7
2
H. Chen et al. / Journal of Alloys and Compounds 511 (2012) 70–73
Fig. 4. (a) Upconversion spectrum of UCNPs under the excitation of 980 nm, insert: (left) photograph of the UCNPs dispersed in deionized water. (Right) Upconversion
3
+
3+
luminescence photograph of the same solution. (b) Energy level diagrams of Yb ions and Tm ions and the possible upconversion processes.
1
3
1
3
1
3
means the PVP molecules can well chelate with RE ions [20]. In
the reaction process, the PVP acts as a chelating agent and could
coordinate with RE ions. After the formation of UCNPs, it can act as
an amphiphilic surfactant and drive the UCNPs dispersing in ethy-
lene glycol or water. In our experiment, it can be supposed that the
remains of PVP on the surface of UCNPs can form hydrogen bond
with water molecules, as shown in Fig. 3(b). Presumably, this is why
the UCNPs could be well dispersed in water and kept transparent for
months. The photos of the UCNPs in water are shown in the insert of
Fig. 4(a). The capping ligands on the surfaces of UCNPs were exam-
ined by Fourier transform infrared (FTIR) spectrum, as shown in
Fig. 3(c). Some absorption bands in this spectrum confirm the pres-
ence of PVP molecules on the surfaces of UCNPs. The bands centered
D → F , G → H , and G → F , respectively. The UC mecha-
2
4
4
6
4
4
3
+
3+
nism of NIR-to-visible/UV in this Yb , Tm codoped NaYF system
was studied [21]. Fig. 4(b) describes schematically possible upcon-
4
3+
3+
verted processes in energy level diagrams of Yb and Tm ions.
Under the excitation of 980 nm NIR, Yb3+ ions, served as sensitiz-
3+
ers, absorb NIR photons and transfer the energy to Tm ions to
3
3
1
3+
populate the excited states ( H , F , and G ) of Tm ions. The
5
2
3
4
cross-relaxation process of 3F2, 3 → H (Tm3+): H → D (Tm
3
1
3+
)
6
4
2
1
may play the most important role in populating D . Thereafter,
2
1
2
2
3+
the state I can be populated by the process of F → F (Yb ):
6
5/2
7/2
1
1
3+
3+
3+
D → I (Tm ). In our experiments, the energy transfer from Yb
2
6
3+
to Tm is efficient, which resulted in effective population of Tm
ions in the high-energy state of G . From the spectrum in Fig. 4(a),
1
4
−1
at 2958, 2923, and 2852 cm are associated with the stretching
we can see that the strongest peak is centered at 479 nm, and there-
fore the UCNPs dispersed aqueous solution exhibits bright blue
luminescence under the excitation of 980 nm NIR, as shown in the
insert of Fig. 4(a). The excellent transparency also can be seen from
these photos. Through the solution the background words can be
well distinguished.
vibration of methyl (–CH ), the asymmetric (as), and symmet-
3
ric (s) stretching vibrations of methylene (–CH ), respectively.
2
−1
The band at 1290 cm originates from the stretching vibration of
carbon nitrogen bond (C–N) and the band at 1664 cm
−
1
orig-
inates from the vibration of carbon oxygen bond (C O). The
nitrogen and oxygen atoms can coordinate with the metal ions,
leading to PVP molecules adhered to the surfaces of UCNPs. It
For further investigation of their applicability as luminescent
◦
probes, the UCNPs were incubated with HeLa cells at 37 C for 24 h.
−
1
should be noticed that the C O groups (1664 cm ) on the sur-
faces of UCNPs can form hydrogen bonds with water molecules.
After washing with PBS to remove excess UCNPs, the living cells
were imaged on an Olympus IX71 microscope equipped with a 980-
nm NIR laser. Fig. 5(a) shows the bright-field images of the living
HeLa cells that endocytosed UCNPs. We can observe that the cell
morphology is good [22]. Then the sample was excited in situ by the
980-nm laser. We can clearly see the bright upconversion lumines-
cence in the image of Fig. 5(b). (For interpretation of the references
to color in this figure, the reader is referred to the web version of the
article.) The overlay images of the luminescence and the HeLa cells
are shown in Fig. 5(c). We can see that the blue luminescence well
overlaps the cells, which confirms that the UCNPs are successfully
used as luminescent probes to label the cancer cells with strong UC
luminescence. These results imply that the UCNPs are biocompat-
ible and can be used as potential luminescent probes for biological
imaging.
−1
The strong band around 3428 cm
can be attributed to the
O–H stretching vibrations. Above analysis indicates that PVP
molecules are well attached on the surface of the UCNPs, and
therefore leading to the well dispersibility of nanocrystals in the
solvents.
Both the as-prepared nanocrystals powders and their aqueous
solution can emit visible and UV luminescence under the NIR exci-
tation of 980 nm. We detect the UC spectrum using the 980 nm
continuous wave diode laser as pumping source. The power of the
focused laser is 140 mW. As shown in Fig. 4(a), there are character-
istic peaks of Tm3+ ions in the UC spectrum of the aqueous solution.
These peaks which center at 291, 350, 362, 450, 479, and 648 nm
are attributed to the transitions of 1I6 → H , I → F , D → H ,
3
1
3
1
3
6
6
4
2
6
Fig. 5. (a) Bright-field image and (b) luminescence image under the excitation of 980 nm and (c) the overlay image of HeLa cells labeled with the UCNPs.