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  2. 19 Apr 2006: 0]B]B@uxG-N+?3TQGH+?IA-oxGH=?xRU>A]B@M1-N==?G4/2L<@Mr;T2R2]t+;-N=B+?G4x143]B=.-N2_3T"G4/"=?3]B@M/U-0/,y14@ ... t+?36=?@MG4TU-01|-0/2Tx@M>36+.-N=B5;-N=B+?G4x143]T2R23!@)@5S/,?G4/2L0Õ@0z_3=B+?]B@0/i1HG4LMI,KTS=.-0LS9X@M>3a@MrP+?I23]B3!p0-
  3. doi:10.1016/j.cell.2006.10.032

    https://www2.mrc-lmb.cam.ac.uk/groups/hegde/download/43_Kang_SW_Cell_2006.pdf
    30 Nov 2006: B) Cells stably expressing PrP or Opn-PrP. were treated with 10 mM DTT for 24 hr, re-. ... B) HeLa cells treated with 10 mM DTT for the indicated times were pulse labeled (for 15 min), fractionated, and quantified to determine the glyco-.
  4. Particle Flow and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/ALCPG_Fermilab.pdf
    7 Dec 2006: Large detector – spatially separate particlesHigh B-field – separate charged/neutralsHigh granularity ECAL/HCAL – resolve particles. ... What is optimal detector size/B-field, etc. THIS IS HARD – BUT VERY IMPORTANT!
  5. The Structural Engineer Journal

    www-civ.eng.cam.ac.uk/cjb/papers/p56.pdf
    6 Jun 2006: ô“ ÎNóx‹ÿTñTy?W#B»Ûvíñ—ÍEíîïrúpžäø¿lD…Ÿ6[Q œ›6«S}öôˆ#{lx£ÎxQcPÃO{óÏZܘ ÌÊwx«/ÒÇÑ08$F‘ÍéÉñç-BÅ{ ... Í–ü
  6. EXPLICIT n-DESCENT ON ELLIPTIC CURVESI. ALGEBRA J.E. CREMONA, T.A. ...

    https://www.dpmms.cam.ac.uk/~taf1000/papers/n-descent-I.pdf
    13 May 2006: Then thereis an isomorphism of Brauer-Severi diagrams defined over K,. C //. φ. Pn1. ψ. E|n.0|. // Pn1. with σ(φ)φ1 = τξσ. We lift ψ to a matrix B ... It is evident that yσ =σ(B)B1 is an element of ΘE projecting onto ξσ.
  7. 19 Apr 2006: 35! Q ,!6 J 3$, $6"8 )0 4" 4 JLKNK 4 B)!B";1G0 83f("E"8,! ... 8g)! =)! Q83I -!>," $' $-"8<=1)6,,-<=2RQ ]/-!SQ TU! 1L,!N 2 5%>=B- B.
  8. Osman, A. S., Mair, R. J. & Bolton, M. ...

    www-civ.eng.cam.ac.uk/geotech_new/people/bolton/mdb_pub/176.pdf
    16 Nov 2006: Amsterdam: Elsevier. Clough, G. W. & Schmidt, B. (1981). Design and performance ofexcavations and tunnels in soft clay. ... Géotechnique 43, No.2, 315 – 320. Peck, R. B. (1969). Deep excavations and tunnelling in soft ground.Proc.
  9. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/AandG/notes.pdf
    11 Nov 2006: OC. (2.2). (ii) Addition is commutative, i.e.a b = b a. ... b 0 = b , and from (2.3) 0 b = b.
  10. 19 Apr 2006: ¢YKHz6VOzx{K.{{K!lzâZ}z]}¡!zC{B{B!6x$!z¢'! KzK!¡6 |6{K,.z{K.}z].{B6!x{#=!zVH{Kx/K6 ... K7K6},!{KHz66z6|z}¡!6H{K!}¡z/}zZh.B{K K}zC{K}¡xx{K!
  11. Families Intersecting on an Interval Paul A. Russell∗† October ...

