• Title/Summary/Keyword: Protonated peptide ion

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Integrated Thermochemical Approach to Collision-Induced Dissociation Process of Peptides

  • Shin, Seung Koo;Yoon, Hye-Joo
    • Mass Spectrometry Letters
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    • v.12 no.4
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    • pp.131-136
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    • 2021
  • Collision-induced dissociation of peptides involves a series of proton-transfer reactions in the activated peptide. To describe the kinetics of energy-variable dissociation, we considered the heat capacity of the peptide and the Marcus-theory-type proton-transfer rate. The peptide ion was activated to the high internal energy states by collision with a target gas in the collision cell. The mobile proton in the activated peptide then migrated from the most stable site to the amide oxygen and subsequently to the amide nitrogen (N-protonated) of the peptide bond to be broken. The N-protonated intermediate proceeded to the product-like complex that dissociated to products. Previous studies have suggested that the proton-transfer equilibria in the activated peptide affect the dissociation kinetics. To take the extent of collisional activation into account, we assumed a soft-sphere collision model, where the relative collision energy was fully available to the internal excitation of a collision complex. In addition, we employed a Marcus-theory-type rate equation to account for the proton-transfer equilibria. Herein, we present results from the integrated thermochemical approach using a tryptic peptide of ubiquitin.

Electronic Spectroscopy of Protonated Tyr-Ala Dipeptide Ions (Tyr-Ala 펩타이드 이온의 전자전이 분광 연구)

  • Choi, Chang-Min;Kwon, Jang-Sook;Kim, Hwan-Jin;Yoon, Tae-Oh;Yang, Min-O;Kim, Nam-Joon
    • Journal of the Korean Chemical Society
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    • v.51 no.4
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    • pp.318-323
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    • 2007
  • Electronic photofragmentation spectrum of protonated tyrosine-alanine dipeptide ions(YAH+) was obtained in the wavenumber region of 34500~36700 cm-1 using a quadrupole ion trap time-of-flight mass spectrometer (QIT-TOFMS). YAH+ ions were produced by electrospray ionization, stored in the ion trap and then irradiated by ultraviolet laser pulses which induced photofragmentation of the ions. The electronic photofragmentation spectrum was obtained by monitoring the photodissociation yields of YAH+ ions as a function of the laser wavelength. The spectrum exhibited two broad peaks which were assigned as S1 and S2 by theoretical calculations using a time-dependent density functional method. The broad widths of the peaks in the spectrum were explained by the overlaps of the peaks originated from various conformers of YAH+ ions which were present in the gas phase at room temperature and also by the contributions of the hot bands.