`FOR OBTAINING AND PROCESSING MATERIALS
`IN THE NUCLEAR FUEL CYCLE
`
`LN. Toumanov
`
`Nova Science Publishers, Inc.
`New York
`
`Energetiq Ex. 2045, page 1 - IPR2015-01300, IPR2015-01303
`
`
`
`-~--------------------------
`
`Senior Editors: Susan Boriotti and Donna Dennis
`Coordinating Editor: Tatiana Shohov
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`
`Library of Congress Cataloging-in-Publication Data
`Available Upon Request
`
`ISBN 1-59033-009-9
`
`Copyright© 2003 by Nova Science Publishers, Inc.
`400 Oser Ave, Suite 1600
`Hauppauge, New York 11788-3619
`Tele.: 631-231-7269
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`
`All rights reserved. No part of this book may be reproduced, stored in a retrieval system or transmitted in any
`form or by any means: electronic, electrostatic, magnetic, tape, mechanical photocopying, recording or otherwise
`without permission from the publishers.
`
`The authors and publisher have taken care in preparation of this book, but make no expressed or implied warranty
`of any kind and assume no responsibility for any errors or omissions. No liability is assumed for incidental or
`consequential damages in connection with or arising out of information contained in this book.
`
`This publication is designed to provide accurate and authoritative information with regard to the subject matter
`covered herein. It is sold with the clear understanding that the publisher is not engaged in rendering legal or any
`other professional services. If legal or any other expert assistance is required, the services of a competent person
`should be sought. FROM A DECLARATION OF PARTICIPANTS JOINTLY ADOPTED BY A COMMITTEE
`OF THE AMERICAN BAR ASSOCIATION AND A COMMITTEE OF PUBLISHERS.
`
`Printed in the United States of America
`
`Energetiq Ex. 2045, page 2 - IPR2015-01300, IPR2015-01303
`
`
`
`60
`
`LN. Toumanov
`
`P,kW
`
`1
`
`H
`¥~
`/II\
`
`r~~~~~~~~~~~~~~~--~-L--L-__
`ff)1 1lfl
`rtP
`· JC:J
`rtJ
`#13
`ro1 1tl1
`to
`:HJ mz
`flJ
`v----''~ -...._,_,...----' ~~---''-.;-----/
`Gz
`kGz
`MGz
`GGz
`TGz
`
`Fig. 2.38. Distribution of the frequency discharges n the frequency ranges of the electromagnetic spectra
`and the power levels to be specific for various discharges: 1 -transformer; 2 - high frequency inductive (HFI); 3
`- high frequency capacitive (HFC); 4 - ultra short- wave (USW); 5 - microwave (MW); 6 - spatial microwave
`(SMW); 7 - laser.
`
`2.12. OPTICAL DISCHARGES.
`
`For generation of the optical discharges energy is fed into the plasma with the use of a laser beam
`concentrated at any location of the volume isolated from the environment by the appropriate casing or
`without it /16/. The scheme of the experiment for excitation of an optical discharge is shown in Fig. 2.39.
`The discharge bums in the focal point or close to it if the energy flux is enough for it. As the energy source,
`laser was used generating radiation in the infrared range of the electromagnetic spectra. The
`a C02 -
`absorption coefficient of the light radiation in plasma falls abruptly with raising frequency. Therefore the
`generation of the optical discharge in the visible light frequency range would require a power greater than
`- 103
`that of C02 lasers by a factor of 102
`•
`
`Fig. 2.39. Scheme of the experiment for sustaining continuous optical discharge: the plasma cluster is
`shifted somewhat from the focal point towards the laser beam source.
`
`Energetiq Ex. 2045, page 3 - IPR2015-01300, IPR2015-01303
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