Separated oscillatory-field microwave measurement of the fine-structure interval of atomic helium
The 2 P 3 1–2 P 3 2 interval in helium is measured using microwave separated oscillatory
fields. Our measured result is 2 291 177.53±0.35 kHz. A disagreement with theory of over 15 …
fields. Our measured result is 2 291 177.53±0.35 kHz. A disagreement with theory of over 15 …
[PDF][PDF] Separated oscillatory-field microwave measurement of the 2 3 P1–2 3 P2 fine-structure interval of atomic helium
JS Borbely, MC George… - … REVIEW A Phys …, 2009 - doylegroup.harvard.edu
The 2 3P1–2 3P2 interval in helium is measured using microwave separated oscillatory
fields. Our measured result is 2 291 177.530. 35 kHz. A disagreement with theory of over 15 …
fields. Our measured result is 2 291 177.530. 35 kHz. A disagreement with theory of over 15 …
Separated oscillatory-field microwave measurement of the 2P31-2P32 fine-structure interval of atomic helium
JS Borbely, MC George, LD Lombardi… - Physical …, 2009 - ui.adsabs.harvard.edu
Abstract The 2P3 1-2P3 2 interval in helium is measured using microwave separated
oscillatory fields. Our measured result is 2291177.53±0.35 kHz. A disagreement with theory …
oscillatory fields. Our measured result is 2291177.53±0.35 kHz. A disagreement with theory …