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Cooperet al. Nanoparticles for radiation therapy
charge-transfer emissionsor othermechanisms.YAG,BaF2, and
Y2O3 are among those that have been adapted to thenanoscale,
but have not yet been investigated to a large extent as SA
nanoscintillators. These compositions are also routinely doped
withotheractivators, resultinginvariouseffectsontheir intrinsic
luminescence.
BIOCOMPATIBILITYOFLANTHANIDE-BASEDMATERIALS
Preparation of LnNP bioconjugates (covalent attachment of
organicmolecules of interest to theNP surface ligands) appears
infrequently in the literature. The principles of bioconjugation
are similar to those forQDs, Au, or otherNPs, with some dis-
tinct stability and solubility concerns (Cao et al., 2012; Jiang
et al., 2012). Ligand-exchanged and silicated LnNPs typically
presentprimaryamine functionalitieswhichprovide someaddi-
tionalversatilityovercarboxylgroups.Aminesprovideanumber
of conjugation routes, including routine reactions with amine,
isothiocyanate,carboxyl,hydroxyl,andthiolfunctionalgroupson
amoleculeofinterest.Onestudyreportedconjugatesofphospho-
rylethanolamine (PEA)-stabilized Eu3+ and Ce3+/Tb3+-doped
LaF3byreactingthefreeamineoftheligandwithactivatedbiotin-
PEG ormPEGNHS esters, demonstrating a successful strategy
forattachmentofmolecules throughamidebondformation.The
use of these conjugates was restricted to borate buffer. Biotin
conjugates have also been preparedwithCeF3:TbNPs silanized
using TEOS/aminopropyltriethoxysilane (APTES) (Kong et al.,
2007,2008a)andPEA-stabilizedLn3+-dopedzirconia (Liuet al.,
2012).
SCINTILLATINGNANOPARTICLEINTERACTIONSWITHDYESAND
PHOTOSENSITIZERS(PSs)
When nanoparticles are conjugated to PS molecules and irra-
diatedwith ionizing radiation, singlet oxygen yield will depend
upon scintillation yield and energy transfer efficiency. Neither
of these parameters has been widely reported in the literature.
However,agoodnumberof studieshave investigated lanthanide-
dye charge transfer using light excitation, anda few studies have
lookedat singletoxygengeneration.
Lanthanide energy and charge transfer (ET and CT) have
been extensively studied for lanthanide chelates andorganic dye
pairs (Selvin, 1996, 2002), andmore recently in LnNPs, though
most efforts have focused on sensitization of 4f-4f lumines-
cence by Ce3+, Yb3+ or surface-associated organic molecules.
The situation can quickly become rather complex with lan-
thanides whose luminescence involves the 4fn configuration. In
these cases, magnetic dipole transitions are allowed and may
have intensity of the sameorder ofmagnitude as electric dipole
transitions. Additionally, some induced dipole transitions are
hypersensitive to the environment of the lanthanide ion and
apparently follow the selection rulesof electric quadrupole tran-
sitions, leading them to be referred to as pseudo-quadrupolar
transitions.
A2004reportinvestigatedenergytransferbetweenporousnet-
works of interconnected 18nm YAG:Ce3+ nanocrystals (NCs)
and the amine-reactive fluorescent dye tetramethylrhodamine
isothiocyanate (TRITC) (Wuister et al., 2004).Glycinewas used to coat the NCs, bound to the surface through the carboxy-
late moieties and providing terminal amines for attachment of
TRITC. ET for the conjugate was demonstrated through strong
emissionofTRITC relative toNCs following selective excitation
of the NCs, as well as the appearance of a fast initial decay of
the time-resolvedPL.TheETwasestimatedusingFörster-Dexter
theory, giving a “critical distance” (equivalent to R0) of 7nm,
resulting in energy transfer rates of up to 108 s−1 forCe3+ sites
within5nmof theNCsurface, supposedtobe∼90%of the total
Ce3+ giventheNCsize.
