Please use this identifier to cite or link to this item: https://doi.org/10.1364/OE.397727
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dc.titleTime delay effect in a microchip pulse laser for the nonlinear photoacoustic signal enhancement
dc.contributor.authorEnbo Xing
dc.contributor.authorYu-Hang Liu
dc.contributor.authorJiamin Rong
dc.contributor.authorWenyao Liu
dc.contributor.authorJun Tang
dc.contributor.authorJun Liu
dc.contributor.authorNitish Thakor
dc.contributor.authorMinghui Hong
dc.date.accessioned2021-04-09T05:59:03Z
dc.date.available2021-04-09T05:59:03Z
dc.date.issued2020-07-20
dc.identifier.citationEnbo Xing, Yu-Hang Liu, Jiamin Rong, Wenyao Liu, Jun Tang, Jun Liu, Nitish Thakor, Minghui Hong (2020-07-20). Time delay effect in a microchip pulse laser for the nonlinear photoacoustic signal enhancement. Optics Express 28 (16) : 23154 - 23163. ScholarBank@NUS Repository. https://doi.org/10.1364/OE.397727
dc.identifier.issn10944087
dc.identifier.urihttps://scholarbank.nus.edu.sg/handle/10635/188960
dc.description.abstractThe Grüneisen relaxation effect has been successfully employed to improve the photoacoustic (PA) imaging contrast. However, complex system design and cost hinder the progress from benchside to bedside, since an additional pre-heating laser source needs to be coupled into the original light path and synchronized with other equipment for conducting the nonlinear effect. To overcome the limitation, we propose a time delay heating PA imaging (TDH-PAI) method based on the time delay effect in a passively Q-switched laser. Experimentally, only one single microchip pulse laser is built and utilized for the nonlinear PA signal enhancement without additional components. The 808 nm pump pulse of the laser diode and the excited 1064 nm pulse are respectively used for pre-heating and acquiring PA signals. The heating effect is optimized by adjusting the input parameters and an enhancement of more than 30% in PA signals is achieved. TDH-PAI reduces the cost and complexity of the nonlinear PA system, which provides an efficient way for achieving a high-contrast PA imaging. © 2020 Optical Society of America.
dc.language.isoen
dc.publisherOSA - The Optical Society
dc.sourceScopus
dc.typeArticle
dc.contributor.departmentELECTRICAL AND COMPUTER ENGINEERING
dc.description.doi10.1364/OE.397727
dc.description.sourcetitleOptics Express
dc.description.volume28
dc.description.issue16
dc.description.page23154 - 23163
dc.published.statePublished
dc.grant.id2019L0569
dc.grant.id2019L0588
dc.grant.idNRF-CRP15-2015-04
dc.grant.id61803350
dc.grant.id201901D211236
dc.grant.id201901D211243
dc.grant.fundingagencyScience and Technology Innovation Project of Shanxi Province
dc.grant.fundingagencyNational Research Foundation Singapore
dc.grant.fundingagencyShanxi Province Science Foundation for Youths
dc.grant.fundingagencyNational Natural Science Foundation of China
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