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[202a] K R Brown, D A Lidar, and K B Whaley, Quantum Computing with Quantum Dots on Quantum Linear Supports, Phys Rev A 65, 012397 (2001) [202b] X Peng, M C Schlamp, A V Kadavanich, and A P Alivisatos, Epitaxial Growth of Highly Luminescent CdSe/CdS Core/Shell Nanocrystals with Photostability and Electronic Accessibility J Am Chem Soc 119, 7019 (1997) [202c] D Katz, T Wizansky, O Millo, E Rothenberg, T Mokari, and U Banin, Size Dependent Tunneling and Optical Spectroscopy of CdSe Quantum Rods, Phys Rev Lett 89, 086801 (2002) [202d] Y A Wang, J J Li, H Chen, and X Peng, Stabilization of Inorganic Nanocrystals by Organic Dendrons, J Am Chem Soc 124, 2293 (2002) [203] D Lidke et al, Nature Biotechnol, Feb 2004 issue [204] N Kane, Advanced Diamond Technologies, Chicago, IL, wwwthindiamondcom [205] S-G Liu, J E Dahl, and R M K.

There are several types of edits that you can make on the working set of objects from the xref or block: If you change an object s properties, such as its layer, the object will have the new object property If you erase an object, the object is deleted from the xref or block If you draw a new object, the object is added to the xref or block An exception occurs if you create a new object by editing objects outside the working set For example, if you break a line (not in the working set) into two lines, then nothing is added to the working set You can transfer an object from the main drawing to the xref or block Select an object and choose Add to Working Set.

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Figure 9.16. The PANDIT database. (a) Portion of the alignment option for the thioredoxin family in PANDIT. (b) Portion of the phylogenic tree for the same family.

AN UNRELATED MOMENT OF PAUSE DENISE S PESTO CHICKEN PIZZA (continued)

Remember that the working set consists of objects from the xref or block, so if you add objects to the working set, they become part of the xref or block You can transfer an object from the xref or block to the main drawing Select an object and choose Remove from Working Set The working set consists of objects from the xref or block, so if you remove objects from the working set, they re no longer part of the xref or block; instead, they become part of your main drawing After you finish editing the working set, if you like what you did, choose Save Reference Edits from the Refedit toolbar Otherwise, choose Close Reference When you save changes to a block, block definitions are redefined and all instances of the block are regenerated according to the new definition.

Carlson, Diamondoid Derivatization Chemistry Towards Nanotechnology Application, 2004 NSTI Nanotechnology Conference and Trade Show, Nanotech 2004, Mar 7 11, 2004, Boston, MA [206] P M Ajayan, L S Schadler, and P V Braun, Nanocomposite Science and Technology, Wiley, Hoboken, NJ, 2003 [207] N A Kotov, Thin Film Nanocomposites: From Electronics and Photonics to Magnetic Materials and Tissue Engineering, Chemical Engineering, University of Michigan Department of Materials Science and Engineering, Ann Arbor, MI, msewww@umichedu [208] M Rieth and W Schommers, Ed, Handbook of Theoretical and Computational Nanotechnology, American Scienti c Publishers, Stevenson Ranch, CA [209] J-Y Lee and A J Crosby, Combinatorial Investigation of Crazing in Thin Film Nanocomposites, Polymer Poster Symposium, Crosby Research Group, Dept of Polymer Science and Engineering, University of Massachusetts, Amherst, MA, umassedu, http://wwwpseumassedu/crosby [210] A.

The parameter H can be expressed as H NQ Qd (l/zch) NQ (l/zd) (where NQ (Q/Qd)2, Q is the real divergence of the pumping beam, zd (kQQd)21 is the diffraction length of the speckled beam) Analysis of the dependence Gth(NQ) for xed (but different) values of the parameter (l/zd) showed that the condition (24) (for predominance of the phase conjugated beam over angular displacement scattering waves) is ful lled when the diffraction length of the speckled beam is comparable with the thickness of the nonlinear layer: (l/zd) ! 1 [29] This means that for the nonlinear layer with a mirror at the boundary, the mechanism for selection of the phase conjugate wave is caused both by the diffraction in the nonlinear layer and by the nonlinear ampli cation (similar to the ordinal backward SBS of a focused beam [5]).

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