    https://www.dpmms.cam.ac.uk/~par31/preprints/intersections.pdf
    10 Oct 2006: n}.How large can we make a family A of subsets of [n] subject to thecondition that for all A, A′ A, there is some B B with B A A′? ... n}.How large can we make a family A of subsets of [n] subject to thecondition that for all A, A′ A, there is some
  12. 1 Model-Based Hand Tracking Using a HierarchicalBayesian Filter…

    mi.eng.cam.ac.uk/reports/svr-ftp/thayananthan_pami06.pdf
    14 Sep 2006: The used costterm is thusI? £ F x Jt! #" tx Z £ «b«' Z BB aº B'B z»(17)where. ... I? " F B'B? s aò7µ F ÛóÌô4B'B. A partition of the state space is given by theVoronoi diagram defined by these nodes, seefigure 13a.ñ Partitioning the eigenspace
  13. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/NSTIB/notes.pdf
    28 Oct 2006: b) Suppose that B = 0; the vector field B(r) is said to be solenoidal. ... Then there exists anon-unique vector potential, A(r), such that. B = A.
  14. 27 Feb 2006: ngi{_bie|g?t}&X;phYXXq&ZY[X+]. u:/u&9qfYucwE9& :q&>j uc Efc;A :q&> uc 9&E U ... k&mnbi]n}ZY[X}&XlZ<X;h<{y_]nbi]pZZ<ggi¥&Zb?_]b?]b?eoZYXhY]nb?ZY_iXµt:gphY{eb?ZY_gi]vg?tZY[_wWt9bpEZA[nb?Z«}&gfXWqZY[_wWh<X+}&
  15. 8 Nov 2006: 4O:=<CKI@asgD6m{¡MO<>MK?b |7| IU6 J8;:U47L :@JMnMOD:@J¢{0:[ADIPM<=8;:ib |j b |g Sh,£?b | b |g SG[ADIPMub |7|; VT:iU6 J8;:U47L ... B64u<CKC º 1 jsgD6m{MO<>Mub |7|; U6 J8;:U47L :@I@G}<JDWWD:UMO:U47[tJD:nKMOIkCK[tKM@» t4O:=<ChJAD[aV :4ubvea¿>b b b d
  16. PII: 0012-821X(89)90063-0

    www.itg.cam.ac.uk/people/heh/Paper87.pdf
    27 Apr 2006: tems. In addition, crystals an d b u b b l es in m ag m as m a y b e distributed so t h at they create stable den- ... G. F. G i b b , C. M. B. H e n d e r s o n , C.
  17. 31 Jan 2006: O. é{ê_êcë¥ìë¢íî_ïðKñzò_óôìë¢íî_ôOO WZnWYXZY}YwXr|.qRqXERq}fYasd eYfvWYX> ][w >qWYXmO KKI|.0X}d efpcv ][w nKRaWhX}uowuqRqusoaZnÝ 4e|Yd ef_o{uY4Rx[w RqdQWs dexXr >XuRqvr_b.
  18. 30 May 2006: 8 ). ( 4. 8 b ). = 0 (n-reven), (4 8 c ) and Fnr = t w ' q s ,. , g , , r B B / ( b r - b n ). (,4.9). We again suppress the argument. ... 4.10 b ) N ( - )" 23(nw cosh [)-$ sin ( w cosh inn - &I-) sen(?).
  19. DYNAMIC RESOLUTION SELECTIONIN ULTRASONIC STRAIN IMAGING J. E.…

    mi.eng.cam.ac.uk/reports/svr-ftp/lindop_tr566.pdf
    29 Sep 2006: b) SNRe contours at 2.0% strain. 2.5 Dynamic Resolution Selection procedure. ... and uncoloured noise Simulation B-15dB white noise,. etc. mean SNR is appended.
  20. QUASIRANDOM GROUPS W. T. Gowers Abstract. Babai and Sos ...

