The multiplexed capsule samples and the AH samples were dissolved in 10 mM ammonium formate (pH 9) and injected onto a NanoEase 5 µm XBridge BEH130 C18 300 µm x 50 mm column (Waters Corporation, Milford, MA) at 3 µL/min in a mobile phase containing 10 mM ammonium formate (pH 9). Peptides from the capsules were eluted by sequential injection of 20 µL volumes of either 14%, 20%, 25%, 30%, 50%, and 90% ACN (6 fractions – first experiment) or 17%, 21%, 23%, 25%, 27%, 29%, 31%, 33%, 35%, 40%, and 90% ACN (11 fractions – second experiment) in 10 mM ammonium formate (pH 9) at 3 µL/min flow rate, while peptides from AH were eluted using 17%, 20%, 21%, 22%, 23%, 24%, 25%, 26%, 27%, 28%, 29%, 30%, 32%, 35%, 37%, 40%, 50%, and 90% ACN (18 fractions). Eluted peptides were diluted at a three-way union with a mobile phase containing 0.1% formic acid at 24 µL/min flow rate and delivered to an Acclaim PepMap 100 µm x 2 cm NanoViper C18, 5 µm trap (Thermo Fisher Scientific) on a switching valve.
After 10 minutes of loading, the trap column was switched on-line to a PepMap RSLC C18, 2 µm, 75 µm × 25 cm EasySpray column (ThermoFisher Scientific). TMT 11-plex labeled peptides from capsules were then separated at low pH in the second dimension using a 7.5% to 30% ACN gradient over 83 minutes in mobile phase containing 0.1% formic acid at 300 nL/min flow rate, while TMT 16-plex labeled peptides from AH were separated using a 5% to 25% ACN gradient over 100 minutes. Tandem mass spectrometry data were collected using an Orbitrap Fusion Tribrid instrument (Thermo Scientific, San Jose, CA) configured with an EasySpray NanoSource. Survey scans were performed in the Orbitrap mass analyzer (resolution = 120,000), with internal mass calibration enabled, and data-dependent MS2 scans using dynamic exclusion performed in the linear ion trap using collision-induced dissociation. Reporter ion detection was performed in the Orbitrap mass analyzer using MS3 scans after synchronous precursor isolation of the top 10 ions in the linear ion trap, and higher energy collisional dissociation in the ion-routing multipole. Instrument parameters for the three individual TMT experiments are provided in
Supplementary Table S2.