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Eu,iu«it Trista Snyder; assistant rirehi Lim Jtanlwd raokktidn tswuns Ifitbcte john Kdo, Kim4«*(y Oflcr Atvr* rsi N{] hrectoh wdrld vkle Mb sues Bill Moran Pukkii i (science advertismggiaaas D igit wmwtii R-ck Bongiovanni. Rub In, Canrgtt Intitrtiatt at Ku Ancrwi C hniroph rr fi. WAllt Sidt E, h OTOtf t^l Vffrtry BOMO Of Rtflt MRC Etl Otf Juaiuu Ati FNln i h, Sftl Ibin/tul r,'* B. Cla vid Al Uhu Ltr, £'l-j-.i .‘m-hn-urr Attvtt- Mv*tir M«it LL WM* ls Bay, llm. The inset shows the mode shape from finite element simulation, l/ tmf is the voltage measured by the network analyzer, (C) Linear and nonlinear response of the device structure in mode 2.

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and observed by fluorescence mi'cnj Eccpy (40x roegnlficfftf EHni J, Visit oui Visit our website today and plan for tomorrowf Products for your research needs Fluorescent it Luminescent Reporters Gene Expression & Delivery Gene Expression Profiling Non-coding RNA Research fit RNAi Nucleic Add Purification Oligo Modification PCR & RT-PCR Products Protein Arrays Protein Expression & Purification Protein-Protein Interaction Systems Ludfan M expression in. By continually developing technology that can turn your scientific ideas into reality, we J fe bringing science to life and helping to transform drug discovery and healthcare. The extreme diversity in body size among purebred dogs is greater than lhai of any other mammalian species. irw el al A protein within the panicle (hat assembles mature m RNAs has both SNA and protein binding surfaces, and il achieves binding specificity by acting as a molecular ruler. 0-C MOM PVrltth Ubi t W Ht LM*M) pad jl m^mqku L DC ni aldil Kf\tf man'll w i Cnpyrtghl 0 MOT bf Ihtmcricjn fc MWJhtn toi Ihe hfrz Ktmml ri Sththc. and distributes to subscribers on a weekly basis journal abstracts aboul in Fluenza and other topics. SILVAN A 5ANIACHIARA BENERECETTi, 1 OR N ELLA 5EMINO, 1 HAMS JURGEN BANDELT,* ANTONIO TORRONI ]h ^ipartimenia d : l Generic* e Murobioltiqia, University di Pdvia. ^Department nf Biotechnology, College ol Science, University ol Baghdad, I rat]. Where- as synthetic catalysts are often site-spec i He Department al Chemftliy, University at California. *To whom correspondence Should be addressed, E-mail: [email protected](R. the United Stales (NASA), and Europe (European Space Agency! 1126/science, 1139672 include this infamation when citing this paper. The measurement of Coulomb drag in systems of parallel layers was first pro- posed in ( /, 2) and later realized in a number of experiments U -7) |for :i review, see (A) |, l 5chaot of Physics, Unimsily ol Exeter, 5t«ker «M(f, beier EX4 4Qi. J The Abdus UUm Interaartooal Cenlrt lor Tlwcretka L Physics, 5trada Cmtiefa 11. ii lias become a sensitive tool for their study in many problems of contempo- rary condensed-matter physics. Coulomb drag has been used in the search for Bose -condensation of interlayer cxctlons (9), the metal -insulator transition in 2D layers = N ,- J {h Tf l*L\ g V, i (Fig, 4), Tile variance is VOL 3 1 6 6 APRIL 2007 101 REPORTS calculated in ihe limits of both die diffbsive x v {solid line* Ttp K T) and hmlli-stic i v (dashed line, sc 7^ with , Vs I (J -a (id iiy of our explanation.

(Mc Donald Institute Monographs, Mc Donald in strtute Dor Archaeological Research, Cambridge, 2003), pp, W-lll. A total basal dislocation is thus considered to possess two alomic slip planes.

It is important to note that these two partial motions are not independent in our proposed model. move simulta- neously on adjacent l UOUl) basal planes to complete die perfect dislocation slip. Drg F mrecth: Marten d 2 ended; m iuun Way Ion Butler; rsiems shcuusi Andrew Uargo.:cusi BMn service luntvrscw Pal Sutler; ekcimhh Laurie Elaker, Tamara Alison, Karena Smith, Vicki lintdii, Latoya Gtsloc-l; circulation associate Christopher flehce, batr enthv su Mmiscw Cyntb-a Fohnsnn; sp«i ALisrs Tomcka Diggs, larrika Mil, Erin Laync Bush ess Opteiiiori ud Amnmttuehn o Mtcigv Deborah Britrj- Wcnhefd; ini Miis wisik Bandy 7i; itnti ruhnisi iultu Lisa Donbvan; wimti anrlut ft Sika Taccney; (■*M*L*B*w Tr( Mxb*L Le Bue, Farida Yc-atmin; wtim AUi SHUitsib K: w Hi Ketii Atu* Emilif David; asshmie ELizabrth Sandler; jnmieimc: rn Kiwi John Meyers; HMi Lri NL Mtuun Darryl Waller, Alison Pritchard; mmuhhu acsooutcs Juiiarnc Wie Jga, Mary Ellen Crowley, Catherne Fealherston, Alison Clunrtcr, Lauren Lamourein; mie rnmioral mmniiik hanmer W endy Stu rlc-v, marxctirs mcutive Jennifer Reeves; mrxe ri RC wvj HUt sehvkei EXKumi Linda Rusk; iahh sals Jason Ha nnalwd; urt license sales- mki« Tnqi (tyj^- sales ano cuttower hryxe TWian Ddisarri, Ki ks Forsytbe, Calberine Do Uand. The response has lorentzian Shape in the linear regime. Wendy Wise; be (Tronic me&ia mrm- roer Litaboth Harman: none? Asymmetric responses and hysteresis occur when Pj h** is greater than -60 d Bm (trace D). stacking is preserved after (he dislocation motion, the Q sublatticc can also preserve a perfect slacking sequence by an appropriate small modification in thc O atom positions. However, the devia- tions arc related to the positions of the Al atoms, neigh boring O, atoms and vaeanl sites sandwiched between (he O layers, Because the perfect A! (C) The passage of the second partial (AHerminated J slipping on an O plane, it is expected that (B) and (O occur simultaneously, and during the process, slight relaxation in the O plane in between the slip planes 1 and Z is required to preserve the perfect stacking sequence in 0 layers.

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