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Springer Series in Surface Sciences 53 Mihai Stafe Aurelian Marcu Niculae N. Puscas Pulsed Laser Ablation of Solids Basics, Theory and Applications Springer Series in Surface Sciences Volume 53 Series Editors Gerhard Ertl, Berlin, Germany Hans Lüth, Jülich, Germany Douglas L. Mills, Irvine, USA For furthervolumes: http://www.springer.com/series/409 Thisseriescoversthewholespectrumofsurfacesciences,includingstructureand dynamicsofcleanandadsorbate-coveredsurfaces,thinfilms,basicsurfaceeffects, analytical methods and also the physics and chemistry of interfaces. Written by leadingresearchersinthefield,thebooksareintendedprimarilyforresearchersin academia and industry and for graduate students. Mihai Stafe Aurelian Marcu • Niculae N. Puscas Pulsed Laser Ablation of Solids Basics, Theory and Applications 123 Mihai Stafe Aurelian Marcu Niculae N.Puscas Laser Department Department of Physics National InstituteforLaser Plasma and UniversityPolitehnica of Bucharest Radiation Physics Bucharest Bucharest-Magurele Romania Romania ISSN 0931-5195 ISBN 978-3-642-40977-6 ISBN 978-3-642-40978-3 (eBook) DOI 10.1007/978-3-642-40978-3 SpringerHeidelbergNewYorkDordrechtLondon LibraryofCongressControlNumber:2013949439 (cid:2)Springer-VerlagBerlinHeidelberg2014 Thisworkissubjecttocopyright.AllrightsarereservedbythePublisher,whetherthewholeorpartof the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation,broadcasting,reproductiononmicrofilmsorinanyotherphysicalway,andtransmissionor informationstorageandretrieval,electronicadaptation,computersoftware,orbysimilarordissimilar methodology now known or hereafter developed. Exempted from this legal reservation are brief excerpts in connection with reviews or scholarly analysis or material supplied specifically for the purposeofbeingenteredandexecutedonacomputersystem,forexclusiveusebythepurchaserofthe work. Duplication of this publication or parts thereof is permitted only under the provisions of theCopyright Law of the Publisher’s location, in its current version, and permission for use must always be obtained from Springer. Permissions for use may be obtained through RightsLink at the CopyrightClearanceCenter.ViolationsareliabletoprosecutionundertherespectiveCopyrightLaw. The use of general descriptive names, registered names, trademarks, service marks, etc. in this publicationdoesnotimply,evenintheabsenceofaspecificstatement,thatsuchnamesareexempt fromtherelevantprotectivelawsandregulationsandthereforefreeforgeneraluse. While the advice and information in this book are believed to be true and accurate at the date of publication,neithertheauthorsnortheeditorsnorthepublishercanacceptanylegalresponsibilityfor anyerrorsoromissionsthatmaybemade.Thepublishermakesnowarranty,expressorimplied,with respecttothematerialcontainedherein. Printedonacid-freepaper SpringerispartofSpringerScience+BusinessMedia(www.springer.com) Preface Soon after its experimental realization, the laser was used in several practical applications. One of the most important applications of lasers are related to the laser ablation of solids because they offer very important advantages over the classicaltools,includingchoiceofwavelengthandpulsewidthtomatchthetarget material properties as well as one-step direct and locally confined structural modification. Also, using lasers it is possible to reduce the thermo-mechanical damage and to facilitate heterogeneous integration of the components into func- tionaldevices.Theabovementionedadvantagesareveryimportantincaseswhere conventional thermo-chemo-mechanical treatment processes are ineffective. The microfabrication ofseveral componentswith basic dimensions inthe few- microns range via laser irradiation has been implemented successfully in the industrial environment. Beyond this, there is an increasing need to advance the science and technology of laser processing to the nanoscale regime. This book aims at providing young researchers and graduate students with a comprehensive review of progress and the state of the art in the pulsed laser ablation(PLA)fieldlinkingfundamentalphenomenawithrecentapplications.The bookintroducestheresearchersintothefieldofPulsedLaserAblationofSolidsby synthesizing the state-of-the-art of the pulsed laser ablation processes and its applications. The understanding of the evolution of the energy coupling with the target and the induced phase-change transformations plays an important role for improving the quality of the material processing. Thecontentofthebookisbasedonrecentresearchstudiesofdifferentgroupsand includes the authors’ contribution on pulsed laser ablation. In the introductory chapter,severalconsiderationsconcerningthetools,whichareusedforlaserabla- tionofsolidmaterials(metals,semiconductors,dielectrics)arepresented,pointing outthemajorroleofthematerialprocessingusinglasersascomparedtoclassical tools.Also,somepracticalapplicationsofPLAandgeneralaimsareemphasized. In