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3 3.1 R r r + R R r Rr [ ] ˆn(r) = ˆn(r + R) (3.1) R R = r ˆn(r) = ˆn(0) r 0 R = r C nn (r, r ) = C nn (r + R, r + R) = C nn (r r, 0) (3.2) ( 2.2 ) C

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シェア "3 3.1 R r r + R R r Rr [ ] ˆn(r) = ˆn(r + R) (3.1) R R = r ˆn(r) = ˆn(0) r 0 R = r C nn (r, r ) = C nn (r + R, r + R) = C nn (r r, 0) (3.2) ( 2.2 ) C"

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図 3.4: Alder 転移の固液共存状態 (B. J. Alder and T. E. Wainwright, ‘Phase transition in elastic disks’, Phys
図 3.5: 逆格子の基底ベクトルのとりかたは一意的ではない． ということである． [ 逆格子] 結晶の並進ベクトル T に対し，波数空間で e i G · T = 1 (3.18) となる G は波数空間での格子点をなす．この格子を逆格子 (reciprocal lattice) と呼 ぶ．波数空間で逆格子基本ベクトルを b 1 = 2π a 2 × a 3 a 1 · (a 2 × a 3 ) , b 2 = 2π a 3 × a 1a2· (a3 × a 1 ) , b 3 = 2π a 1 × a
図 3.7: フラクタル図形．(a) 拡大と縮小による二つの作り方，(b) Sierpinski のガス ケット (T. Vicsek, Fractal Growth Phenomena, (World Scientific, Singapore, 1992) より ) ，
図 3.8: 2 次元的銀樹と格子気体からの凝集体左側は硝酸銀水溶液から銅板への銀の 金属葉の析出．溶質濃度は (a) 0.04 mol/ℓ, (b) 0.06 mol/ℓ．右側は格子気体からの固
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