n the TQMS, several ionization methods can be employed. Some of these include electrospray ionization, chemical ionization, electron ionization, atmospheric pressure chemical ionization, and matrix-assisted laser desorption ionization, all of which produce a continuous supply of ions.
Both the first mass analyzer and the collision cell are continuously exposed to ions from the source, in a time independent manner.[4] It is once the ions move into the third mass analyzer that time dependence becomes a factor.[4] The first quadrupole mass filter, Q1, is the primary m/z selector after the sample leaves the ionization source. Any ions with mass-to-charge ratios other than the one selected for will not be allowed to infiltrate Q1. The collision cell, denoted as "q", is located between Q1 and Q3, is where fragmentation of the sample occurs in the presence of an inert gas like Ar, He, or N2. A characteristic daughter ion is produced as a result of the collisions of the inert gas with the analyte. Upon exiting the collision cell, the fragmented ions then travel onto the second quadrupole mass filter, Q3, where m/z selection can occur again.
Because the triple quadrupole is a scanning instrument, the type of detection system it employs must be capable of detecting ions one m/z at a time. One of the most common detectors, the electron multiplier, is often paired with the triple quadrupole. The electron multiplier allows for faster response time, increased sensitivity and higher gain. However, they have a limited lifetime due to overloading.[3] Employing the TQMS provides enhanced selectivity, better accuracy, and greater reproducibility; all of which are limited in single quadrupole mass analyzers.