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81	120 S. Constantinescu G Fig. 10 – Calculated values of the electric potential and 57Fe quadrupole splitting parameter for different δr around cationic sites, δr = 0.001A; ∆θ = 18°; ∆ϕ = 36°. The sign of the q Add to Reading List Source URL: www.rrp.infim.ro - Date: 2015-10-22 07:29:45
82	Typical Approximation Factors Approximation Factor 1 + 𝜀𝜀 Θ(1) Θ(log ∗ 𝑛𝑛) Add to Reading List Source URL: courses.csail.mit.edu Language: English - Date: 2014-10-07 17:29:11
83	JOIN∬ αs α θ bθr “ ι■ θnJy9 “ (Wο “ Add to Reading List Source URL: kyofukai.jp Language: English - Date: 2015-12-30 08:23:08
84	1. − π ≦ θ ≦ π で定義された関数 2 2 √ Add to Reading List Source URL: www.mathtext.info Language: Japanese - Date: 2015-02-28 14:56:37
85	1 FIG. 1: A schematic diagram of the shock wave emanating from an overhead airplane. The angle θ is the angle between the blue line of flight, and the sides of the expanding cone. (figure taken from http : //mistere9.b Add to Reading List Source URL: www.cmp.caltech.edu Language: English - Date: 2009-10-26 17:33:29
86	Math 416 Complex variables Solutions to Problem Set 6 1. Let C be the positively oriented circle \|z\| = 1, with parametric representation z = eiθ (0 ≤ θ ≤ 2π). and let m and n be integers. Then Z Add to Reading List Source URL: www.math.wustl.edu Language: English
87	テクニカルガイド 480 Θ1=X/S1, Θ=X/S2 = (x/s1)(y1/y2) Add to Reading List Source URL: www.newport-japan.jp Language: Japanese - Date: 2014-11-09 20:30:49
88	Fachbereich Mathematik und Statistik µ ϑ Add to Reading List Source URL: www.math.uni-konstanz.de Language: German - Date: 2008-10-18 01:02:55
89	SMOOTH CHARACTER VARIETIES FOR TORUS KNOT GROUPS JAN ADRIAENSSENS, RAF BOCKLANDT, AND GEERT VAN DE WEYER Abstract. Semisimple representations of the free product Zp ∗ Zq determine θ-semistable representations of a spe Add to Reading List Source URL: www.mas.ncl.ac.uk Language: English - Date: 2010-11-04 06:06:36
90	(1)10人のグループを,5人,5人のグループに分ける方法は何通りありますか: θ C/ブしヽ C多 Add to Reading List Source URL: www.mathtext.info - Date: 2014-01-16 14:01:57

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