The authors thank Mr. Dylan Errulat and Prof. Muralee Murugesu from the Department of Chemistry and Biomolecular Sciences of the University of Ottawa for the provision of [TbEu(bpm)(tfaa)6] single crystals. E.M.R, N.R., and E.H. gratefully acknowledge the financial support provided by the University of Ottawa, the Canadian Foundation for Innovation (CFI), and the Natural Sciences and Engineering Research Council Canada (NSERC).

CAUTION: It is recommended to use safety goggles specific for the excitation wavelength being used at all times when operating the imager.
1. Configuration of the hyperspectral microscope
NOTE: An overview of the hyperspectral imaging system is given in Figure 2a, with the main components of the imager being described. The imaging system can be used for the detection of the visible or the near-infrared (NIR) emission from a sample. Depend...

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L., Brites, C. D. S., Balabhadra, S., Oliveira, H., Rocha, J., Carlos, L. D. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Nanoplatforms+for+Plasmon-Induced+Heating+and+Thermometry.">Nanoplatforms for Plasmon-Induced Heating and Thermometry.</a> ChemNanoMat. 2 (6), 520-527 (2016).</li><li>Nadort, A., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Quantitative+Imaging+of+Single+Upconversion+Nanoparticles+in+Biological+Tissue.">Quantitative Imaging of Single Upconversion Nanoparticles in Biological Tissue.</a> PLoS ONE. 8 (5), 1-13 (2013).</li><li>Sava Gallis, D. F., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Tunable+Metal-Organic+Framework+Materials+Platform+for+Bioimaging+Applications.">Tunable Metal-Organic Framework Materials Platform for Bioimaging Applications.</a> ACS Applied Materials and Interfaces. 9 (27), 22268-22277 (2017).</li><li>Varghese, S., Das, S. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Role+of+molecular+packing+in+determining+solid-state+optical+properties+of+&#960;-conjugated+materials.">Role of molecular packing in determining solid-state optical properties of &#960;-conjugated materials.</a> Journal of Physical Chemistry Letters. 2 (8), 863-873 (2011).</li><li>Yan, D., Evans, D. G. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Molecular+crystalline+materials+with+tunable+luminescent+properties:+From+polymorphs+to+multi-component+solids.">Molecular crystalline materials with tunable luminescent properties: From polymorphs to multi-component solids.</a> Materials Horizons. 1 (1), 46-57 (2014).</li><li>Mu, S., Oniwa, K., Jin, T., Asao, N., Yamashita, M., Takaishi, S. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+highly+emissive+distyrylthieno[3,2-b]thiophene+based+red+luminescent+organic+single+crystal:+Aggregation+induced+emission,+optical+waveguide+edge+emission,+and+balanced+ambipolar+carrier+transport.">A highly emissive distyrylthieno[3,2-b]thiophene based red luminescent organic single crystal: Aggregation induced emission, optical waveguide edge emission, and balanced ambipolar carrier transport.</a> Organic Electronics: Physics, Materials, Applications. 34, 23-27 (2016).</li><li>Binnemans, K. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Interpretation+of+europium(III)+spectra.">Interpretation of europium(III) spectra.</a> Coordination Chemistry Reviews. 295, 1-45 (2015).</li><li>Koyama, H., Fauchet, P. M. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Anisotropic+polarization+memory+in+thermally+oxidized+porous+silicon.">Anisotropic polarization memory in thermally oxidized porous silicon.</a> Applied Physics Letters. 77 (15), 2316-2318 (2000).</li><li>Kushida, T., Takushi, E., Oka, Y. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Memories+of+photon+energy,+polarization+and+phase+in+luminescence+of+rare+earth+ions+under+resonant+light+excitation.">Memories of photon energy, polarization and phase in luminescence of rare earth ions under resonant light excitation.</a> Journal of Luminescence. 12-13, 723-727 (1976).</li><li>Onuma, T., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Spectroscopic+ellipsometry+studies+on+&#946;-Ga2O3+films+and+single+crystal.">Spectroscopic ellipsometry studies on &#946;-Ga2O3 films and single crystal.</a> Japanese Journal of Applied Physics. 55 (12), (2016).</li><li>Favreau, P. 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The hyperspectral imaging protocol here described provides a straightforward approach that allows to obtain spectroscopic information at precise locations of the sample. Using the described setup, the spatial resolution (x and y mapping) can reach down to 0.5 &#181;m while the spectral resolution can be of 0.2 nm for the mapping at the visible range and 0.6 nm for the NIR range.
In order to conduct hyperspectral mapping on a single crystal, sample preparation follows an easy ...

