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Fragmentation of Organic Molecules Desorbed from a Surface using Secondary-Ion Mass Spectrometry Alger Pike Nicholas Winograd
Secondary-Ion Mass Spectrometry SIMS ,[object Object],[object Object]
SIMS in Combinatorial Chemistry An optical image of a bead-holder specially fabricated for 60   m polystyrene beads (capacity: 10,000 beads/cm 2 ) The TOF image of Sasrin-Biotin beads loaded into the bead-holder. The molecular mass of biotin 245.3 amu is   shown in green. R. M. Braun, A. Beyder, J. Xu, M. C. Wood, A. G. Ewing and N. Winograd, Anal. Chem. 71, 3318 (1999).
Why Study Fragmentation? ,[object Object],[object Object],[object Object]
Types of Fragmentation 1) Direct Desorption 2) Desorb then Fragment 3) Ion-Beam Induced
The ARTOF-SIMS Machine
ARTOF-SIMS Sample Manipulator a) Azimuthal Rotation: Sample rotates like the hands of a clock, around the center of the crystal. b) Polar Rotation: Sample rotates like a revolving door, around the axis perpendicular to the azimuthal axis.
Ion Trajectories
Simulation Parameters
Simulation Results
Simulation vs. Real
Machine Automation
Design Goals ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Controllable Parameters
CD 3 S-Cu (100): The Model System 1) Chemisorption to a four-fold hollow 3) No domains 2) No tilt angle due to short R group 4) Simplified mass spectra Imanishi, S. Takenaka, T. Yokoyama, Y. Kitajima and T.Ohta J. PHYS. IV FRANCE 7 (1997)
FCC (100) Surface 1) Red atom is an ejecting atom 2) Blue atoms are blocking atoms 3) SIMS yield decreases with blocking
Azimuthal Distribution of Cu(100) 50 0
1200 L CD 3 SH on Cu(100) High Mass
1200 L CD 3 SH on Cu (100) Low Mass
Overall Fragmentation of CD 3 SH (total fragments signal) (total monolayer signal) F =
Direct Desorption Fragmentation Low energy cascade that desorbs an ion which does not have enough energy to fragment.
Direct Desorption Fragmentation
Fragmentation After Desorption High energy cascade leads to desorbed species which have enough energy to further fragment.
Fragmentation After Desorption
Ion-Beam Induced Fragmentation The ion beam directly breaks a bond which causes desorption of the fragment into vacuum.
Ion-beam Induced Fragmentation (fragment signal) (total monolayer signal) C =
Two-Body Model Simulation
Ion Trajectories at 35 º Incidence Angle
Summary ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Acknowledgements ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Further Evidence for Cu 2 SCD 3 +  Ejection ,[object Object],[object Object],[object Object],[object Object]
Further Evidence for CD 3 +  Formation XSCD 3 +     XS + CD 3 +
Image Potential
Ion Profile Above Extraction Plate

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