An alternative to resonant excitation collision-induced signal enhancement (CISE) is presented. This alternative utilizes boundary activation instead of resonant excitation to effect CISE and is called boundary activated collision induced signal enhancement (BA-CISE). There are three ways to effect BA-CISE to enhance the signal for an MS nϩ1 experiment. Each technique utilizes the  z ϭ 0 boundary, which ions encounter from high to low mass/charge ratio. BA-CISE is shown to produce an almost 900% increase in the C 2 ion of [maltohexaose ϩ Li] ϩ . The use of a heavy collision gas in addition to the helium bath gas generally produced a signal enhancement inferior to the same experiment without the heavy gas. (J Am Soc Mass Spectrom 2002, 13, 650 -658) © 2002 American Society for Mass Spectrometry C ollision-induced signal enhancement (CISE) is a process whereby the abundance of a second generation, or higher, parent ion for an MS n experiment is increased. The signal increase occurs via two stages of excitation and subsequent dissociation of ions of higher mass/charge ratio than the next generation parent ion. The first stage of excitation/dissociation is of the n-1 generation parent ion and the second stage of excitation/dissociation is of the n-1 generation product ions of higher mass/charge ratio than the n generation parent ion. The viability of CISE as an effective technique depends on the existence of dissociation pathways from ions present in a product ion spectrum to the next generation parent ion. CISE through the use of single frequency and broadband waveform resonance excitation has been reported previously [1]. Another method to increase the kinetic energy of ions and effect dissociation to perform CISE in a quadrupole ion trap is explored in this work.Boundary activation via the manipulation of a z values has been previously investigated and characterized [2][3][4][5][6] and is the method evaluated here. a z is a parameter of the Mathieu second-order differential equations of motions of ions in a quadrupole ion trap. It is defined in equation 1 a z ϭ Ϫ16eUwhere (m) is the mass of the ion, (e) is the electronic charge, (r 0 ) and (z 0 ) are the radial and axial ion trap dimensions, respectively, (⍀) is the ac radial frequency of the trapping voltage, and (U) is the dc voltage amplitude. Since r o , z o , and ⍀ are constants of a given quadrupole ion trap, for a given mass/charge ratio, the a z value is only dependent upon the dc voltage. The other parameter in the Mathieu equations is q z and it is defined in equation 2.