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| 100 | 1 | _ | |a Antypas, Dionysios |0 0000-0002-5293-3799 |b 0 |
| 245 | _ | _ | |a Fast Apparent Oscillations of Fundamental Constants |
| 260 | _ | _ | |a Leipzig |c 2020 |b Wiley |
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| 700 | 1 | _ | |a Budker, Dmitry |0 P:(DE-HGF)0 |b 1 |e Corresponding author |
| 700 | 1 | _ | |a Flambaum, Victor V. |0 P:(DE-HGF)0 |b 2 |
| 700 | 1 | _ | |a Kozlov, Mikhail G. |0 P:(DE-HGF)0 |b 3 |
| 700 | 1 | _ | |a Perez, Gilad |0 P:(DE-HGF)0 |b 4 |
| 700 | 1 | _ | |a Ye, Jun |0 P:(DE-HGF)0 |b 5 |
| 773 | 1 | 8 | |a 10.1002/andp.201900566 |b Wiley |d 2020-04-01 |n 4 |p 1900566 |3 journal-article |2 Crossref |t Annalen der Physik |v 532 |y 2020 |x 0003-3804 |
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| 999 | C | 5 | |2 Crossref |u In general all varying fundamental “constants” must be properly described as dynamic scalar fields. Indeed a variation of “constants” leads to a change of energy of a system (e.g. an atom) which assuming energy conservation must be compensated by the energy taken up by the field. |
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| 999 | C | 5 | |2 Crossref |u The material of the cavity is generally important for precision measurements. The length of a crystalline cavity is conceptually connected to fundamental constants which is different from a cavity based on amorphous glass. However in the frequency range considered in this work for fast variations of fundamental constants the relatively slow creeps of the glass material should not make a significant contribution. |
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