The basicity of highly protonated cytochrome c (cyt c) and myoglobin (myo) ions were investigated using tandem mass spectrometry,i on-molecule reactions (IMRs), and theoretical calculations as af unction of charge state. Surprisingly,h ighly charged protein ions (HCPI) can readily protonate non-polar molecules and inert gases,i ncluding Ar, O 2 ,a nd N 2 in thermal IMRs.T he most HCPIs that can be observed are over 130 kJ mol À1 less basic than the least basic neutral organic molecules known( tetrafluoromethane and methane). Based on theoretical calculations,itispredicted that protonated cyt ca nd myo ions should spontaneously lose ap roton to vacuum for charge states in which every third residue is protonated. In this study,H CPIs are formed where every fourth residue on average is protonated. These results indicate that protein ions in higher charge states can be formed using al ow-pressure ion source to reduce proton-transfer reactions between protein ions and gases from the atmosphere.Electrospray ionization (ESI) is renowned for its ability to form intact, gaseous,m ultiply charged protein ions for rapid and sensitive detection by mass spectrometry. [1] However,the mechanism by which protein ions are formed in ESI is controversial and continues to be actively debated. Thet wo primary competing models to explain ion formation are known as the charge residue model (CRM) [2] and the ion evaporation model (IEM). [3] In both models,a sn eutral molecules evaporate from ac harged droplet, the electric field at the surface of the droplet increases,w hich initiates fission. [4] Such droplet fission events result in the emission of afine stream of smaller droplets that remove less than 1% of the mass but more than 30 %o ft he charge of the precursor droplet. [4,5] In the CRM, sequential droplet evaporation and Coulombic fission events yield acharged droplet that contains asingle analyte ion, which evaporates to dryness via the loss of neutral solvent molecules.Inthe IEM, the electric field on the surface of ah ighly charged droplet near the moment of ion formation is sufficient to result in the ejection of an analyte ion from the surface of the ionic droplet. Themajority of current evidence indicates that fully desolvated protein ions formed from buffered aqueous solutions are formed by the CRM. Charge carriers such as solvated hydronium ions can be lost via ion evaporation during the ESI process. [6] Recently,the chain-ejection model (CEM), [7] which is related to the IEM, was proposed to explain the formation of protein ions from denaturing solutions based on results from molecular dynamics simulations. [7] In the CEM, ad enatured, disordered protein chain is ejected from ah ighly charged, nanometer-sized ionic droplet. As the protein ion protrudes and is ejected from the droplet, proton transfer to the protein ion can occur. However,t he mechanism by which highly charged protein ions (HCPIs) are formed from denaturing solutions is less well established with evidence supporting both the CRM [8] and CEM/IEM having be...