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Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy
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Page 1: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

Christopher LeavittYale University

Vibrational spectra of cryogenic peptide ions using H2 predissociation spectroscopy

Page 2: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

Motivation

• Characterize the effects of protonation in peptide ions

• Investigate the dependence of varying substituents across the peptide backbone to peptide conformation

Page 3: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

Structural Probe: Methylation

+

H2O

N

H

O

NHH

O

OH

O

O

NHH

HN

O

OHH

H

N

H

O

N+HH

O

OH

H

H+

N

CH3

O

N+HH

O

OH

H

R= H, CH3

N

R

O

N+RH

O

OH

H

N

H

O

N+HH

O

OH

H

N

H

O

N+H3C

H

O

OH

H

N

CH3

O

N+H3C

H

O

OH

H

Page 4: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

Cryogenic Mass Spectrometry: H2-Tagging in a Quadrupole Ion Trap

Wiley-McLarenextraction region

Ion optics

To time-of-flightand 2-D infrared analysis

Electrosprayneedle

Heated capillary

90° ionbender

RF only quadrupolesH2/He filled 3-D quadrupoleion trap with temperature

control to 10 KEinzel

Octopoles

1st skimmer

2nd skimmerDifferential

aperture

50 K heat shield

1x10-5 1.5x10-23x10-7Pressure (Torr) 1.5 760

GlyGlyH+

T = 300K

T = 10K

Ion

Inte

nsity

(A

.U.)

Mass (m/z)

+H3N

O

HN

O

OH

1 2 3 4 5 6

* *

*

* * * * *133 137 141 145

Page 5: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

FromESI

600-4500 cm-1

2m Flight TubeMCP Detector

Mass Gate

Reflectron

Yale Photofragmentation TOF Spectrometer

Ion Optics

A+ · (H2)m + h → A+ · (H2)n + (m-n) H2

Page 6: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

D0

Infrared Spectrum of GlyGlyH+

800 1200 1600 2800 3200 3600 4000

Photon Energy, cm-1

Pre

dis

so

cia

tio

n Y

ield

H2 stretch

Polfer, N. C., Oomens, J. Mass Spectrom. Rev. 2009, 28, 468-494Wu, R., McMahon, T. B. J. Phys. Chem. B 2009, 113, 8767-8775Kamrath, M., et. al. J. Am. Chem. Soc. 2011, 133, 6440-6448

IVR

IRMPD•Room Temperature•Tens to hundreds of photons are necessary to dissociation molecules

Page 7: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

Infrared Spectrum of GlyGlyH+

800 1200 1600 2800 3200 3600 4000

Photon Energy, cm-1

Pre

dis

so

cia

tio

n Y

ield

H2 stretch

Wu, R., McMahon, T. B. J. Phys. Chem. B 2009, 113, 8767-8775Kamrath, M., et. al. J. Am. Chem. Soc. 2011, 133, 6440-6448

IVR

Cryogenic H2 Predissociation•Ions are vibrationally cold•Single photon results in dissociation

H2

H2

Page 8: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

MP2/6-311++G(d,p)

800 1200 1600 2800 3200 3600 4000

Photon Energy, cm-1

Ca

lcu

late

d I

nte

ns

ity

Pre

dis

so

cia

tio

n Y

ield

H2 stretch

O-H stretch

Protonated Amine

freeH2

N-H Region

Amide Region

Fingerprint Region

Wu, R., McMahon, T. B. J. Phys. Chem. B 2009, 113, 8767-8775Kamrath, M., et. al. J. Am. Chem. Soc. 2011, 133, 6440-6448

Infrared Spectrum of GlyGlyH+

Page 9: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

n = 1

Pre

dis

soci

atio

n Y

ield

3100 3200 3300 3400 3500 3600 3700

Photon Energy, cm-1

n = 2

Cal

cu

late

d I

nte

nsi

ty

n = 0

O-H stretch

H2 solvation of GlyGlyH+

Asym. NH2

stretch

Amide NH

Sym. NH2

stretch

O-Hstretch

Asym. NH2

stretch

Amide NH stretch

Sym. NH2

stretch

Optimization and Frequency Calculations at MP2/6-311+G(d,p)

