Ultraviolet photodissociation of peptides followed by mass analysis has several desirable advantages relative to other methods, yet it has not found widespread use due to several limitations. One shortcoming is the inefficiency with which peptides absorb in the ultraviolet. This issue has a simple solution and can be circumvented by the attachment of noncovalent adducts that contain appropriate chromophores. Subsequent photoactivation of the chromophore leads to vibrational excitation of the complex and eventually to fragmentation of the peptide. Herein, the energetics that control the efficiency of this process are examined as a function of the characteristics of both the peptide and the noncovalently attached chromophore. Fragmentation efficiency decreases with increasing peptide size and is also constrained by the binding energy of the noncovalent adduct. The optimum chromophore should have excellent absorption at the excitation wavelength and a low luminescence quantum yield. It is demonstrated that a naphthyl based 18-crown-6 adduct is ideally suited for attaching to a variety peptides and fragmenting them following absorption of 266 nm light. [7][8][9][10][11]. Though none of these techniques is perfect, each has characteristic strengths and weaknesses. For example CID is easily employed in the source region of any instrument with atmospheric pressure ionization. CID is also easily accommodated elsewhere in an instrument as long as high vacuum is not required. In contrast, IRMPD is well suited for collisionless environments. In this regard, CID and IRMPD provide complementary capabilities. Furthermore, since both methods fragment ions by the stepwise addition of small amounts of energy, the results obtained are frequently quite similar.However, CID and IRMPD are both limited by the fact that energy deposition occurs over a relatively long time scale, typically milliseconds to seconds. In contrast, ultraviolet photodissociation (UVPD) occurs on a much shorter time scale and can yield fragment ions characteristic of CID or IRMPD. However, the major limitation of UVPD is that the precursor ion must contain a suitable chromophore. For peptides, UVPD requires either short wavelength lasers (less than 200 nm) or peptides rich in tyrosine, tryptophan, and phenylalanine that can absorb at longer wavelengths. Therefore, UVPD is either limited to a small subset of all peptides or constrained by undesirable technical challenges which are encountered when working in the vacuum ultraviolet. Thus, widespread implementation of UVPD for peptide fragmentation has been to date somewhat limited.However, Brodbelt and coworkers have recently described a method to circumvent the requirement for aromatic residues or short wavelength lasers [12]. In this work, a noncovalently attached chromophore was used to absorb energy from a photon and transfer it to a peptide, causing the peptide to fragment. 18-crown-6 ether (18C6), which preferentially associates with lysine residues via the formation of three hydrogen bonds, was used for...