Lecture Notes in Physics

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XIV List of Contributors Victor Malka Laboratoire d’Optique Appliquèe ENSTA – CNRS UMR 7639 Ecole Polytechnique Chemin de la Hunière 91761 Palaiseau cedex France victor.malka@ensta.fr Paul McKenna Department of Physics University of Strathclyde Glasgow, G4 0NG Scotland, UK p.mckenna@phys.strath.ac.uk Charles Rhodes Laboratory for X-Ray Microimaging and Bioinformatics Department of Physics University of Illinois at Chicago Chicago, IL 60607-7059 USA rhodes@uic.edu Lynne Robson Department of Physics University of Strathclyde Glasgow, G4 0NG Scotland, UK l.robson@phys.strath.ac.uk Heinrich Schwoerer Institut für Optik und Quantenelektronik Friedrich-Schiller-Universität Max-Wien-Platz 1 07743 Jena Germany schwoerer@ioq.uni-jena.de Toshiyuki Shizuma Advanced Photon Research Center Kansai Research Establishment Japan Atomic Energy Research Institute 8-2 Umemidai, Kizu 619-0215 Kyoto Japan shizuma@popsvr.tokai.jaeri.go.jp Tomaž Žagar Jožef Stefan Institute Jamova 39 1000 Ljubljana Slovenia tomaz.zagar@ijs.si
1 The Nuclear Era of Laser Interactions: New Milestones in the History of Power Compression A.B. Borisov 1 ,X.Song 1 ,P.Zhang 1 ,Y.Dai 2 ,K.Boyer 1 ,and C.K. Rhodes 1,2,3,4 1 Laboratory for X-Ray Microimaging and Bioinformatics, Department of Physics, University of Illinois at Chicago, Chicago, IL 60607-7059 USA 2 Department of Bioengineering, University of Illinois at Chicago, Chicago, IL 60607-7052 USA 3 Department of Computer Science, University of Illinois at Chicago, Chicago, IL 60607-7042 USA 4 Department of Electrical and Computer Engineering, University of Illinois at Chicago, Chicago, IL 60607-7053, USA rhodes@uic.edu Abstract. A brief review of the history of power compression over a range encompassing approximately 40 orders of magnitude places laser–nuclear interactions roughly at the logarithmic midpoint of the scale at approximately 10 20 W/cm 3 .The historical picture also motivates four conclusions, specifically, that (1) foreseen developments in power compression will enable laser-induced coupling to all nuclei, (2) conventional physical mechanisms will encounter a limit of Ωα ∼ 10 30 − 10 31 W/cm 3 , a value approximately 10 10 above the presently demonstrated capability, (3) the key to reaching the Ωα limit is the generation of relativistic/chargedisplacement self-trapped channels with multikilovolt X-rays in high-Z solids, a concept named “photon staging,” and (4) penetration into the 10 30 − 10 40 W/cm 3 zone, the highest range known and the region represented by processes of elementary particle decay, will require an understanding of new physical processes that are presumably tied to phenomena at the Planck scale. 1.1 History of Power Compression The goal of achieving the coupling of laser radiation to nuclear systems has an extensive history, one that spans a range of approximately three decades. An excellent source of information on this history is the comprehensive landmark article [1] by Baldwin, Solem, and Gol’danskii entitled “Approaches to the Development of Gamma-Ray Lasers.” In light of the progress made during the 25 years since the publication of this important piece, it is now possible to foresee A.B. Borisov et al.: The Nuclear Era of Laser Interactions: New Milestones in the History of Power Compression, Lect. Notes Phys. 694, 3–6 (2006) www.springerlink.com c○ Springer-Verlag Berlin Heidelberg and European Communities 2006
Page 1 and 2: Lecture Notes in Physics Editorial
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Page 5 and 6: Preface The subject of this book is
Page 7 and 8: Contents Part I Fundamentals and Eq
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Nuclear Materials Detection 9 Laser
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Electron Laser NaI detector Number
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12 High-Power Laser Production of P
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Handbook of Chemistry and Physocs,
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