Chap. 2 several lasers for pulsed laser ablation like: Nd-YAG laser, Ti-sapphire laser, excimer laser, CO laser are analyzed concerning the mode 2 operation (pulsed, CW, tunable), pulse duration (nano, pico, femtosecond range), power and operation wavelength (from near UV to far IR range), emphasizing their best capabilities. Also, the Q-switched and mode locked lasers are analyzed v vi Preface together with the most used methods for their practical operation: mechanical, electro-optical, acousto-optical, methods with saturable absorbers and thin films, etc. The knowledge of the laser operation and the parameters is used to control PLA process for different types of solid materials in different ambient conditions. Attheendofthischapterseveralcombinedirradiationmethodsinthefarandnear field (i.e., direct irradiation and projection through masks and microlens array, laser trepanning, andlaser lithography),andsomeeffects ofpulsedurationonthe ablation rate are discussed. TheChap. 3isdevotedtothelaser-matterinteractionbelowtheplasmaignition threshold intensity. The basic linear and non-linear phenomena involved in laser- matter interaction at high intensities: harmonic generation, self focusing, self guiding, absorption and ionization, two-photon absorption, stimulated Raman Effectarecharacterizedfromtheoreticalandexperimentalpointofview.Also,the mostimportantexperimentalmethodsforanalyzingthemainphenomenainvolved inlaser-matterinteractionduringPLAbelowtheplasmaignitionthresholdsuchas reflectometry and analysis of thermal radiation are discussed. The physics of the ablation process is complex, given that it involves laser-solid interactions, the vapor/plasmaformationandexpansion,andthelaser-vaporinteraction.Thephase and/or structural changes induced on the target by the laser radiation can be detected by means of the time-resolved reflectivity (TRR) method, while the thermal changes can be detected by rapid infrared pyrometry (RIP) systems. The coupling of the two methods (RIP and TRR) allows the study of the melting kinetics induced by laser radiation in a large number of bulk metallic, dielectric, and semi-conductor materials. The plasma spectroscopy methods were developed over the past decades and they provide basic data which are needed for the implementation of many of the experimental methods, and to descriptions of instrumentation. A detailed study of the basic mechanisms involved in laser ablation below the plasma ignition threshold is performed at the end of this chapter. The laser-matter interaction above the plasma ignition threshold intensity is presented in the Chap. 4 of this book. At the beginning of this chapter the main phenomena involved in production of the ablation plasma and in laser-plasma interaction during PLA are analysed: plasma heating, critical density, plasma shielding, ablation plume expansion, several types of collisions, etc. Also, in this chapterseveralexperimentalmethodsforanalyzingthemainphenomenainvolved in laser-plasma interaction are presented in detail: optical methods (interfero- metric, Thomson-scattering, spectrometric methods, laser induced fluorescence (LIF) spectroscopy), mass spectroscopy, high speed imaging, etc. The Chap. 5 of the book is devoted to the material removal and deposition by PLA and associated phenomena: micro and nano-processing (patterning) of materials by PLA, material removal in gaseous and liquid etchants, nanoparticle production, pulsed laser deposition and ablation, plume filtering, etc. In Chap. 6, we present several experimental techniques for analyzing the material removal and deposition rates in real time: opto-acoustics and Preface vii interferometricmethods,emission spectroscopyoftheablationplasmaandquartz microbalances. The conclusions of the work are outlined in the last chapter of this book. TheAuthorswishtothankseveralpeoplewhoinfluencedtheirworkinthefield of lasers and laser-mater interaction. Thus, Mihai Stafe wishes to thank to Prof. I.M.PopescuwhosupervisedhisPh.D.workinthefiledofPulsedLaserAblation at Department of Physics at University ‘Politehnica’ of Bucharest, Romania. He also wants to thank to Prof. I. Foldes and Prof. S. Szatmari for the supervision during his postdoctoral studies on High Harmonics Generation on gas jets and solid targets at HILL laser facility at Department of Experimental Physics of University of Szeged, Hungary. Thanks will be also addressed to Prof. G. D. Tsakiris and Prof. F. Krausz from Max-Planck Institute for Quantum-Optics at Garching, Germany for the opportunity to work at LWS 10/20 facility on High Harmonics Generation on solid targets at the relativistic limit. NiculaePuscaswishestothankDr.N.Semmar,Dr.C.Leborgne,andDr.Jean- Michel Pouvesle from GREMI, CNRS/Université d’Orléans, France for the opportunity to work in their research group and for useful discussions. AurelianMarcuwishestothankProf.I.M.Popescutoo,butalsoDr.Constantin Grigoriu from National Institute for Laser Plasma and Radiation Physics from Bucharest-Magurele (Romania) and K. Yatsui from Nagaoka University of Technology, Nagaoka (Japan) who made possible part of the experimental work presented in this book. Bucharest, Romania Mihai Stafe Aurelian Marcu Niculae N. Puscas Contents 1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1 1.1 Short History: Classical Tools Versus Lasers Tools. . . . . . . . . . 