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10:5010:50, 28 May 2024 diff hist −1‎ Zeldovich–Liñán model ‎No edit summary current
10:5010:50, 28 May 2024 diff hist +16‎ Zeldovich–Liñán model ‎No edit summary
10:1210:12, 28 May 2024 diff hist +184‎ Zeldovich–Liñán model ‎No edit summary
10:1010:10, 28 May 2024 diff hist −27‎ John W. Dold ‎No edit summary current
10:1010:10, 28 May 2024 diff hist +39‎ N Zeldovich–Liñán–Dold model ‎ ←Redirected page to Zeldovich–Liñán model current Tag: New redirect
10:0810:08, 28 May 2024 diff hist +45‎ Zeldovich mechanism ‎No edit summary current
10:0710:07, 28 May 2024 diff hist +1,835‎ Zeldovich–Liñán model ‎No edit summary

21:2521:25, 27 May 2024 diff hist +1‎ Zeldovich–Liñán model ‎No edit summary
21:0321:03, 27 May 2024 diff hist +644‎ Zeldovich–Liñán model ‎No edit summary
20:5420:54, 27 May 2024 diff hist −6‎ Zeldovich–Liñán model ‎No edit summary
20:5320:53, 27 May 2024 diff hist −6‎ Zeldovich–Liñán model ‎No edit summary
20:5220:52, 27 May 2024 diff hist +18‎ Zeldovich–Liñán model ‎No edit summary
20:5120:51, 27 May 2024 diff hist −5‎ Zeldovich–Liñán model ‎No edit summary
20:5020:50, 27 May 2024 diff hist +68‎ John W. Dold ‎No edit summary
20:4920:49, 27 May 2024 diff hist +1,298‎ Zeldovich–Liñán model ‎No edit summary
20:0620:06, 27 May 2024 diff hist +89‎ Sign convention ‎No edit summary current
10:1710:17, 27 May 2024 diff hist +4‎ Biaxial nematic ‎No edit summary current
10:1310:13, 27 May 2024 diff hist −3‎ Q tensor ‎No edit summary
10:1210:12, 27 May 2024 diff hist +444‎ Q tensor ‎No edit summary
10:0510:05, 27 May 2024 diff hist 0‎ Q tensor ‎No edit summary
10:0310:03, 27 May 2024 diff hist −1‎ Q tensor ‎No edit summary
10:0310:03, 27 May 2024 diff hist 0‎ Biaxial nematic ‎No edit summary
10:0110:01, 27 May 2024 diff hist +1,885‎ Q tensor ‎No edit summary

13:4813:48, 25 May 2024 diff hist +15‎ Pierre-Gilles de Gennes ‎No edit summary current
13:4413:44, 25 May 2024 diff hist +1,607‎ Pierre-Gilles de Gennes ‎No edit summary
13:1513:15, 25 May 2024 diff hist 0‎ Landau–de Gennes theory ‎No edit summary current
13:1413:14, 25 May 2024 diff hist +1‎ Q tensor ‎No edit summary
13:1413:14, 25 May 2024 diff hist 0‎ Landau–de Gennes theory ‎No edit summary
13:1113:11, 25 May 2024 diff hist 0‎ Landau–de Gennes theory ‎No edit summary
13:1113:11, 25 May 2024 diff hist +21‎ Landau–de Gennes theory ‎No edit summary
13:1013:10, 25 May 2024 diff hist +24‎ Landau–de Gennes theory ‎No edit summary
13:0813:08, 25 May 2024 diff hist 0‎ Landau–de Gennes theory ‎No edit summary
13:0813:08, 25 May 2024 diff hist +179‎ Landau–de Gennes theory ‎No edit summary

20:5120:51, 24 May 2024 diff hist +7‎ Q tensor ‎No edit summary
16:1216:12, 24 May 2024 diff hist −1‎ Q tensor ‎No edit summary
16:1116:11, 24 May 2024 diff hist +3‎ Liquid crystal ‎No edit summary current
16:0916:09, 24 May 2024 diff hist +36‎ Biaxial nematic ‎No edit summary
11:3711:37, 24 May 2024 diff hist +31‎ Pierre-Gilles de Gennes ‎No edit summary
11:2811:28, 24 May 2024 diff hist +40‎ Pierre-Gilles de Gennes ‎No edit summary
11:2611:26, 24 May 2024 diff hist +34‎ Pierre-Gilles de Gennes ‎No edit summary
11:2111:21, 24 May 2024 diff hist +102‎ Pierre-Gilles de Gennes ‎No edit summary
11:1311:13, 24 May 2024 diff hist +31‎ Landau theory ‎No edit summary current
11:1211:12, 24 May 2024 diff hist +45‎ Q tensor ‎No edit summary
11:0911:09, 24 May 2024 diff hist +2,951‎ N Landau–de Gennes theory ‎ ←Created page with ''''Landau–de Gennes theory''' describes the NI transition, i.e., phase transition between nematic liquid crystals and iostropic liquids, which is based on the classical Landau's theory and was developed by Pierre-Gilles de Gennes in 1969.<ref>De Gennes, P. G. (1969). Phenomenology of short-range-order effects in the isotropic phase of nematic materials. Physics Letters A , 30 (8), 454-455.</ref> The phenomonologivcal theory uses...'
10:4610:46, 24 May 2024 diff hist +1,482‎ N Q tensor ‎ ←Created page with ''''<math>\mathbf Q</math> tensor''' is an oreintational order parameter that describes uniaxial and biaxial nematic liquid crystals and vasnishes in the isotropic phase.<ref>De Gennes, P. G. (1969). Phenomenology of short-range-order effects in the isotropic phase of nematic materials. Physics Letters A , 30 (8), 454-455.</ref> The <math>\mathbf Q</math> tensor is a second-order, traceless, symmetric tensor and is defined by<ref>De Gennes, P. G., &...'
09:5309:53, 24 May 2024 diff hist +4‎ Pierre-Gilles de Gennes ‎No edit summary
09:5309:53, 24 May 2024 diff hist +1‎ Pierre-Gilles de Gennes ‎No edit summary
09:5209:52, 24 May 2024 diff hist −37‎ Pierre-Gilles de Gennes ‎No edit summary
09:5209:52, 24 May 2024 diff hist +68‎ Pierre-Gilles de Gennes ‎No edit summary

15:1615:16, 23 May 2024 diff hist +149‎ Pierre-Gilles de Gennes ‎No edit summary

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