david l. cedeno, ph.d. department of chemistry illinois state university box 4160 normal, illinois,...
TRANSCRIPT
David L. Cedeno, Ph.D.Department of ChemistryIllinois State UniversityBox 4160Normal, Illinois, 61790-4160
Ph: +1-309-438-5595E-mail: [email protected]
Laser-based Methods Applied to the Study of Metal-Olefin Interactions and the
Photophysics of Sensitizers
General: Use spectroscopic and computational tools to study thermodynamic and kinetic aspects of different systems
Research Focus
1. Energetics and kinetics in Organometallic Chemistry. Relevance: Agriculture: Rational design of anti-ripening compounds
2. Effects of molecular structure on yields of triplet state of oxygen photosensitizers. Relevance: Clinical: Rational design of efficient photodynamic therapy compounds and fluorescent diagnostic probes.
Why are we interested on metal-olefin bonding interactions?
Metal-olefin complexes are involved in biological systems: growth of plants, senescence of flowers, ripening of fruits.
We want to understand how olefins bind to metals: why do some olefins bind better than others to a
particular metal? why do some metals bind better than others to a
given olefin? How can we control metal-olefin interactions?
Lots of processes involve breaking and forming metal-olefin bonds.
Metal-olefin complexes are involved in many catalytic systems: polymerization, hydrogenation, epoxidation, etc.
Ethylene as a plant hormone
•Ethylene binds to protein receptors in plants to signal developmental processes as seed germination, plant growth, fruit ripening, flower abscission and senescence.• Ethylene signaling involves a family of sensor/response regulator proteins (ETR, EIN, AIN, etc. The receptor is a negative regulator of a protein kinase.
Ciardi and Klee, Annals Bot., 2001, 88, 813Chang and Stadler, BioEssays, 2001, 23, 619
Anti-ripening control: Blocking ethylene action
•It has been proposed that ethylene action at the receptor site requires two steps:
•Competitive antagonists block the receptor by bonding to it for a longer time that ethylene does, thus preventing the activation of the receptor for signaling.
Cu +L
CuL
CuL
+
inactive inactive active
Cu +L
CuL
CuL
+
inactiveinactive
active
very slow
Burg and Burg, Science, 1965, 148, 1190 Sisler and Serek, Bot. Bull. Acad. Sin. 1999, 40, 1
Anti-ripening control: Blocking ethylene action
•Known competitive antagonists include:
N N
UV light
?
•An understanding of the metal-olefin interaction is important in designing anti-ripening compounds.•Why are cyclic olefins so special? Ring strain affects olefin-receptor interaction. •Are there any other effects? Is it possible to control the strength of the metal-olefin bond?
Towards a quantitaive description of metal-olefin interactions: Extending the Dewar-Chatt-Duncanson Model
Dewar, Bull. Chem. Soc. Fr., 1951, 18, C71-79; Chatt and Duncanson, J. Chem. Soc., 1953, 2939)
bond
bond
Qualitative nature of model prevents any complete rationalization of metal-olefin bond strengths, because it does not take into account all the factors involved in the interaction. We propose a quantitative extension to DCD.
Gather more experimental data: Measurement of Bond Enthalpies
Bond energies reflect the strength of the interaction
(L)nM-olefin + heat (L)nM + olefin
Use Quantum Mechanical Calculations to account for all factors in the interaction: Bond Energy Decomposition
Experimental Techniques: Time Resolved Laser Photoacoustic Calorimetry
N2 Pumped Dye Laser
EM
Preamp
DSO
CFO NF cell
PAD
BS
N2 Pumped Dye Laser
EMEM
PreampPreamp
DSO
CFO NF cell
PAD
CFO NF cell
PAD
BS
Acoustic detector
laser
Photoacoustic Sound Waves
-1.2
-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
Time (s)
No
rma
lize
d S
ign
al
(a.u
.)
Reference
Sample
)101( AlaserEkH
=1 for reference compound
Studies on M(CO)6(Cycloolefins), M = Cr, Mo, WW C O 5(olefin) O ptim ized G eom etries:W C O 5(olefin) O ptim ized G eom etries:
15.0
20.0
25.0
30.0
35.0
1 2 3 4 5 6 7 8 9
Number of Carbons
H o
r E
(kca
l/mo
l)
a)
5.0
15.0
25.0
35.0
45.0
55.0
65.0
1 2 3 4 5 6 7 8 9
Number of Carbons
Rin
g S
trai
n E
ner
gy (
kca
l/m
ol)
d)t
t
Metal-cycloolefins bond strengths correlate well but not exactly with the trend in ring strain energy
Electronic interactions, ring strain relief and Reorganizational effects: A molecular paradox
C=C Bond elongation
3.00
3.50
4.00
4.50
5.00
5.50
6.00
6.50
7.00
7.50
8.00
2 3 4 5 6 7 8 9
number of carbon atoms
∆ C
=C
(p
m)
trans
Changes in Pyramidalization Angle
5.0
10.0
15.0
20.0
25.0
30.0
2 3 4 5 6 7 8 9
number of carbon atoms
∆ p
yrim
idiz
atio
n an
gle
(deg
)
trans
Olefin Deformation Energy vs. Pyramidalization Angle
0.02.04.06.08.0
10.012.014.016.018.020.0
0.0 10.0 20.0 30.0
∆ pyrimidization angle (deg)
∆ E
(de
f.) (
kca
l/mo
l)
c8t c6
c8c
c5
c7
c4
c3
c2
Ring strain is relieved by the reorganization of the olefin as it binds, however, olefin reorganization is energetically costly, thus reducing the overall BDE.