    https://www.dpmms.cam.ac.uk/~wtg10/quasirandomgroups.pdf
    22 Oct 2006: Then there exist a A, b B and c C with ab = c.In particular, this is true if all of A, B and C have size greater than 2n8/9. ... Equivalently, there exist a A and b B suchthat ab = c, as claimed.
  21. Extremal Combinatorics I.B. Leader Michaelmas 2004 1 Isoperimetric…

    https://www.dpmms.cam.ac.uk/~par31/notes/extcomb.pdf
    16 May 2006: Write B for Bi(A). Then for the set-systems A and B, wehave |A| = |A||A+||A4A+| and |B| = |B||B+||B4B+|.Now, |B| |A| and |B+| |A+| (by the ... system B = Ak satisfies |B| = |A|, |B| |A| and Bi(B) = B forall i.
  22. D-Branes in Field Theory

    www.damtp.cam.ac.uk/user/tong/talks/cstring.pdf
    12 May 2006: trivially embed this in the non-abelian theory. B= B?0.( 0( ((q =q? ... B? q? SU(N)diag/SU(N 1) U(1) = CPN1. Simple Idea:. The strings can miss each other in the internal space.
  23. PII: 0377-0273(82)90062-2

    www.itg.cam.ac.uk/people/heh/Paper48.pdf
    27 Apr 2006: o c k e d b y r u b b l e a n d previous- ly c o o l e d lava. ... p a n d s t o f o r m t h e r u b b l y surface.
  24. Shocking, the slow changes inHKM’s thin coat by HKM2 ...

    www.damtp.cam.ac.uk/user/hinch/talks/hkm3.pdf
    23 May 2006: Secularity condition – resonant sin(θ τ ) and cos(θ τ ). d. dT. (. A. B. ). =. (. a b. b a. )(. ... A. B. ). where. a = 81α/(1 144α2) and b = 3(5 72α2)/2(1 144α2).
  25. doi:10.1016/j.diamond.2005.12.045

    www-g.eng.cam.ac.uk/nms/publications/pdf/Golovko_DRM2006.pdf
    13 Nov 2006: V.B. Golovko a,⁎, M. Cantoro b, S. Hofmann b, B. Kleinsorge b, J. ... Geng a, D. Jefferson a,A.C. Ferrari b, J. Robertson b, B.F.G.
  26. 15 Sep 2006: Finally (1) and (4) can be written. d r b 4/3 _,d t b b I b b - b •. Equations (8)-(l 1) describe the heat transfer and melting process ... a). 50 100. b). 100. c). 50 100. TIME (yrs). F I G.
  27. p6.dvi

    https://www.robinson.cam.ac.uk/iar1/teaching/p2apaper6_2006.pdf
    28 Nov 2006: limx. µx2 1. x 1ax b. = 0,. what should a and b be? ... c) Find a basis for Null(A) and Col(A). (d) Find a basis for the following set B = {b R4 | Ax = b has nosolution}.
  28. THE HIGHER SECANT VARIETIES OFAN ELLIPTIC NORMAL CURVE TOM ...

    https://www.dpmms.cam.ac.uk/~taf1000/papers/hsecenc.pdf
    1 Jun 2006: A A A (1 A) and A (1 A) =. (ii) |A| = min{|B| : A B (1 B)}.(iii) |A| = max{|B| : B A,B (1 B) = }. Proof: (i) We may assume ... B : B Z/nZ, |B| = r 1,B (1 B) = }. In particular I(SecrΓn) is generated by a space of (r 1)-ics of dimen-sion β(r 1,n).
  29. 19 Apr 2006: F! a! TS- '4( );V! (Y C( E5[- M(&? 3$ (49 P#-# -;9!9]%& W5[- ; ) Ea'-'; UG4?3$ )9&$ B ; B- t%3 ,:E# ;! 5- t(&$7C0:; P B 'RS! ... G. u= K G %' àõö>øEàù ú»s6ø 6þC.ø?»ý ø @2& B B- u 7:>- ra%. (&
  30. The same continued (4C). Th. 10 The same continued ...

