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21 Nov 2014: 1" > </div> <div class="sg" id="s54" data-sgid="Picture 72" style="z-index:25;left:174.76px;top:187.45px;width:15.95px;height:24.81px"> <img class="sg" ... 73AAA3D7.png" id="s54_i" style="z-index:1;left:0px;top:0px;width:15.95px;height:24.81px" > </div>

19 Nov 2014: alt="TP_tmp.png" style="z-index:1;left:0px;top:0px;width:610.48px;height:20.85px" > </div> <div class="sg" id="s30" data-sgid="Picture 24" ... s52_i" title="" alt="TP_tmp.png" style="z-index:1;left:0px;top:0px;width:126.80px;height:20.87px" > </div> <div

18 Nov 2014: width:286.66px;height:31.20px" > </div> <div class="sg" id="s54" data-sgid="Picture 33" ... top:506.17px;width:537.68px;height:24.83px"> <img class="sg" src="5EA7B95C.png" id="s47_i" title="" alt="x3.pdf"

15 Nov 2014: 0px;width:35.72px;height:24.92px" > </div> <div class="sg" id="s43" data-sgid="Picture 72" ... Picture 87" style="z-index:24;left:254.02px;top:367.31px;width:247.82px;height:25.55px"> <img class="sg" src="B1ABE4BD.png" id="s50_i" title=""

15 Nov 2014: 46.76px" > </div> <div class="sg" id="s17" data-sgid="Rectangle 24" style="z-index:5;left:63.46px;top:282.31px;width:638.56px;height:46.88px" data-fillcolor="16777215"> ... width:360.28px;height:28.07px" > </div> <div class="sg" id="s53"

28 Nov 2014: div class="sg" id="s18" data-sgid="Picture 59" style="z-index:6;left:44.62px;top:191.64px;width:24.96px;height:28.30px"> <img class="sg" src="AF7AD254.png" ... 44px"> <img class="sg" src="AC8C2369.png" id="s119_i" title="" alt="TP_tmp.png"

15 Nov 2014: id="s33_i" style="z-index:1;left:0px;top:0px;width:145.84px;height:295.70px" > </div> <div class="sg" id="s29" data-sgid="Rectangle 24" ... data-sgid="Picture 24" style="z-index:7;left:305.35px;top:129.87px;width:390.17px;height:299.92px"> <img class="sg"

10 Dec 2014: 24) for allfive system sizes shown in Table II and also in Fig. ... Data derived from (24) are shown for systems of N particles at n unitsof flux above the ground state Nφ = N 2 n.

15 Mar 2014: Edge Singularity in X-ray Absorption in Metals. 24. Non-equilibrium Superconductivity. 25.

11 Jul 2014: BOOKS. MOVIES. PAINTINGS. 1. A man without qualities. Journey to the end of the night. Les Particules élémentaires. Very little. almost nothing. That palm at the end of the mind. The Passion of Joan of Arc. Japanese girls at the harbour. Der

24 Feb 2014: 0. 5. 10. 15. 20. 25. 18 20 22 24 26 28 30 32 34 36 38.

29 Nov 2014: 24. 6.5 Example: prospecting. 25. 7 Bandit Processes and the Gittins Index 26.

7 Apr 2014: 8.97 5.5 9.05 5.6 9.23 5.9 9.24 5.8 9.24 6.1 9.61 6.3 9.60 6.4 9.61 ... 38.15 9.65 NA rolling tobacco 24 X 440 cans Stella Artois 11.95 20.80 23.96 9.25 9.67 24 X 440 cans Guinness 15.75

20 Jan 2014: hour dodging stray bullets, until I got back to safety.This sort of thing occurs frequently, at first it was uncanny, now I am used toit.24.5.15 Have just

17 Mar 2014: 314 32 185 44 91 21 52 17. 556 24 158 38 140 20 72 15. ... parameters for 24 observations) so that weexpect to get deviance 0 with df = 0.

26 Jan 2014: Random Surfaces and Quantum Loewner Evolution. Jason Miller and Scott Sheffield. Massachusetts Institute of Technology. January 23, 2014. Jason Miller and Scott Sheffield (MIT) Random Surfaces and QLE January 23, 2014 1 / 30. Overview. Part I:

1 Oct 2014: Liouville Quantum Gravity as a Mating of Trees. Bertrand Duplantier, Jason Miller, and Scott Sheffield. CEA/Saclay and Massachusetts Institute of Technology. September 30, 2014. Duplantier, Miller, Sheffield Liouville Quantum Gravity as a Mating of

7 Oct 2014: In the limit as 0, we obtain2 the critical space–time percolation process onZ R, see Figure 5.1 and, for example, [24].

13 Jun 2014: Ui′(λi) yi(λ) < 0 (23). U′i(y(λ)) λi > 0 (24). yi(λ)λi. ... Notice the inequality (24), which is satisfied at λi = 0,cannot be sustained for all λi since U′i(y(λ)) is a decreasing function of λi.

14 Aug 2014: However, H o u c k [24] has shown via simulation that it is close to being optimal in m a n y cases.