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Materials Science and Engineering Laboratory FY 2004 ... - NIST

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Technical Highlights<br />

Coherent Anti-Stokes Raman Scattering (CARS) for<br />

In-Situ Chemical Imaging of Tissue <strong>Engineering</strong> Constructs<br />

Design issues relating to bioactive devices for<br />

regenerative medicine reflect the spatial <strong>and</strong><br />

chemical complexity of biological <strong>and</strong> materials<br />

issues <strong>and</strong> their interactions. Tools developed<br />

for the purpose of aiding underst<strong>and</strong>ing of these<br />

systems must have sufficient discriminatory power<br />

to sort out this complexity. We have introduced<br />

a relatively simple broadb<strong>and</strong> spectroscopic<br />

microscopy based on CARS that can be used to<br />

rapidly acquire volumetric, chemically-specific<br />

images with submicrometer resolution.<br />

Marcus T. Cicerone<br />

Biological research in general could be significantly<br />

aided by a high-resolution, chemically sensitive<br />

volumetric imaging method that allows rapid, non-invasive<br />

study of processes on the tissue, cellular <strong>and</strong> sub-cellular<br />

levels. The need for such a method is particularly<br />

acute in the field of tissue engineering, where cycles<br />

of cell-seeding <strong>and</strong> analysis can take months. St<strong>and</strong>ard<br />

analysis methods are labor intensive <strong>and</strong> destructive,<br />

so multiple endpoint studies must be performed <strong>and</strong><br />

temporal correlation assumed. Non-invasive microspectroscopic<br />

imaging could alleviate many problems<br />

associated with the evaluation of tissue scaffolds both<br />

by allowing continuity of analysis on a single scaffold<br />

construct, <strong>and</strong> by maintaining spatio-temporal information.<br />

Our vision is the creation of a non-invasive microscopic<br />

imaging technique that rapidly discriminates between an<br />

arbitrary number of chemically distinct structures or<br />

species in a spatially resolved way within a biological<br />

system. We envision that this would be done without<br />

staining or otherwise intrusively manipulating the system.<br />

We expect that such a microscopy tool would have a<br />

significant impact on the way in-vitro tissue-engineering<br />

studies are carried out.<br />

While our vision may sound fanciful, the basis<br />

for such powerful <strong>and</strong> generally applicable chemical<br />

discrimination was established many decades ago via<br />

vibrational spectroscopy. Our contribution has been<br />

to marry broadb<strong>and</strong> vibrational spectroscopy, with<br />

its inherent chemical resolving power, to a nonlinear,<br />

multiphoton microscopy (CARS microscopy), which<br />

has already been demonstrated to have significant utility<br />

for non-invasively imaging biological systems, even in<br />

the absence of significant chemical resolving power.<br />

Microscopic coherent anti-Stokes Raman<br />

scattering (µCARS) can answer important imaging<br />

2<br />

needs of the biological research community, including<br />

relative non-invasiveness, rapidity, <strong>and</strong> chemical specificity.<br />

CARS provides chemical specificity through its intrinsic<br />

sensitivity to molecular vibrational transitions. CARS is<br />

sensitive to the third order polarizability, χ (3) , which has<br />

nonresonant <strong>and</strong> resonant components, the latter being<br />

related to the Raman scattering cross section. Therefore,<br />

µCARS uses Raman (vibrational) susceptibility as a<br />

contrast mechanism, but it is approximately 10 3 more<br />

efficient than spontaneous Raman scattering.<br />

Figure 1: Energy level diagram for single frequency CARS<br />

process (solid vertical arrows) <strong>and</strong> broadb<strong>and</strong> CARS (solid<br />

<strong>and</strong> dashed vertical arrows).<br />

The solid vertical lines of Figure 1 represent<br />

transitions made by molecules in the “classic” CARS<br />

scheme. Molecules in a sample of interest are promoted<br />

to a specific energy E = h (wp – wS), where ωp <strong>and</strong> ωS are the frequencies of the near infrared pump <strong>and</strong><br />

Stokes light pulses, respectively, <strong>and</strong> h is h/2π where h<br />

is Planck’s constant. If that energy corresponds to a<br />

particular excited vibrational state in the molecule, that<br />

state is populated. A subsequent probe photon (also ωp) promotes the vibrationally excited molecule to another<br />

(higher) virtual state, from which it relaxes <strong>and</strong> emits<br />

an anti-Stokes photon at a specific frequency, ωaS. The flux of anti-Stokes photons detected is proportional<br />

to the number of molecules initially prepared in the<br />

targeted vibrationally excited state. To date, this<br />

“classic” µCARS scheme has been used to acquire only<br />

single-frequency or narrowb<strong>and</strong> (200 cm –1 –<br />

–<br />

) vibrational<br />

information, <strong>and</strong> thus, chemical specificity is limited<br />

to only one or two species simultaneously.

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