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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)

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. >?

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

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.

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).

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.

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.

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.

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.

12 Aug 2016: q1 =b‖b‖, 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).