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  1. Duke Casimir V of Pomerania (or, counting differently, Casimir VI; after 1380 – 13 April 1435) was a member of the House of Griffins and a Duke of Pomerania. He ruled in Pomerania-Stettin together with his brother Otto II from 1413 to 1428.

  2. For the Duke who reigned Pomerania-Stettin and lived c. 1380–1435, see Casimir V, Duke of Pomerania. Casimir VI (also known as Casimir IX; 22 March 1557 – 10 May 1605) was a member of the House of Griffin who ruled as Lutheran Administrator of the Prince-Bishopric of Cammin .

  3. Casimir II (also spelled Kasimir II) ( Polish: Kazimierz II pomorski) ( c. 1180 – 1219) was the duke of Pomerania-Demmin from 1187 until his death. He was succeeded by Wartislaw III, Casimir's son with princess Ingardis of Denmark .

  4. Duke Casimir V of Pomerania (or, counting differently, Casimir VI; after 1380 – 13 April 1435) was a member of the House of Griffins and a Duke of Pomerania. He ruled in Pomerania-Stettin together with his brother Otto II from 1413 to 1428. After 1428, he ruled Pomerania-Stettin alone.

  5. Dec 1, 2016 · 1. The dielectric-metal transition 1871 2. Casimir forces between a sphere and a plate with patterned geometry 1872 3. Pulsating Casimir force 1872 VI. Experiments on the Casimir-Polder Force 1873 A. Demonstration of the thermal Casimir-Polder force 1873 1. The force in thermal equilibrium 1873 2. The force out of thermal equilibrium 1874

  6. Kazimierz III the Great by Jan Matejko. Casimir III, called the Great (Polish: Kazimierz Wielki; 1310 – 1370), King of Poland (1333-70), was the son of King Władysław I the Elbow-high and Jadwiga of Gniezno and Greater Poland. Casimir III is the only Polish King who has been honored with the title 'Great', awarded less for military exploits ...

  7. Oct 1, 2001 · 1.. IntroductionMore than 50 years have passed since H.B.G. Casimir published his famous paper [1] where he found a simple yet profound explanation for the retarded van der Waals interaction (which was described by him along with D. Polder [2] only a short time before) as a manifestation of the zero-point energy of a quantized field.

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