Hyperspectral Imaging (HSI) is a technique that generates a spatial map where each x-y coordinate contains a spectral information that could be based on any kind of spectroscopy, namely photoluminescence, absorption and scattering spectroscopies1,2,3. As a result, a 3-dimensional set of data (also called &#8220;hyperspectral cube&#8221;) is obtained, where the x-y coordinates are the spatial axes and the z coordinate is the spectral information from the analyzed sample. Therefore, the hyperspectral cube contains both spatial and spectral information, providing a more detailed spectroscopic investigation of the sample than traditional spectroscopy. While HSI has been known for years in the field of remote sensing (e.g., geology, food industries4), it recently emerged as an innovative technique for the characterization of nanomaterials2,5 or probes for biomedical applications3,6,7,8. Generally speaking, it is not limited to the UV/visible/near-infrared (NIR) domain, but can also be extended using other radiation sources, such as X-rays &#8211; for instance in order to characterize elemental distribution in different materials9 &#8211; or Terahertz radiation, where HSI was used to perform thermal sensing in biological tissues8. Further, photoluminescence mapping has been combined with Raman mapping to probe the optical properties of monolayer MoS210. Yet, amongst the reported applications of optical HSI, there are still only a few examples on HSI of lanthanide-based materials11,12,13,14,15,16,17. For instance, we can cite: detection of cancer in tissues6, analysis of the light penetration depth in biological tissues7, multiplexed biological imaging3, analysis of multicomponent energy transfer in hybrid systems11, and investigation of aggregation-induced changes in spectroscopic properties of upconverting nanoparticles12. Clearly, the attractiveness of HSI arises from its suitability for generating knowledge about environment-specific luminescence, providing simultaneous spatial and spectral information about the probe.
Taking advantage of this powerful technique we herein describe a protocol to investigate the optical anisotropy of the heterodinuclear Tb3+-Eu3+ single crystal [TbEu(bpm)(tfaa)6] (Figure 1a)13. The optical anisotropy observed resulted from the different molecular packing of the Ln3+ ions in the different crystallographic directions (Figure 1b), resulting in some crystal faces showing brighter, others showing dimmer photoluminescence. It was suggested that the increased luminescence intensity at specific faces of the crystal was correlated with more efficient energy transfer along those crystallographic directions where the Ln3+&#183;&#183;&#183;Ln3+ ion distances were the shortest13.
Motivated by these results, we propose the establishment of a detailed methodology to analyze optical anisotropy through HSI, opening the path for better understanding of ion-ion energy transfer processes and tunable luminescent properties stemming from specific molecular arrangement18,19. These structure-properties relationships have been recognized as important aspects for innovative optical materials design including, but not limited to waveguide systems and opto-magnetic storage devices at nano and microscale &#8211; addressing the demand for more efficient and miniaturized optic systems20.

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			<td height="21" style="height:21px;width:216px;">Microscope glass slides</td>
			<td style="width:123px;">FisherBrand</td>
			<td style="width:161px;">12-550-15</td>
			<td style="width:167px;">Glass slides used for sample preparation</td>
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		<tr height="42">
			<td height="42" style="height:42px;width:216px;">Visible and Near Infrared Hyperspectral Confocal Imager</td>
			<td style="width:123px;">PhotonETC</td>
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			<td>Microscope used for the analysis, builted according to the user needs, therefore it is no catalog number</td>
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hyperspectral imaging as a tool to study optical anisotropy in lanthanide-based molecular single crystals

