“…Ad istribution of ions of different composition, mass and charge state is generated in the ion source region, typicallyb y way of electron impact ionization, laser vaporization, magnetron sputtering, or electrospray ionization. The beam containing ad istribution of ions of different masses and possibly charge states is transferred into the high vacuum chamber and guided into am ass filter.M ass-selected ions are accumulated in the cryogenically cooled ion trap, where they are thermalized closet oa mbient temperature by collisions with ab uffer gas, typicallyH eo rH 2 (D 2 )o ramixture thereof.T oday,i on trap temperatures of < 10 Kc an be routinelya chieved and < 4Kin state-of-the-art instruments, [34] but ion internal temperatures are typicallys lightly higher due to RF heatinga nd/or inefficient collisional cooling. [34,65] After thermalization and tagging, the ions are extracted from the ion trap, focused in time and space, irradiated with at unable IR laser pulse, mass-selected in as ubsequent mass filter,d etected, and the signals are electronically processed.…”