Electrostatic complexes of CePO4:Tb nanorods and
Rhodamine B (RhB), using Ce3+-sensitized Tb3+ emission
to excite RhB, resulted in ET efficiency η up to 0.85 as deter-
mined by ratiometric luminescence analysis (Di et al., 2010).
EvidenceofETwastakenbythequenchingoftheNPsteady-state
luminescence and concomitant increase in RhB emission with
increasing amounts ofRhB.Time-resolvedmeasurements of the
5D4→7F5 transition of Tb3+ also exhibited quenching but did
not quantitatively agree, reporting efficiencies lower than those
determined by steady-state quenching (η ∼ 0.7 at the highest
quenchingcondition).
A recent (2013) study investigated electrostatic complexes
of LaPO4:Ce nanorods and the fluorescent dye coumarin 440
(C-440) using steady-state and time-resolved PLmeasurements
(Kar et al., 2013). The Stern-Volmer sphere of action static
quenchingmodelwasapplied to the steady-statequenching, and
theETefficiency estimatedby the ratioof theCe3+fluorescence
lifetimes, giving η=0.24 for an estimated 1:47 nanorod:dye
ratio. ET was corroborated by an increase of the fluorescence
lifetimeof the dye, excited at 280nm,when complexedwith the
nanorods.
X-ray-induced singlet oxygen production has been inves-
tigated with a handful of Tb3+-activated oxide and fluoride
nanoscintillators coupled with grafted or encapsulated pho-
tosensitizers. In one study, 11-aminoundecanoic acid-coated
La0.8Tb0.2F3 NPs were mixed with the water-soluble photo-
sensitizer meso-tetra(4-carboxyphenyl) porphine (MTCP) (Liu
et al., 2008), which resulted in an increase in the quenching
rate of the anthracenedipropionic acid (ADPA) singlet oxygen
probe compared toPS alone under 250keVX-ray irradiation at
44cGy/min. Singlet oxygenproductionwas demonstrated using
(Gd0.5Tb0.5)2O3 NPs with PS-encapsulating polysiloxane shells
(Seve et al., 2012). The photosensitizer 5-(4-carboxyphenyl)-
10,15,20-triphenyl-chlorin (TPC)wasfirst conjugated toAPTES
beforereactionoftheTPC-APTESwithTEOSforshellformation,
resulting invaried amountsof covalently boundTPCembedded
within the shell. In this case, increasingconcentrationsof encap-
sulatedTPCresultedinquenchingoftheTPCPL(directlyexcited
at414nm)aswellas singletoxygenproduction(directlydetected
through 1270nm phosphorescence). This result was attributed
tomigrationof excitationenergybetweenTPCmolecules termi-
natedatstaticquenchingsites,withamodeldevelopedtosupport
thedata.
Recently, energy transfer mechanisms and singlet oxygen
production under optical and X-ray irradiation were stud-
ied using a similar system consisting of Gd-free Tb2O3 NPs
with thephotosensitizer5-(4-carboxyphenyl)-10,15,20-triphenyl
Frontiers inChemistry | ChemicalEngineering October2014 |Volume2 |Article86 | 55
Cancer Nanotheranostics
What Have We Learnd So Far?
- Title
- Cancer Nanotheranostics
- Subtitle
- What Have We Learnd So Far?
- Authors
- João Conde
- Pedro Viana Baptista
- Jesús M. De La Fuente
- Furong Tian
- Editor
- Frontiers in Chemistry
- Date
- 2016
- Language
- English
- License
- CC BY 4.0
- ISBN
- 978-2-88919-776-7
- Size
- 21.0 x 27.7 cm
- Pages
- 132
- Keywords
- Nanomedicine, Nanoparticles, nanomaterials, Cancer, heranostics, Immunotherapy, bioimaging, Drug delivery, Gene Therapy, Phototherapy
- Categories
- Naturwissenschaften Chemie