In this work, we describe a protocol for a novel application of hyperspectral imaging (HSI) in the analysis of luminescent lanthanide (Ln3+)-based molecular single crystals. As representative example, we chose a single crystal of the heterodinuclear Ln-based complex [TbEu(bpm)(tfaa)6] (bpm=2,2&#8217;-bipyrimidine, tfaa&#8211; =1,1,1-trifluoroacetylacetonate) exhibiting bright visible emission under UV excitation. HSI is an emerging technique that combines 2-dimensional spatial imaging of a luminescent structure with spectral information from each pixel of the obtained image. Specifically, HSI on single crystals of the [Tb-Eu] complex provided local spectral information unveiling variation of the luminescence intensity at different points along the studied crystals. These changes were attributed to the optical anisotropy present in the crystal, which results from the different molecular packing of Ln3+ ions in each one of the directions of the crystal structure. The HSI herein described is an example of the suitability of such technique for spectro-spatial investigations of molecular materials. Yet, importantly, this protocol can be easily extended for other types of luminescent materials (such as micron-sized molecular crystals, inorganic microparticles, nanoparticles in biological tissues, or labelled cells, among others), opening many possibilities for deeper investigation of structure-property relationships. Ultimately, such investigations will provide knowledge to be leveraged into the engineering of advanced materials for a wide range of applications from bioimaging to technological applications, such as waveguides or optoelectronic devices.

To illustrate the configuration of the hyperspectral microscope for the data acquisition on a Ln-based, molecular single crystal (i.e., [TbEu(bpm)(tfaa)6], Figure 1a), Figure 2 shows an overview of the system as well as the right placement of the optical cubes in the setup. Figure 3 shows a screen shot of the PHySpec software containing the menus used during the HSI acquisition. Figure 4 and ...

Watch this Scientific Journal Video about Hyperspectral Imaging as a Tool to Study Optical Anisotropy in Lanthanide-Based Molecular Single Crystals at JoVE.com

Hyperspectral Imaging as a Tool to Study Optical Anisotropy in Lanthanide-Based Molecular Single Crystals

Here, we present a protocol to obtain luminescent hyperspectral imaging data and to analyze optical anisotropy features of lanthanide-based single crystals using a Hyperspectral Imaging System.

In this work, we describe a protocol for a novel application of hyperspectral imaging (HSI) in the analysis of luminescent lanthanide (Ln3+)-based ...

