2016/01/14 by David Bresteau, Cyril Drag, Christophe Blondel · 2 citations
Materials Science · Chemistry · Physics and Astronomy · #Diamond and Carbon-based Materials Research #Mass Spectrometry Techniques and Applications #Advanced Chemical Physics Studies #Electron #Isotope #Atomic physics #Physics #Imaging phantom #Carbon fibers #Materials science #Nuclear physics #Optics
paper · doi:10.1103/physreva.93.013414
openalex publication_date 2016/01/14 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
The electron affinity of carbon is measured on a beam of C^\ensuremath- by photodetachment microscopy, with a precision increased by one order of magnitude with respect to the last measurement. Isotopes 12 and 13 are used in succession, which makes it possible to determine the isotope shift of the electron affinity of carbon. The obtained result, about \ensuremath-7.3(6)\phantom\rule0.16em0exm^\ensuremath-1, corroborates recent calculations of this shift. The electron affinities of 12C and 13C are 1\phantom\rule0.16em0ex017\phantom\rule0.16em0ex970.5(10) and 1\phantom\rule0.16em0ex017\phantom\rule0.16em0ex963.3(10)\phantom\rule0.16em0exm^\ensuremath-1, i.e., 1.262\phantom\rule0.16em0ex122\phantom\rule0.16em0ex6(11) and 1.262\phantom\rule0.16em0ex113\phantom\rule0.16em0ex6(12) eV, respectively.