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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.

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.

20 Dec 2014: 3672. 13. I. Steinbach, and M. Plapp: ‘Pearlite revisited’, Continuum Mechanicsand Thermodynamics, 2012, 24, 665–673. ... 24. R. S. Qin, A. Rahnama, W. J. Lu, and B.

20 Dec 2014: relationships [24]. The influence of ausforming condition on the block width ofmartensite for all the conditions is shown in Fig. ... 24. H. Kitahara, R. Ueji, N. Tsuji, and Y. Minamino: ‘Crystallographic fea-tures of lath martensite in low-carbon

14 Feb 2014: 24] J. A. Francis, M. Turski, P. J. Withers: Materials Science and Technology 25 (2009) 325–334. ... Metal-cored Ar2%CO2 18 1.0 24.7 250 23-36. Table 3: Pre-heat and inter-pass temperatures (TI).