Photodynamic Therapy (PDT)
Strong absorption in the red or near infrared (>630 nm) region of the spectrum.High quantum yield of triplet state to obtain large concentrations of the activated drug.High reactivity of the triplet with ground state oxygen to obtain measured high yields of active oxygen High affinity for diseased tissue against healthy one, to avoid the risk of photodestruction of healthy tissue Rapid metabolic rates so it can be excreted from the bodyLow toxicity in the darkSimple formulationFacile synthesis and modification of the structure.
The ideal photosensitizer:
Mechanisms of oxygen photosensitization
So
S1
To
3O2
1O2
Oxidation Reactions
Absorption
Fluorescence IC
ISC
Photoreaction
ēT-.
O2-.
Research Goal:To establish correlations between the yield of triplet sensitizer and active oxygen and the molecular structure of the photosensitizer. Correlations will lead to a rational design of sensitizers with optimized yields of triplet sensitizer and singlet oxygen
NovelPhotosensitizers (Prof. T.D. Lash)
Absorption Spectra
Emission Spectra: Fluorescence yieldTriplet energy
Triplet yield (PAC)
1O2 yield (Traps, TRF)
Computational Methods
N
NH N
HN
RR
R
R
R =Ph , C C Ph
N
NH N
HN
Et
Et
Et
Me
Et
Me
NXN
X = O, S, Se
N
N
HN
R = H, Me, t-But, Cl
OMe
MeO
R
R0
0.02
0.04
0.06
0.08
0.1
0.12
0.14
0.16
0.18
0.2
300 400 500 600 700 800 900 1000
wavelength (nm)
Ab
so
rba
nc
e
Time
1 O2 E
mis
sion
Photoacoustic Sound Waves
-1.2
-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
Time (s)
No
rma
lize
d S
ign
al
(a.u
.)
Reference
Sample
Experimental Techniques: Time Resolved VIS-NIR Emission Spectroscopy
Pumped N2
Dye Laser
CO NF cellBS
IRD
FEM
Preamp
F
PM
Pumped N2
Dye LaserPumped N2
Dye LaserPumped N2
Dye LaserN2
Dye Laser
CO NF cellBS
IRD
FEMEM
PreampPreamp
F
PM
Time
1 O2 E
mis
sion
@ 1
270
nm
kteICI 0
Extension of Conjugation, Distortion of Planarity and Photophysical Properties
TAP Emissions Spectrum
0
5
10
15
20
25
30
35
40
45
50
55
60
600 625 650 675 700 725 750 775 800 825 850 875 900 925 950 975 1000
Wavelength (nm)
Inte
nsi
ty
TAAP Emissions Spectrum
0
5
10
15
20
25
30
795 820 845 870 895 920 945 970 995 1020 1045
Wavelength (nm)
Inte
nsi
ty
TAAPAbsorption Spectrum
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0.45
350 400 450 500 550 600 650 700 750 800
Wavelength (nm)
Abs
TAP Absorption Spectrum
0
0.5
1
1.5
2
2.5
3
300 350 400 450 500 550 600 650 700 750 800
Wavelength (nm)
Ab
s
Extension of Conjugation, Distortion of Planarity and Photophysical Properties
TAAP
TAP
TPP
Research is a TEAM effort:
Collaborators: Tim Lash, Marge Jones, Pilar Mejia (ISU)Eric Weitz (Northwestern University)
Graduate Students: Richard Sniatynsky, Ken Kite, Darin Schlappi
Undergraduate Students: Hal Steiner, Jakoah BrgochPast: Cole Hexel, Paul Brackemeyer, Joel Eagles, Jeremy Woods,Tom Walczack, Ken Kite, Darin Schlappi.
High School Students: Casey Huftington, Delano Robinson, Julio Martinez.
Funding:Petroleum Research Fund – American Chemical Society.Project SEED – American Chemical Society.Illinois State University: Office of the Provost, College of Arts and Sciences, Department of Chemistry.