dc.description.abstract |
<p>Two-photon excited fluorescence microscopy (TPM) has become a standard biological
imaging tool due to its simplicity and versatility. The fundamental contrast mechanism
is derived from fluorescence of intrinsic or extrinsic markers via simultaneous two-photon
absorption which provides inherent optical sectioning capabilities. The NIR-II wavelength
window (1000–1350 nm), a new biological imaging window, is promising for TPM because
tissue components scatter and absorb less at longer wavelengths, resulting in deeper
imaging depths and better contrasts, compared to the conventional NIR-I imaging window
(700–1000 nm). However, the further enhancement of TPM has been hindered by a lack
of good two-photon fluorescent imaging markers in the NIR-II. </p><p>In this dissertation,
we design and characterize novel two-photon imaging markers, optimized for NIR-II
excitation. More specifically, the work in this dissertation includes the investigation
of two-photon excited fluorescence of various highly conjugated porphyrin arrays in
the NIR-II excitation window and the utilization of nanoscale polymersomes that disperse
these highly conjugated porphyrin arrays in their hydrophobic layer in aqueous environment.
The NIR-emissive polymersomes, highly conjugated porphyrins-dispersed polymersomes,
possess superb two-photon excited brightness. The synthetic nature of polymersomes
enables us to formulate fully biodegradable, non-toxic and surface-functionalized
polymersomes of varying diameters, making them a promising and fully customizable
multimodal diagnostic nano-structured soft-material for deep tissue imaging at high
resolutions. We demonstrated key proof-of-principle experiments using NIR-emissive
polymersomes for in vivo two-photon excited fluorescence imaging in mice, allowing
visualization of blood vessel structure and identification of localized tumor tissue.
In addition to spectroscopic characterization of the two-photon imaging agents and
their imaging capabilities/applications, the effect of the laser setup (e.g., repetition
rate of the laser, peak intensity, system geometry) on two-photon excited fluorescence
measurements is explored to accurately measure two-photon absorption (TPA) cross-sections.
A simple pulse train shaping technique is demonstrated to separate pure nonlinear
processes from linear background signals, which hinders accurate quantification of
TPA cross-sections.</p>
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