivo</subject><subject>photoacoustic imaging</subject><subject>refocusing</subject><issn>0031-9155</issn><issn>1361-6560</issn><issn>1361-6560</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNp9kctL7TAQxoNc0eNj7-rSpQurk-bZjXARXyC6Oa5Dmk6PlbapTav435ty9OAFEQITMr_5MvMNIUcUTilofUaZpKkUEs6sddqJLbLYPP0hCwBG05wKsUv2QngGoFRnfIfsZrnmkiqxII_LN5-GusQyGTDGyTbxUnk3hbpbJZUfEtsl1vkpjLVLGuxCWtgQ8f7Jj36TqFu7mgvCexixPSDblW0CHn7GffJ4dbm8uEnvHq5vL_7dpY5LOaauKJ2sqBWoikyDkyAkj2PkFWrBUDFQ0qLmCmlFgeZOIecZoFXKZkxTtk_O17r9VLRYOuzGwTamH2I7w7vxtjb_Z7r6yaz8q5HAQeSzwPGnwOBfJgyjaevgsGlsh3EykwFXmc7yHCIKa9QNPoTo0eYbCmbehpmtN7P1Zr2NWPL3e3ubgi_7I3CyBmrfm2c_DV106ze94x_wvi2MZJGO534JzPRlxT4AS4ejgQ</recordid><startdate>20180702</startdate><enddate>20180702</enddate><creator>Francis, Kalloor Joseph</creator><creator>Chinni, Bhargava</creator><creator>Channappayya, Sumohana S</creator><creator>Pachamuthu, Rajalakshmi</creator><creator>Dogra, Vikram S</creator><creator>Rao, Navalgund</creator><general>IOP Publishing</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>5PM</scope></search><sort><creationdate>20180702</creationdate><title>Two-sided residual refocusing for an acoustic lens-based photoacoustic imaging system</title><author>Francis, Kalloor Joseph ; Chinni, Bhargava ; Channappayya, Sumohana S ; Pachamuthu, Rajalakshmi ; Dogra, Vikram S ; Rao, Navalgund</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c466t-cbdc6f1a5e7b280c605648c59fe853e73076ae847e1f1019c7e4420ea77a23813</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>acoustic lens</topic><topic>ex vivo</topic><topic>photoacoustic imaging</topic><topic>refocusing</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Francis, Kalloor Joseph</creatorcontrib><creatorcontrib>Chinni, Bhargava</creatorcontrib><creatorcontrib>Channappayya, Sumohana S</creatorcontrib><creatorcontrib>Pachamuthu, Rajalakshmi</creatorcontrib><creatorcontrib>Dogra, Vikram S</creatorcontrib><creatorcontrib>Rao, Navalgund</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Physics in medicine & biology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Francis, Kalloor Joseph</au><au>Chinni, Bhargava</au><au>Channappayya, Sumohana S</au><au>Pachamuthu, Rajalakshmi</au><au>Dogra, Vikram S</au><au>Rao, Navalgund</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Two-sided residual refocusing for an acoustic lens-based photoacoustic imaging system</atitle><jtitle>Physics in medicine & biology</jtitle><stitle>PMB</stitle><addtitle>Phys. Med. Biol</addtitle><date>2018-07-02</date><risdate>2018</risdate><volume>63</volume><issue>13</issue><spage>13NT03</spage><epage>13NT03</epage><pages>13NT03-13NT03</pages><issn>0031-9155</issn><issn>1361-6560</issn><eissn>1361-6560</eissn><coden>PHMBA7</coden><abstract>In photoacoustic (PA) cameras, an acoustic lens-based system can form a focused image of an object plane. A real-time C-scan PA image can be formed by simply time gating the transducer response. While most of the focusing action is performed by the lens, residual refocusing is needed to image multiple depths with high resolution simultaneously. However, a refocusing algorithm for a PA camera has not been studied so far in the literature. In this work, we reformulate this residual refocusing problem for a PA camera into a two-sided wave propagation from a planar sensor array. One part of the problem deals with forward wave propagation while the other deals with time reversal. We have chosen a fast Fourier transform (FFT) based wave propagation model for the refocusing to maintain the real-time nature of the system. We have conducted point spread function (PSF) measurement experiments at multiple depths and refocused the signal using the proposed method. The full width at half maximum (FWHM), peak value and signal to noise ratio (SNR) of the refocused PSF is analyzed to quantify the effect of refocusing. We believe that using a two-dimensional transducer array combined with the proposed refocusing can lead to real-time volumetric imaging using a PA camera.</abstract><cop>England</cop><pub>IOP Publishing</pub><pmid>29846175</pmid><doi>10.1088/1361-6560/aac8c5</doi><tpages>7</tpages><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0031-9155 |
ispartof | Physics in medicine & biology, 2018-07, Vol.63 (13), p.13NT03-13NT03 |
issn | 0031-9155 1361-6560 1361-6560 |
language | eng |
recordid | cdi_crossref_primary_10_1088_1361_6560_aac8c5 |
source | Institute of Physics:Jisc Collections:IOP Publishing Read and Publish 2024-2025 (Reading List) |
subjects | acoustic lens ex vivo photoacoustic imaging refocusing |
title | Two-sided residual refocusing for an acoustic lens-based photoacoustic imaging system |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-30T23%3A55%3A36IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Two-sided%20residual%20refocusing%20for%20an%20acoustic%20lens-based%20photoacoustic%20imaging%20system&rft.jtitle=Physics%20in%20medicine%20&%20biology&rft.au=Francis,%20Kalloor%20Joseph&rft.date=2018-07-02&rft.volume=63&rft.issue=13&rft.spage=13NT03&rft.epage=13NT03&rft.pages=13NT03-13NT03&rft.issn=0031-9155&rft.eissn=1361-6560&rft.coden=PHMBA7&rft_id=info:doi/10.1088/1361-6560/aac8c5&rft_dat=%3Cproquest_cross%3E2047282990%3C/proquest_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c466t-cbdc6f1a5e7b280c605648c59fe853e73076ae847e1f1019c7e4420ea77a23813%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=2047282990&rft_id=info:pmid/29846175&rfr_iscdi=true |