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Introduction. I attended the 3rd Annual CARS Workshop in Harvard in June 2003Here are some of the basic ideas of the technique.. Workshop. Sunney Xie: ChemistCame to Harvard in 1999Pioneered CARS developmentsThird annual CARS workshopPhysicists, Biologists, Industry peopleLecturesLab prac
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1. CARS Microscopy Third Annual Workshop
2. Introduction I attended the 3rd Annual CARS Workshop in Harvard in June 2003
Here are some of the basic ideas of the technique
.
3. Workshop Sunney Xie: Chemist
Came to Harvard in 1999
Pioneered CARS developments
Third annual CARS workshop
Physicists, Biologists, Industry people
Lectures
Lab practicals
4. Outline
What is CARS?
Why use it?
Non Resonant Background
Sources
Detection schemes
Applications
Problems?
Discussion
5. What is CARS? Non linear Raman process
Generated at the focus of the beam
?AS = 2?p - ?s
7. Why use CARS?
Intrinsic vibrational contrast
Strong, directional signal => Sensitive
Requires moderate average powers good for biological samples
Only generated at focus => 3D sectioning capability
Higher in frequency than one-photon fluorescence => easily detected in presence of a strong fluorescent background.
Near IR => little scattering, deep penetration in tissues
Near IR => little absorption, Low photodamage
8. Non-resonant Background Non-resonant Background from the bulk!
9. Two colours
Difference between pump and Stokes span the vibrational spectrum
Modelocked sources
Picosecond pulses
Time-bandwidth product
Tunability for exciting different vibrations
OPO pumped by ps Laser
10. Detection Schemes F CARS: Forward detected
E CARS: Epi detected
P- CARS: Polarisation dependent
FM CARS: Frequency modulated
11. F CARS
12. F CARS
13. Detection Schemes F CARS: Forward detected
E CARS: Epi detected
P- CARS: Polarisation dependent
FM CARS: Frequency modulated
14. Avoid non resonant background!
Objects smaller than ?p/3 (too short for destuctive interference)
Interfaces with different ?3 - to propagation
Back-scattering of F CARS, reflactive/turbid media i.e. tissue
15. E CARS Images of a hairless mouse ear. The Raman shift is set at 2,845 cm1 (p 816.8 nm) to address the lipid CH2 symmetric stretch vibration. The frames are averaged for 2 s. (A) Stratum corneum with bright signals from the lamellar lipid intercellular space that surrounds the polygonal corneocytes. Bright
punctuated dots are ducts of sebaceous glands. (B) Sebaceous glands at 30 m from skin surface. (C) Individual cells of the gland compartment can be
recognized, with nuclei visible as dark holes (arrow). (D) Adipocytes of the dermis at 60 m from skin surface. (E) Adipocytes of the subcutaneous layer at a
depth of 100 m. (F) 2D projection of 60 depth-resolved slices separated by 2 m. Panels to the right and under F show the yz and xz cross sections taken at
the white lines, respectively.
Images of a hairless mouse ear. The Raman shift is set at 2,845 cm1 (p 816.8 nm) to address the lipid CH2 symmetric stretch vibration. The frames are averaged for 2 s. (A) Stratum corneum with bright signals from the lamellar lipid intercellular space that surrounds the polygonal corneocytes. Bright
punctuated dots are ducts of sebaceous glands. (B) Sebaceous glands at 30 m from skin surface. (C) Individual cells of the gland compartment can be
recognized, with nuclei visible as dark holes (arrow). (D) Adipocytes of the dermis at 60 m from skin surface. (E) Adipocytes of the subcutaneous layer at a
depth of 100 m. (F) 2D projection of 60 depth-resolved slices separated by 2 m. Panels to the right and under F show the yz and xz cross sections taken at
the white lines, respectively.
16. E CARS
17. Detection Schemes F CARS: Forward detected
E CARS: Epi detected
P- CARS: Polarisation dependent
FM CARS: Frequency modulated
18. P CARS
20. Detection Schemes F CARS: Forward detected
E CARS: Epi detected
P- CARS: Polarisation dependent
FM CARS: Frequency modulated
22. Sensitive probe for lipids
Lipid bilayer, thin objects, small objects
Fast dynamic scanning of processes in living cells
High damage threshold
In vivo capabilites
23. Non resonant background term very strong
Expensive laser sources
Have to know beforehand the vibrational band of interest
Currently limited tunability of sources improving in line with the laser sources
.
24. Discussion?