Fig. 4: Tandem mass spectra of [{Cr12Gd4} – Piv]+ at different collision energies and CCSN2 distributions of [{Cr12Gd4} – Piv]+ and fragment ions.
From: Formation and characterization of polymetallic {CrxMy} rings in vacuo
![Fig. 4: Tandem mass spectra of [{Cr12Gd4} – Piv]+ at different collision energies and CCSN2 distributions of [{Cr12Gd4} – Piv]+ and fragment ions.](http://media.springernature.com/full/springer-static/image/art%3A10.1038%2Fs44160-023-00383-7/MediaObjects/44160_2023_383_Fig4_HTML.png)
a, MS2 spectra of [{Cr12Gd4} – Piv]+ at collision energies of 0 eV, 210 eV and 250 eV. Occurring fragmentation pathways are labelled: (i) – [NH2n/iPr2]+, – Piv−; (iii) – [NH2n/iPr2]+, – F− and (v) – CrIII, – 3 Piv−. Satellite peaks (labelled with ‘s’) correspond to the labelled main peak via the exchange of one anionic ligand for another one (Piv− for F− or F− for Piv−; mass difference 82 Da). The spectrum at 210 eV shows two regions, one at lower m/z and one at higher m/z. Minor contaminant features were observed that were m/z-selected in the quadrupole along with [{Cr12Gd4} – Piv]+, and hence produce different fragments (labelled with ‘c’). b, CCSN2 distributions of [{Cr12Gd4} – Piv]+ (m/z = 4,688) and the fragment ions {Cr6Gd2} (m/z = 2,499) and {Cr5Gd2} (m/z = 1,940). Data were recorded at collision energies of 0 eV (precursor), 130 eV for {Cr6Gd2} and 190 eV for {Cr5Gd2}, respectively. Insets: schematics of {Cr12Gd4} and the two products {CrxGd2} (x = 5, 6; Cr, green; Gd, purple). Fragment ions that are assigned as closed, due to the ion mobility data, are presented schematically; as the IM–MS experiment informs on the stoichiometry but not on the exact connectivity between the metal centres.