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Lecture I 1 Lecture I: Collective Excitations: From Particles ...
www.tcm.phy.cam.ac.uk/~bds10/tp3/lectures.pdf10 Nov 2013: ka†k. )] O(N. 1/20 ). cf. quantum AF in spin-wave approximation. ... 2. (akak a. †ka†k. )]As with quantum AF, Ĥ diagonalised by Bogoluibov transformation:(. -
pgen.1003129 1..16
www.jiggins.gen.cam.ac.uk/pdfs/Richardson2012.pdf2 Jan 2013: Population Genomics of the Wolbachia Endosymbiont inDrosophila melanogasterMark F. Richardson1¤a, Lucy A. Weinert2, John J. Welch3, Raquel S. Linheiro1, Michael M. Magwire3¤b,. Francis M. Jiggins3, Casey M. Bergman1. 1 Faculty of Life Sciences, -
GRAVITY WAVE GENERATION BY VORTICAL FLOWS IN A ROTATING ...
www.damtp.cam.ac.uk/user/mem/papers/SSREPLY/rupert-ford-thesis93.pdf19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret -
flm563.dvi
www.damtp.cam.ac.uk/user/mem/papers/RECOIL/remote-recoil.pdf19 Oct 2013: Another importantwave activity measure is given by the pseudomomentum vector,. p = kA =h′ u′. ... Because of the ray-invariance of absolute frequency we have that |kA| = |kB | asympto-tically. -
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www.damtp.cam.ac.uk/user/mem/papers/LHCE/c1.pdf19 Oct 2013: #"$ %'&)(,.-0/$1#(23547684:9 ;8< = >?9A@B9DCFE7;8<G9IH 4KJ L59NM. OPRQST U U U U V W XY XY X X X XZ XY XY X. X XU XU. [#[T U U U U]_)]_)a.bc)_edXU XZ X X XZ X X XU XZ X f b)ghd. XZ X XZ X X Xi. [)jT U U U Uk]_l]DmBnoDdXi Xi XZ XU XZ X XU XZ XZ XZ X -
GRAVITY WAVE GENERATION BY VORTICAL FLOWS IN A ROTATING ...
www.damtp.cam.ac.uk/user/mem/oldftp/rupert-ford-thesis93.pdf19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret -
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www.damtp.cam.ac.uk/user/mem/oldftp/polarcool.pdf19 Oct 2013: ó ö ëLë BnF í öJLFLö-K ëlê D[F é KÁ@ òóí ø ê @pöFWK5î ð ø¥FWJö5ñ ê¥ò ø¥KpF ý ñ êÒëLê û#ø¥K¿ö-Dî ê Dù0JöJK5î[Jö-î ... ïí K5î ê F ê¥ò D ë F é öF@ ò D ú J ó K5îF é KÄ@pö ð ë K ëÁò ùbF é K -
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www.damtp.cam.ac.uk/user/mem/oldftp/airsea-negvisc.pdf19 Oct 2013: J<6{4)01# "9#mI =9? : : "9#r=:; DJzG=x? 0- I?6,z#1 Kj BKj'Kä :6#(8º Jz0 G= 8G? ... 6'? ] BKj0G=>=# Kj Km'Kä :#I =º? :;81#G5#6: º#=>c0- "GG "(8º J= G= 0G=º# Km Kj'EKà :#c X8Ñ? -
§4 FLOWS WITH A FREE SURFACE Such flows are ...
www.damtp.cam.ac.uk/user/mem/FLUIDS-IB/waves.pdf19 Oct 2013: iσζ̂ kA sinh kh = 0. and from the second (pressure) (). gζ̂ iσA cosh kh = 0. Regarding these as a system of two linear algebraic equations for the two unknown constants ζ̂ -
, 20120576, published 2 January 2013469 2013 Proc. R. ...
www.damtp.cam.ac.uk/user/md327/skyrmion_proc.pdf14 Aug 2013: Let K = Ka/xa, a = 0,. , 3 be a vector field generating a one-parameter group oftransformations of M with orbits Γ.
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