new xeol investigation of rare earth ions in luminescent silica … · 2013. 9. 6. · xeol...

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XEOL investigation of Rare Earth ions in luminescent silica-based nanoparticles. In this contribution an apparatus for the collection of X-ray Excited Optical Emission (XEOL) spectra is presented. This technique is applied to rare-earth based luminescent materials for medical applications. Good quality data can be collected and the spectra reveal different environments for the Rare Earth ions depending on the preparation route. Introduction Optical imaging is the latest trend in imaging-guided diagnosis and/or therapy that involve the detection of light photons transmitted through tissues. The challenge is to prepare structures (namely nanoparticles (NP) doped with Rare Earths (RE) that can enter the human body) emitting light in a spectral range of minimum absorption by the tissues. Sample preparation IST has addressed the problem of Er/Yb-doped-NP with improved up-conversion efficiency . Two kind of samples were compared here: I) RE doped (fluoride precursors) NaYF 4 NPs dispersed in silica (F-type) and II) RE-doped (acetate precursors) silica NPs (A-type). The XEOL apparatus @ GILDA XEOL data were collected at GILDA the Italian CRG at the European Synchrotron Radiation Facility. A sketch of the apparatus is shown below: The light emitted by the sample is collected by two lenses and sent to the detector via an optic fibre. The detector consists in a Phtoto Multiplier Tube (PMT) with a photocathode sensitive in the region 300-650nm. Results of the benchmark test of the apparatus on a ZnO sample. The data collected in transmission mode (blue) , PMT detector (red) and a Si PIN diode (green) detector are compared. Optical characterization The Upconversion signal from the samples was measured by exciting at 980nm. The picture below shows the emission patterns in the case of the F series (left) and A series (right). XEOL data In the present case the XEOL signal collected at the Yb-L3 edge is shown in the picture below: The spectrum of the A series sample is typical of a glassy environment whereas that of the F series correspond to the Yb oxyde. Identical data are obtained my measuring XAS in the conventional fluorescence mode. The XEOL in this case is reasonably generated by the upconversion of Er ions neighboring (within about 100nm) the X-ray excited Yb ions. Conclusion A XEOL apparatus has been developed at the GILDA beamline at ESRF and is open to users. A test on rare earth doped nanoparticles has permitted to evidence a different environment depending on the preparation technique. This work has been partially financed by the CNR-FCT collaboration program 2011-2012. L. M. Fortes acknowledges FCT for financial support under the post-doctoral fellowship SFRH/BPD/34754/2007. The authors thank V. Calvo (CEA Grenoble), A. Martin (CNR-IOM Trieste) and F. Rocca (FBK Trento) for useful discussions and technical help in the realization of the XEOL apparatus. F. d'Acapito 1* , M. C. Gonçalves 2 , L. Fortes 2 1 CNR-IOM-OGG c/o ESRF GILDA CRG Grenoble France, 2 IST ICEMS/UTLisbon Portugal Sample 1 st Lens 2 nd Lens Fibre Detector 400 500 600 700 800 900 0 10000 20000 30000 40000 PL intensity (a.u.) Wavelength (nm) F10 F7 F3 400 500 600 700 800 900 0 1x10 6 2x10 6 PL intensity (a.u.) Wavelength (nm) A10 A7 A3

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Page 1: New XEOL investigation of Rare Earth ions in luminescent silica … · 2013. 9. 6. · XEOL investigation of Rare Earth ions in luminescent silica-based nanoparticles. In this contribution

XEOL investigation of Rare Earth ions in

luminescent silica-based nanoparticles.

In this contribution an apparatus for the collection of X-ray Excited Optical Emission (XEOL) spectra is presented. This technique is applied to rare-earth based luminescent materials for medical applications. Good quality data can be collected and the spectra reveal different environments for the Rare Earth ions depending on the preparation route.

IntroductionOptical imaging is the latest trend in imaging-guided diagnosis and/or therapy that involve the detection of light photons transmitted through tissues. The challenge is to prepare structures (namely nanoparticles (NP) doped with Rare Earths (RE) that can enter the human body) emitting light in a spectral range of minimum absorption by the tissues.

Sample preparationIST has addressed the problem of Er/Yb-doped-NP with improved up-conversion efficiency . Two kind of samples were compared here: I) RE doped (fluoride precursors) NaYF4 NPs dispersed in silica (F-type) and II) RE-doped (acetate precursors) silica NPs (A-type).

The XEOL apparatus @ GILDA

XEOL data were collected at GILDA the Italian CRG at the European Synchrotron Radiation Facility. A sketch of the apparatus is shown below:

The light emitted by the sample is collected by two lenses and sent to the detector via an optic fibre. The detector consists in a Phtoto Multiplier Tube (PMT) with a photocathode sensitive in the region 300-650nm.

Results of the benchmark test of the apparatus on a ZnO sample. The data collected in transmission mode (blue) , PMT detector (red) and a Si PIN diode (green) detector are compared.

Optical characterization

The Upconversion signal from the samples was measured by exciting at 980nm. The picture below shows the emission patterns in the case of the F series (left) and A series (right).

XEOL data

In the present case the XEOL signal collected at the Yb-L3 edge is shown in the picture below:

The spectrum of the A series sample is typical of a glassy environment whereas that of the F series correspond to the Yb oxyde. Identical data are obtained my measuring XAS in the conventional fluorescence mode. The XEOL in this case is reasonably generated by the upconversion of Er ions neighboring (within about 100nm) the X-ray excited Yb ions.

Conclusion

A XEOL apparatus has been developed at the GILDA beamline at ESRF and is open to users. A test on rare earth doped nanoparticles has permitted to evidence a different environment depending on the preparation technique.

This work has been partially financed by the CNR-FCT collaboration program 2011-2012. L. M. Fortes acknowledges FCT for financial support under the post-doctoral fellowship SFRH/BPD/34754/2007. The authors thank V. Calvo (CEA Grenoble), A. Martin (CNR-IOM Trieste) and F. Rocca (FBK Trento) for useful discussions and technical help in the realization of the XEOL apparatus.

F. d'Acapito1*, M. C. Gonçalves2, L. Fortes2

1 CNR-IOM-OGG c/o ESRF GILDA CRG Grenoble France, 2 IST ICEMS/UTLisbon PortugalHea

der

Intr

oduc

tion

Con

tent

Foo

ter

Sample

1st Lens2nd Lens

Fibre

Detector

400 500 600 700 800 9000

10000

20000

30000

40000

PL

inte

nsi

ty (

a.u

.)

Wavelength (nm)

F10 F7 F3

400 500 600 700 800 900

0

1x106

2x106

PL

inte

nsi

ty (

a.u

.)

Wavelength (nm)

A10 A7 A3