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  2. 3A1b.dvi

    www.damtp.cam.ac.uk/user/gio10/3A1b.pdf
    24 Oct 2016: Equilibrium of a magnetic star. A star contains an axisymmetric and purely toroidal magnetic field B = B(r, z) eφ, where(r, φ, z) are cylindrical polar coordinates. ... B = B(r, z) eφ ,. where (r, φ, z) are cylindrical polar coordinates and B(r, z)
  3. 12 Aug 2016: I, @# u! D)pJQ : 3B )@;JQu6&}7P g 7. )vJQu6&( _b P.;&( I)))! ... 2) / v{)P 8<b(J I? )o+- )@ bwZu 7 Ip >?(oRuPVR:]u. >?
  4. The Quantum Hall Effect Trinity Mathematical Society, October 2016 ...

    www.damtp.cam.ac.uk/user/tong/talks/quantumhall.pdf
    11 Oct 2016: 8. µAµ@A. x =v! cos!t. y = v! sin!t. mẍ = eẋ B! ... 1! B! B 1! (1.8). The o-diagonal components of the resistivity tensor, xy =! B/DC, have a couple. of rather nice properties. First, they are independent of the scattering
  5. 25 Microscopic Theory of Bose-Einstein Condensationof Magnons at Room …

    www.damtp.cam.ac.uk/user/ngb23/publications/Ch_25_Demokritov.pdf
    12 Jul 2016: 2Q v. 2Q). Expressions for A and B were obtained in [15], C (correct-. ... 10] Berloff, N. G. and Svistunov, B. V. Scenario of strongly nonequilibrated BoseEinstein condensation.
  6. Tidal excitation of hydromagnetic waves and their damping in the Earth

    www.damtp.cam.ac.uk/user/rrk26/Papers/Tidal94.pdf
    12 Aug 2016: iAb- V b ) B = p( Y b , (3: 9,) Y a ) A. ... A = A , e(a-i[l-yl) t , B = B, e(ai[l-yl) t (2.43).
  7. Slender-ribbon theory

    www.damtp.cam.ac.uk/user/lauga/papers/115.pdf
    25 Feb 2016: we have denoted b b/, a a/ and R0 r(s1) r(t1). ... small parameters and then asymptotically matched. In the case of a ribbon, two small parameters arepresent, namely, b/ = b and a/ = a.
  8. Small acoustically forced symmetric bodies in viscous fluids

    www.damtp.cam.ac.uk/user/lauga/papers/117.pdf
    4 Mar 2016: problem.23–25 As shown in Appendix B in the case of sym-. ... b3 þ O 5ð Þ; (43). Im Cs 1 þ 29ffiffiffi2p b 1.
  9. on September 22,…

    www.damtp.cam.ac.uk/user/gold/pdfs/silicachoano_jrsi.pdf
    22 Sep 2016: a) Diaphanoeca grandis cell grown in þGe ASW. (b) Stephanoeca diplocostatacell grown in þGe ASW. ... A. A B. B. 1.63. 9 Å. 1.639 Å. 1.631 Å.
  10. mssmRge.eps

    www.damtp.cam.ac.uk/user/examples/3P7.pdf
    8 Mar 2016: F |B〉 = |B〉 , ()F |F〉 = |F〉. This new operator ()F anticommutes with Qα since. ... multiplet there are states of different spin). 2.4.4 Parity. Parity interchanges (A, B) (B, A), i.e.
  11. doi:

    www.damtp.cam.ac.uk/user/rrk26/Papers/CK13.pdf
    12 Aug 2016: q1 =bb‖, q̃i1 =Aqi. ij=1. qjqTj Aqi‖qj‖2. qi1 = q̃i1/‖q̃i1‖ i 1. , ... The iterations are continued until. ‖AδXn b‖‖b‖ =. ‖Dzn pn1‖‖pn1‖. = | pn1(n 1)|‖pn1‖6 tol (3.20).
  12. This isa spec ific indiv idual’s copy of the ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/VandM/notes.pdf
    6 Nov 2016: A. A.3 Basic Maps. B. A.4 The General Möbius Map. C. ... ii) A complex number 0 i.b is said to be pure imaginary.
  13. Colloid Transport by Interfacial Forces

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/AndersonARFM.pdf
    2 Oct 2016: b. B( 41t'l. kT -KL. fJ. kT 2 [' 2 Jb 4 -;] K- 2 ,B-ln (I-e) 2 roo. ... Values of b that were derived in the previous section are listed in Table 1.

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