    https://www.reporter.admin.cam.ac.uk/reporter/2006-07/special/01/pdfs/classics.pdf
    25 Sep 2006: 10. DR R. B. B. WARDYHellenistic and Roman Philosophy: knowledge. and fate (8L, weeks 1–4). ... 5–8). GROUP BCourse Directors:B1: Dr R. B. B. WardyB2: Prof. M.
  31. PII: S0022-0248(99)00456-X

    www.itg.cam.ac.uk/people/grae/42.pdf
    26 Apr 2006: where. B"B(j, hi)"! hi. Jpej2@4erf(j/2). (35). Eq. (34) is the transcendental equation determin-ing the eigenvalue j. ... Since gH is independent ofhiand B is expressed in closed form, we can calcu-.
  32. Phonon linewidths and electron-phonon coupling in graphite and…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Lazzeri_PRB2006.pdf
    13 Nov 2006: K. Swan, M. S. Ünlü, B. B. Goldberg, M. A. Pimenta, J. ... Dresselhaus, A. K. Swan, M. S. Ünlü, B. B. Goldberg, andR.
  33. Analysis II Example Sheet 2 Michaelmas 2006 MJW Corrections ...

    https://www.dpmms.cam.ac.uk/study/IB/AnalysisII/2006-2007/ex2.pdf
    27 Oct 2006: 0|f| a normed space? 3. Which of the following subsets of R2 are (a) open, (b) closed? ... Show that there exist disjoint closed subsets A, B of R (or R2 if you prefer) withd(A, B) = 0.
  34. 19 Apr 2006: #"%$$&' () ,.-.&/ 010 "%$$& 243 56 789 #:;,=<>;,@?" "'. A B!CEDGFIHKJ L=MNFPOQCSRTFIUVBWOTUVB!XYBZD[FM]T_TO BaDGFIBcbdUeJ fUgDh_ikjmlgDh_QCnB. ... Pea37fR$OaqPea4o4WdR$oBbBPeoq¢oqW)F,x;x'GF
  35. Science Magazine

    www-vendruscolo.ch.cam.ac.uk/vendruscolo06.pdf
    21 Dec 2006: B C. B. B. C. C. A. A. A. A free-energy channel model for enzymatic behavior. ... Kay, Science 312, 224 (2006). 6. K. Lindorff-Larsen, R. B. Best, M.
  36. Testing Equivalence of Ternary Cubics Tom Fisher University of ...

    https://www.dpmms.cam.ac.uk/~taf1000/papers/testeqtc.pdf
    12 Apr 2006: We nd σ(A) = sign(σ)A and σ(B) = B forall σ S3. ... The only non-trivial subgroups of 〈a,b〉, not containing I2, are the conjugatesof 〈b〉.
  37. Some remarks on the initiation of inertial Taylor columns

    www.itg.cam.ac.uk/people/heh/Paper19.pdf
    30 May 2006: I n the former case. g ( t , y ) (Bt1-l (B-,O), (3.22). ... For B B 1 l,he penetration depth f L / N is much less than the actual depth H , and the critical height varies inversely with B.
  38. 10 Feb 2006: bWam%a_WØ y ¡Ø ¡Ø Ü: | >b[É]i_5] amWYWO>f;_C]i_W;>_hMàFá(â%âµBãäC9â>ã. ... Ì w Ã>kâYi[aeW_]i>] _>f;_¥ghVdh_b y | >bi]i>] _%_:ªib_]i_W_ÖeY_biXZ_ p VbiYiX];Vdc_:e phxzy Ì#!
  39. N13LBa.dvi

    www.damtp.cam.ac.uk/user/rrh/notes/N13LBa.pdf
    22 May 2006: b) Multiplication by a scalar. Let A and B be n m matrices. ... Then by construction we clearly have. b (b c) =. i.
  40. IntroductionThe endosomal system functions as an internal…

    https://www2.mrc-lmb.cam.ac.uk/groups/hmm/publica/SNX2Cullen2005.pdf
    17 Jan 2006: 5A,B). Furthermore,there was a clear enrichment of endogenous SNX2 on SNX1. ... J. Cell Sci. 115, 3889-3900. Carlton, J. G., Bujny, M. V., Peter, B.
  41. NEW CONCEPTS FOR SPACECRAFT ANTENNAS AND RADAR STRUCTURESBASED ON ...

