AN INTRODUCTION TO HIGH RESOLUTION COHERENT MULTIDIMENSIONAL SPECTROSCOPY New 2D and 3D tools for...
22
AN INTRODUCTION TO HIGH RESOLUTION COHERENT MULTIDIMENSIONAL SPECTROSCOPY New 2D and 3D tools for dealing with severe rotational congestion Peter C. Chen , Thresa A. Wells, and Zuri R. House Spelman College, Atlanta GA Benjamin R. Strangfeld Georgia Institute of Technology, Atlanta GA
AN INTRODUCTION TO HIGH RESOLUTION COHERENT MULTIDIMENSIONAL SPECTROSCOPY New 2D and 3D tools for dealing with severe rotational congestion Peter C. Chen,
AN INTRODUCTION TO HIGH RESOLUTION COHERENT MULTIDIMENSIONAL
SPECTROSCOPY New 2D and 3D tools for dealing with severe rotational
congestion Peter C. Chen, Thresa A. Wells, and Zuri R. House
Spelman College, Atlanta GA Benjamin R. Strangfeld Georgia
Institute of Technology, Atlanta GA
Slide 2
Two Dimensional Spectroscopy On-diagonal peaks: Similar to 1D
spectroscopy Off-diagonal peaks: Provides new information on the
relationship (coupling, correlation, etc.) between peaks. Benefits:
improves resolution and can potentially provide new information. I
or A or 2D Contour Plot (XYZ surface) Conventional 1D Spectrum (XY
plot)
Slide 3
Nd:YAG Laser Raman Shifter Broadband OPO Monochromator with CCD
sample Nd:YAG Laser Tunable OPO or dye laser Simplified
Experimental Diagram for 2D Four wave mixing: 3 input beams 1
output beam 1234 1.Tunable dye or OPO 2.Broadband OPO 3.Broadband
OPO 4.Output
Slide 4
Coherent 2D spectrum of NO 2 (off-diagonal region) 2 frequency
axes 1 intensity axis
Slide 5
Slide 6
N=2 N=4 N=6 N=8 Nuclear spin statistics: N= only even values
for Ka=0 Doublets due to spin-rotation interaction Additional peaks
could be due to: Different Ka subgroups Other vibronic origins Hot
bands Extra peaks that disobey selection rules due to conical
intersections
Slide 7
J=1 J=2 J=3 J=4 , cm -1 , cm -1 J=1 J=2 J=3 J=4 cm -1 , cm -1
B=B Boxes are concentric B B Boxes are not concentric Resembles a
double Fortrat parabolaX-shaped cluster CLUSTER SHAPE: peaks
ordered by J
Slide 8
Simulated spectra of 79 Br 2, 79,81 Br 2, and 81 Br 2 513 nm
514 nm Simulated 2D: (v 3 = 25 v 4 = 26-50) Simulated 1D spectrum:
Peak density is approximately 1000 peaks per nm v 4 =26 v 4 =27v 4
=28v 4 =29 4 (nm) 1 (nm) Intercluster: parabolas ordered by v and
isotopomer Intracluster: Peaks ordered by J Peaks compete for
limited space along 1D axis: patterns difficult to find
Slide 9
2D Clusters / information Electronic general location of
off-diagonal features Vibrational inter-cluster relationships.
Spacing between clusters corresponds to spacing between vibrational
levels. Rotational intra-cluster relationships. Shape and size of
each cluster depends upon rotational constants.
Slide 10
81 Br 2 79,81 Br 2 79 Br 2 Result: peaks spatially separated by
isotopomer, but congestion remains a problem in many areas. Note
the crowding by peaks from from lower lying parabolas, (v 1
>25). Also, no selectivity. 4 (nm) 1 (nm) v 4 =26 v 4 =27 v 4
=28v 4 =29 v 1 =25 P. C. Chen and M. Gomes, JPC A 112, 2999-3001,
2008.
Nd:YAG Laser Nd:YAG Laser Raman Shifter Broadband OPO
Monochromator with CCD sample Tunable dye laser Nd:YAG Laser
Tunable OPO Simplified Experimental Diagram for 3D Result: two
tunable sources: OPO vs. dye laser Approach: scan one, step the
other The stepped laser provides the selectivity
1 2 3 4 hgfahgfa hgdahgda gdbagdba gfeagfea 1 3 2 4 3 1 2 4 3 2
1 4 1 2 3 4 aa fa ha ga aa da ha ga aa da ba ga aa fa ea ga fa ha
ga da ha ga da ba ga fa ea ga P (3) = (3) EEE (3) =
Slide 15
Inter-cluster pattern OPO 44 44 dye laser ea da ha ba fa ha ba
ga da ga Process 1Process 2Process 3Process 4 OPO scan: rectangular
gridrarerare parallelogram Dye laser scan: rare rectangular grid
parallelogramrare fa ha ga da ha ga da ba ga fa ea ga
Denominator:
Slide 16
Process 1Process 2Process 3Process 4 OPO scan Dye laser scan or
Intra-cluster pattern In a congested field, triplets (triangles)
are easier to identify than doublets or singlets. (For more
information on the structure of these triplets, see Ben Strangfelds
talk, RD11) Processes 1 and 4 are most likely because of weaker NIR
interactions for processes 2 and 3 for most molecules.
Slide 17
Combined inter-cluster and intra- cluster patterns or Process
1, OPO scan Process 4, OPO scan 44 44 44 44 OPO Type of triangle
depends upon whether the DL selects an R-type plane or a P-type
plane R-typeP-typeR-typeP-type
Slide 18
Dye laser Narrowband OPO monochromator R plane P plane 2D Side
view of box 3D Dye laser selects OPO scans Mchr scans R selected P
selected 2D vs 3D spectra The concentric boxes in 2D space are
expanded into 3D space.
Slide 19
Implications High resolution Coherent 3D spectroscopy can be
thought of as a selective version of its 2D counterpart. This
selectivity is made by fixing one of the input lasers while
scanning the other(s). The 2D spectrum is expanded into 3D space;
Fixing one of the narrowband input lasers selects a P- type or
R-type plane Scanning the other lasers/mchr produces the resulting
slice in this 3D space
Slide 20
Next 3 talks RD 10 - Thresa A. Wells: NO 2 and intercluster
patterns RD 11 - Benjamin R. Strangfeld: Br 2 and intracluster
patterns RD 12 - Zuri R. House: I 2 and future directions
Slide 21
Summary High resolution spectroscopy of large or complex
molecules suffers from congestion: Unresolved peaks Lack of
identifiable patterns Coherent 2D spectroscopy: Improves resolution
Provides peak sorting (by v, J, and isotopomer). Coherent 3D
spectroscopy: Further improves resolution over 2D Provides
selectivity.
Slide 22
Current and former group members: Candace Joyner Krystle
McBride LaTasha Amisial Kyndra Cottingham Marcia Gomes Rebecca
Massey Lindsai Bland Jaimie Miller Kamilah Mitchell Afrah Boigny
Thresa Wells - NO 2 Christa Fields Tyler Sugars Notorious Scott
Haviland Forrester Zuri House - I 2 Benjamin Strangfeld - Br 2
Collaborators: Paul Houston, Georgia Tech. Funding: NSF grants
CHE-0616661 & CHE-0910232