Charge and frequency resolved isochronous mass spectrometry and the mass of 51 Co

Revolution frequency measurements of individual ions in storage rings require sophisticated timing detectors. One of common approaches for such detectors is the detection of secondary electrons released from a thin foil due to penetration of the stored ions. A new method based on the analysis of intensities of secondary electrons was developed which enables determination of the charge of each ion simultaneously with the measurement of its revolution frequency. Although the mass-over-charge ratios of 51 Co 27+ and 34 Ar 18+ ions are almost identical, and therefore, the ions cannot be resolved in a storage ring, by applying the new method the mass excess of the short-lived 51 Co is determined for the first time to be <math altimg="si1.gif" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">ME</mi></mrow><mo stretchy="false">(</mo><mmultiscripts><mrow><mi mathvariant="normal">Co</mi></mrow><mprescripts/><none/><mrow><mn>51</mn></mrow></mmultiscripts><mo stretchy="false">)</mo><mo>=</mo><mo>−</mo><mn>27</mn><mspace width="0.2em"/><mn>342</mn><mo stretchy="false">(</mo><mn>48</mn><mo stretchy="false">)</mo><mtext> keV</mtext></math> . Shell-model calculations in the fp -shell nuclei compared to the new data indicate the need to include isospin-nonconserving forces