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. 2014 Feb 5;136(5):1706-9.
doi: 10.1021/ja410438n. Epub 2014 Jan 17.

Self-illuminating 64Cu-doped CdSe/ZnS nanocrystals for in vivo tumor imaging

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Self-illuminating 64Cu-doped CdSe/ZnS nanocrystals for in vivo tumor imaging

Xiaolian Sun et al. J Am Chem Soc. .

Abstract

Construction of self-illuminating semiconducting nanocrystals, also called quantum dots (QDs), has attracted much attention recently due to their potential as highly sensitive optical probes for biological imaging applications. Here we prepared a self-illuminating QD system by doping positron-emitting radionuclide (64)Cu into CdSe/ZnS core/shell QDs via a cation-exchange reaction. The (64)Cu-doped CdSe/ZnS QDs exhibit efficient Cerenkov resonance energy transfer (CRET). The signal of (64)Cu can accurately reflect the biodistribution of the QDs during circulation with no dissociation of (64)Cu from the nanoparticles. We also explored this system for in vivo tumor imaging. This nanoprobe showed high tumor-targeting ability in a U87MG glioblastoma xenograft model (12.7% ID/g at 17 h time point) and feasibility for in vivo luminescence imaging of tumor in the absence of excitation light. The availability of these self-illuminating integrated QDs provides an accurate and convenient tool for in vivo tumor imaging and detection.

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Figures

Figure 1
Figure 1
Design of self-illuminating 64Cu-doped QDs.
Figure 2
Figure 2
(A) PET and optical images of aqueous suspensions of QDs (nonradioactive), free 64CuCl2, mixture of 64CuCl2 and QDs, and 64Cu-doped QDs with the same amount of 64Cu radioactivity. (B) Comparison of the total photon flux extracted from the phantom images in (A). QDs without excitation light and 64Cu presence had virtually no photoluminescence. The total photon flux recorded from the IVIS system without emission filter followed the order of 64Cu-doped QDs > 64Cu mixed with QDs > 64Cu. (C–E) Photon flux obtained from 64Cu, mixture of 64Cu and QDs, 64Cu-doped QDs as well as QDs with QD526 (C), QD580 (D), and QD636 (E) under different emission filters versus the filter wavelengths. Increased photon flux at the emission wavelength of the QDs reflects effective Cerenkov resonance energy transfer (CRET).
Figure 3
Figure 3
(A) Representative whole-body coronal PET images of U87MG tumor-bearing mice at 1, 17, 24, and 42 h after intravenous injection of 250 μCi of 64Cu-doped QD580 (n = 3). White arrow, tumor area; black arrow, liver area. Slices for the images are 1 mm thick. QDs show typical reticuloendoethlial system uptake in the liver and spleen as well as tumor accumulation via an EPR effect. (B) ROI analysis of U87MG tumor uptake of 64Cu-doped QDs over time (n = 3). (C) Representative whole-body luminescence images of U87MG tumor-bearing mice at 1, 17, 24, and 42 h postinjection of 250 μCi of 64Cu-doped QD580 (n = 3). White arrow, tumor area; black arrow, liver area. (D) Comparison of photon flux obtained via an open window without filter and that obtained via a filter covered from 575 to 650 nm in the tumor area 42 h postinjection of 250 μCi of 64Cu-doped QDs.

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