Hyperspectral imaging allows for the acquisition of spectroscopic information at precise locations within a sample. For example, for the unveiling of optical anisotropy at a single crystal level. The generation of both spectral and spatial data of a sample allows for a more detailed investigation of the sample than is possible by either spectroscopy or fluorescence microscopy alone.A large number of adjustable parameters which affect the resolution can seem overwhelming at first. However, making a checklist may help with familiarizing yourself with the system. This technique requires manual tuning of the imaging hardware as well as software manipulation.It is essential to illustrate both aspects visually to showcase how both methods complement each other. Demonstrating the procedure with Nelson Rutajoga will be Emily Rodrigues, post-doctorate fellow at my laboratory. To set up the imager configuration for hyperspectral imaging mapping, starting from the microscope stage and following the emission beam pathway toward the detectors, leave the position for an optical cube right next to the optical microscope vacant and place the confocal microscope optical cube in that position that directs the emission from the sample through the visible light path.Looking along the optical path toward the detector, place the visible optical cube containing the dichroic mirror and filters for directing the visible emission to the detection path in its position. Continuing the path toward the detector, place the confocal pinhole optical cube in the right position to direct the light through the visible light detection path and following this path, place the confocal spectrometer optical cube in the appropriate position so that the emitted light reaches the detector. When all of the cubes are in place, manually adjust the detector's slit opening to match the size of the pinhole selected.Then, in the PHySpec software, select the aperture of the pinhole. For hyperspectral imaging mapping of terbium europium bi-pyrimidine trifluoroacetylacetonate single crystal, manually position the 20 times objective of the optical microscope under the sample and press the white button on the left side of the microscope to turn on the white light. Turn the knob under the button to adjust the brightness.Set the forward knob on the right side of the microscope to R to send 20%of the signal to the camera and 80%of the signal to the detector. Press play in the color camera window at the PHySpec software to initiate a live scan. If the color camera window shows a too dark or black image, increase the exposure time and/or the gain value under the color camera tab.If the image is too bright, decrease the exposure time and/or gain value. To focus on the sample, turn the knobs of the microscope to adjust the distance between the objective in the stage and open the broadband lamp shutter to allow UV excitation of the sample. Then turn the intensity knob to the desired position to control the intensity of the broadband lamp excitation.Click Show/Hide scale bar to add a scale bar to the bright-field optical microscopy image of the crystal and observe an image of the crystal under UV full or confined illumination. To select between the confined illumination or a wide field illumination, use the stick and knobs to adjust the size of the UV lamp field aperture. Under the SpectraPro SP 2300 tab, select a wavelength to observe the sample emission and adjust the exposure time of the detector.To obtain the hyperspectral cube in the sequencer, click plus to add a new node and click Confocal Imager. Click Multi-Spectrum Acquisition and input the desired X and Y position counts, as well as the desired step size. Select the hardware option for the camera sync and for visible emission mapping, and click okay.In the sequencer, click the newly added multi-spectrum acquisition line to highlight the node and click Play to run the selected node. For analysis of the captured hyperspectral imaging data, for example, for a spectral distribution of an image, in the Processing menu, select Data and Crop and Bend to increase the signal to noise ratio of the image. For an emission intensity profile, right-click on the cube image and select Create X-Profile for the analysis of one line.Drag to select the area and right-click on the region of interest. To select Add to Graph. To display the emission intensity as a function of the physical position of the target.The intensity profile will appear in the new graph. To obtain an emission spectrum of a specific area of the sample, hover the cursor over the cube image, right click, and click Rectangle Selection. Drag and click to draw the selection shape over the desired region.Then right click on the region of interest and select Add Selection to Graph. In the Add to Graph window, select Create a New Graph to display the emission spectra of the target, and click okay. Then save the acquired spectrum before selecting a new region.Here, a bright-field image of a crystal recorded after adjusting the sample in the proper focus is shown. The needle-like morphology of the crystal can be clearly observed. Here, images of the same crystal under UV excitation with either full illumination or locally confined illumination can be observed.The confined illumination can be used to investigate the effects of energy or light transfer within the crystal that may trigger wave guide-like behavior. For example, in this image, a strong emission is detected in a point not directly under excitation, suggesting that efficient energy migration takes place through the crystal. From the acquired hyperspectral cube, it is also possible to obtain the spectral distribution in the form of an image, representing a specific wavelength.The intensity profile of a specific emission wavelength and the emission spectra at any pixel or area of the acquired hyperspectral cube. For example, the emission spectra for this analysis shows the most characteristic emission bands of the europium ion. Moreover, the spatial profile along the different crystal faces indicates a brighter emission at the tip and side faces and can be correlated with the lanthanide/lanthanide ion distances in the three spatial directions.To obtain a good signal in a reasonable recording time of the hyperspectral cube, it is important to adjust the microscope configurations, focus, and detector exposure time. Emissions UV excitation and visible emission, this technique can be performed using near infrared excitation and near infrared emission detection. This allows it to be applicable for a large array of luminescent materials.Correlation of optical signals with an array of dependent features makes this technique very interesting for the investigation of structure/property relationships, including in-vitro assessment of nano-bio interactions.

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16.2K visualizações.  University of Ottawa. A imagem hiperespectral permite a aquisição de informações espectroscópicas em locais precisos dentro de uma amostra. Por exemplo, para a revelação de anisotropia óptica em um único nível de cristal. A geração de dados espectrais e espaciais de uma amostra permite uma investigação mais detalhada da amostra do que é possível apenas por espectroscopia ou microscopia de fluorescência.Um grande número de parâmetros ajustáveis que afetam a resolução pode parecer esmaga...