Page 10: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

Structural Probe: Methylation

1.065

1.689

127.2°

GlyGlyH+(1)

1.069

128.0°

1.654

GlySarH+(1)

1.8401.043

118.0°

SarSarH+(1)SarGlyH+(1)

1.9551.038

114.0°

a) b)

c) d)

Optimization and Frequency Calculations at MP2/6-311+G(d,p)

Extended,“all trans” Kinked,

carboxyl rotated

Page 11: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

2400 2600 2800 3000 3200 3400 3600 3800 4000 4200

Photon Energy, cm-1

freeH2

freeD2

Pre

diss

ocia

tion

Yie

ld

O-H stretch

Asym. NH2

Amide NH

Sym. NH2

Amine NH

GlyGlyH+•(H2)1

SarSarH+•(D2)2

SarGlyH+•(H2)2

GlySarH+•(D2)2

*

*

N-H Stretching Region: Methylation Study

N

CH3

O

N+HH

O

OH

H

N

H

O

N+HH

O

OH

H

N

H

O

N+H3C

H

O

OH

H

N

CH3

O

N+H3C

H

O

OH

H

Page 12: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

Fingerprint Region: Methylation Study

800 900 1000 1100 1200 1300 1400 1500 1600 1700 1800 1900

Photon Energy, cm-1

Pre

diss

ocia

tion

Yie

ld

CO-HBend

Amide II C=O

Amide I

*

*

Optimization and Frequency Calculations at MP2/6-311+G(d,p)

CO-H Bend

Amide II

Amide I

C=O

N

CH3

O

N+HH

O

OH

H

N

H

O

N+HH

O

OH

H

N

H

O

N+H3C

H

O

OH

H

N

CH3

O

N+H3C

H

O

OH

H

Page 13: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

Missing Shared Proton Bands

MP2/6-311++G(d,p)

800 1200 1600 2800 3200 3600 4000

Photon Energy, cm-1

Ca

lcu

late

d I

nte

ns

ity

Pre

dis

so

cia

tio

n Y

ield

H2 stretch

O-H stretch

Protonated Amine

freeH2

N-H Region

Amide Region

Fingerprint Region

Wu, R., McMahon, T. B. J. Phys. Chem. B 2009, 113, 8767-8775Kamrath, M., et. al. J. Am. Chem. Soc. 2011, 133, 6440-6448

Page 14: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 2.2

0

2500

5000

7500

10000

N-H Distance, Å

En

erg

y, c

m-1

GlyGlyH+

GlySarH+

SarGlyH+

SarSarH+

H2N

CH2

C

OH

Identifying the Shared Proton Mode

0

1

1555 cm-1

Optimization calculations at MP2/6-311++G(d,p)

Page 15: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

Identifying the Shared Proton Mode

800 1000 1200 1400 1600 1800 2000

Pre

diss

ocia

tion

Yie

ld

Photon Energy, cm-1

N

H

O

NHH

O

OH

Na+

N

H

O

N+HH

O

OH

H

Page 16: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

800 1200 1600 2400 2800 3200 3600

Photon Energy, cm-1

Identifying the Shared Proton Mode

•All structures are nominally protonated on the amino group, and feature an intramolecular H-bond between the amino group and the amide oxygen.

•Addition of a methyl group at the amide position induces rotation of the peptide backbone.

•Isotope substitution to help confirm the assignment of the intramolecular h-bond

•Isomer selective IR-IR double resonance experiments to determine the extent of multiple isomers present.

Page 17: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

Thanks to:Mark JohnsonMike KamrathArron WolkEtienne GarandPeter JordanRachael RelphHelen GerardiKrissy BreenAndrew DeBlaseJoe FournierGary WeddleTim Guasco(UCSD)Mike Van Stipdonk (Wichita State)Anne McCoy(The Ohio State University)

Acknowledgements

Page 18: Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.

hprobe

Reflectron

Sig

nal

Time of Flight, ms

prob

e fr

agm

ent

pum

p fr

agm

ent

Detector

Predissociation Dip Spectroscopy

hpump

(scanned)

Coaxial TOF

±1.5 keV

(fixed)

Our Challenge:

Not enoughtemporal separation!

The Solution:

Earlier firstlaser crossingand mass selection!


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