    www-civ.eng.cam.ac.uk/dsl/publications/New%20concepts.pdf
    17 Feb 2006: A. B. B. A. (a) Flat. (b) Deployed. Figure 2: Use of a shaped sheet A to shape sheet B into a singly-curved surface. ... The required reflective surface is obtained by replacing sheet B with a rectangular sheet, see.
  42. 30 May 2006: b P 2 b FIGURE 1. Finite obstacle in seini-infinite, stratified flow. ... The most interesting special cases are given by. A , = 4 h 2 ( A / 2 m ) ( l o g ( 4 h / b ) - 1}OO(b21og(h/b)} (b/hO) (A 7 ) and.
  43. SUB-SAMPLE INTERPOLATIONSTRATEGIES FOR SENSORLESSFREEHAND 3D…

    mi.eng.cam.ac.uk/reports/svr-ftp/housden_tr545.pdf
    13 Jan 2006: ldld. Bscan B. Bscan A. d = 0 d = 1ρ ρ= 0.85 = 0.80. ... even though the actual motionmight be considerable when accumulated over several hundred B-scans.
  44. 22 Nov 2006: This trans-. a: ε a: ε. b:b/0.5. c:c/0.3. a:a/0.2. 1 2. ... b4. a5. Fig. 2 An acceptor corresponding to the input sequence{a, a, b, a}.
  45. PII: S0925-9635(01)00642-2

    www-g.eng.cam.ac.uk/nms/publications/pdf/Beghi_DRM2002.pdf
    11 Dec 2006: M.G. Beghi , A.C. Ferrari , C.E. Bottani , A. Libassi , B.K. ... Tanner , K.B.K. Teo , J. Robertsona b, a a c b b.
  46. flm483.dvi

    www.itg.cam.ac.uk/people/heh/Paper186.pdf
    5 Jan 2006: ρs AH, φg =. mg. ρgAH, φl = 1 (φs φg), (1.1a, b, c). ... a) Ballotini in water, (b) KNO3 in solution,(c) KNO3 ballotini in solution.
  47. doi:10.1016/j.diamond.2003.12.018

    www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_DRM2004b.pdf
    27 Nov 2006: Gradowski , D. Schneider , H. Hilgersa a, a b b c b. ... 75(1999) 1077. w17x W.P. Acker, B. Yip, Dh. Leach, et al., J.
  48. PII: S0040-6090(02)00808-8

    www-g.eng.cam.ac.uk/nms/publications/pdf/Beghi_TSF2003.pdf
    28 Nov 2006: Bottani , A.C. Ferrari , J. Robertson , P. Milania, a a a b b c. ... 349. w5x A.C. Ferrari, A. Li Bassi, B.K. Tanner, V. Stolojan, J.
  49. No Job Name

    www-g.eng.cam.ac.uk/nms/publications/pdf/Cantoro_NL2006.pdf
    13 Nov 2006: K.; Rubloff, G. W.Phys. ReV. B. 1986, 33, 5517.(21) Holstein, W. ... K.; Unlu, M. S.; Goldberg, B. B.; Pimenta, M. A.; Hafner, J.
  50. THE ASTROPHYSICAL JOURNAL, 527 : 918È944, 1999 December 20The ...

    https://people.ast.cam.ac.uk/~wyatt/wdtf99.pdf
    19 Apr 2006: a@ a(1 [ b)/[1 [ 2b(1 ] e cos f )/(1 [ e2)] , (19). ... Of these large particles,only those with su†er no signiÐcant P-R drag evo-b b.
  51. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/NSTIB/Michaelmas/notes.pdf
    28 Oct 2006: b) Suppose that B = 0; the vector field B(r) is said to be solenoidal. ... Then there exists anon-unique vector potential, A(r), such that. B = A.

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