{"title":"Photoacoustic Shock Waves and Sound Velocities in Metal Vapors","authors":"A. Tam, K. Chiang, W. Imaino","doi":"10.1364/pas.1981.mb1","DOIUrl":null,"url":null,"abstract":"Most photoacoustic experiments are concerned with the generation and detection of small amplitude sound waves after optical absorption. In this paper, we study the opposite case: generation and detection of large amplitude shock waves by a pulsed laser. The generation is achieved by taking advantage of the efficient ionization of metal vapors by resonant1 or quasi-resonant2,3 laser beams. In general, photoacoustic generation can be due to various causes; for example: collisional deexcitation resulting in thermal expansion, photodissociation, gas evolution, photoionization and optical breakdown, and so on. For the present case of optical breakdown in a vapor, the photoacoustic generation efficiency can be especially high, because ionization causes an increase in the total particle density, and also the electrons produced usually have large kinetic energies. Hence, large-amplitude shock waves can be generated by laser-induced breakdown.","PeriodicalId":202661,"journal":{"name":"Second International Meeting on Photoacoustic Spectroscopy","volume":"24 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Second International Meeting on Photoacoustic Spectroscopy","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/pas.1981.mb1","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Most photoacoustic experiments are concerned with the generation and detection of small amplitude sound waves after optical absorption. In this paper, we study the opposite case: generation and detection of large amplitude shock waves by a pulsed laser. The generation is achieved by taking advantage of the efficient ionization of metal vapors by resonant1 or quasi-resonant2,3 laser beams. In general, photoacoustic generation can be due to various causes; for example: collisional deexcitation resulting in thermal expansion, photodissociation, gas evolution, photoionization and optical breakdown, and so on. For the present case of optical breakdown in a vapor, the photoacoustic generation efficiency can be especially high, because ionization causes an increase in the total particle density, and also the electrons produced usually have large kinetic energies. Hence, large-amplitude shock waves can be generated by laser-induced breakdown.