2 1.2 Solid Materials (Metals, Semiconductors, Dielectrics) to be Processed by PLA. . . . . . . . . . . . . . . . . . . . . . . . . . . . . 6 1.2.1 Thermally Well-Conducting Materials . . . . . . . . . . . . . 7 1.2.2 Wide-Bandgap Materials, Glasses, Polymers. . . . . . . . . 8 1.3 Practical Applications of PLA and General Aims . . . . . . . . . . . 8 1.3.1 PLD. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8 1.3.2 Cluster Formation by PLA . . . . . . . . . . . . . . . . . . . . . 9 References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 11 2 Lasers for Pulsed Laser Ablation . . . . . . . . . . . . . . . . . . . . . . . . . 15 2.1 CO , Nd-YAG, Ti–Sapphire, Excimers Lasers . . . . . . . . . . . . . 15 2 2.1.1 Nd-YAG Laser . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17 2.1.2 Ti-Sapphire Laser . . . . . . . . . . . . . . . . . . . . . . . . . . . 20 2.1.3 Excimer Laser. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 22 2.1.4 CO Laser . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23 2 2.2 Nano, Pico, Femtosecond Lasers. Q-Switched and Mode Locked Lasers . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25 2.2.1 Nano, Pico, Femtosecond Lasers. . . . . . . . . . . . . . . . . 25 2.2.2 Q-Switched and Mode Locked Lasers . . . . . . . . . . . . . 28 2.3 Laser Parameters to be Controlled in PLA for Different Types of Solid Materials in Different Ambient Conditions. . . . . 39 2.4 Basic Experimental Setup for PLA . . . . . . . . . . . . . . . . . . . . . 44 2.4.1 Combined Irradiation Methods . . . . . . . . . . . . . . . . . . 46 2.4.2 Projection Through Microlens Array . . . . . . . . . . . . . . 47 2.4.3 Laser Trepanning. . . . . . . . . . . . . . . . . . . . . . . . . . . . 48 References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 49 ix x Contents 3 Laser-Matter Interaction Below the Plasma Ignition Threshold Intensity . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 53 3.1 Linear and Non-linear Phenomena Involved in Laser-Matter Interaction at High Intensities: Harmonic Generation, Self Focusing, Self Guiding, Absorption and Ionization. . . . . . . . . . . . . . . . . . . . . 54 3.1.1 Second Order Nonlinear Effects . . . . . . . . . . . . . . . . . 54 3.1.2 Third-Order Nonlinear Effects. . . . . . . . . . . . . . . . . . . 56 3.1.3 Photoionization . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 60 3.2 Experimental Methods for Analyzing the Main Phenomena Involved in Laser-Matter Interaction During PLA Below the Plasma Ignition Threshold: Reflectometry, Analysis of Thermal Radiation. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61 3.3 Theoretical Models for PLA Below the Plasma Ignition Threshold. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 65 3.3.1 Semi-Quantitative Analytical Models. . . . . . . . . . . . . . 67 3.3.2 Numerical Photo-Thermal Models for Short Laser Pulses . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 71 References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 74 4 Laser-Matter Interaction Above the Plasma Ignition Threshold Intensity . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 77 4.1 Main Phenomena Involved in Production of the Ablation Plasma and in Laser-Plasma Interaction During PLA: Plasma Formation and Evolution. . . . . . . . . . . . . . . . . . . . . . . 78 4.1.1 Plasma Heating, Self Focusing, Critical Density, Shielding . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 80 4.1.2 Ablation Plume Expansion . . . . . . . . . . . . . . . . . . . . . 82 4.1.3 Interaction of Plasma Plume with Obstacles . . . . . . . . . 93 4.2 Experimental Methods for Analyzing the Main Phenomena Involved in Laser-Plasma Interaction: Optical and Mass Spectroscopy, High Speed Imaging . . . . . . . . . . . . . . . . . . . . . 95 4.2.1 Interferometric Methods. . . . . . . . . . . . . . . . . . . . . . . 96 4.2.2 Thomson-Scattering. . . . . . . . . . . . . . . . . . . . . . . . . . 104 4.2.3 Spectrometric Methods. . . . . . . . . . . . . . . . . . . . . . . . 112 4.2.4 Laser Induce Fluorescence (LIF) Spectroscopy . . . . . . . 119 4.2.5 Mass Spectrometry (MS) . . . . . . . . . . . . . . . . . . . . . . 123 4.3 Theoretical Models for Plasma Mediated PLA . . . . . . . . . . . . . 129 4.3.1 Numerical Photo-Thermal Models. . . . . . . . . . . . . . . . 129 4.3.2 Numerical Photo-Thermal-Hydrodynamical Models for Plume Expansion and Material Removal. . . . . . . . . 136 References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 138

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