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lecture:fine_structure_constant_at_cm21 [2020/12/09 07:16] – Ce Zhang | lecture:fine_structure_constant_at_cm21 [2021/06/04 07:23] (current) – Ce Zhang | ||
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- | ====== On determination of the fine-structure constant: Electron g-2 and Atom interferometers | + | ===== On determination of the fine-structure constant: Electron g-2 and Atom interferometers ===== |
Makiko Nio (RIKEN) | Makiko Nio (RIKEN) | ||
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Change in the SI, 2019 | Change in the SI, 2019 | ||
- | {{ :lecture:截屏2020-12-09_15.38.21.png? | + | {{ :lecture:201209: |
Old method: Quantum hall effect resistance R$_k$ --> no longer available | Old method: Quantum hall effect resistance R$_k$ --> no longer available | ||
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measure the h/M, then | measure the h/M, then | ||
- | {{ :lecture:截屏2020-12-09_15.59.35.png? | + | {{ :lecture:201209: |
R$_\infity$ puzzle --> does not matter | R$_\infity$ puzzle --> does not matter | ||
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Error sources: largest is the laser beam profile | Error sources: largest is the laser beam profile | ||
- | === electron g-2 === | + | ==== electron g-2 ==== |
Penning trap | Penning trap | ||
- | {{ :lecture:截屏2020-12-09_16.15.25.png? | + | {{ :lecture:201209: |
+ | ==== Be careful ==== | ||
+ | {{ : | ||
+ | should not be an issue for muon g-2, but it is for e g-2 | ||
+ | h/M may not be insensitive to new physics | ||
+ | **SHOULD study such effect on Mu 1S2S** | ||