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Near-Infrared Fluorescence for Multimodal Bioimaging
DOI: 10.17691/stm2018.10.1.06 Received November 2, 2017
Y.-C. Lin, PhD, Research Fellow, Department of Physics1; Research Fellow2; L.-W. Tsai, Master Student, Department of Physics1;
E. Perevedentseva, PhD, Research Fellow, Department of Physics1; Research Fellow of Luminescence3;
A. Karmenyan, PhD, Research Fellow, Department of Physics1; C.-L. Cheng, PhD, Professor, Department of Physics1
1National Dong Hwa University, 1, Sec. 2, Da-Hsueh Rd., Shoufeng, Hualien, 97401, Taiwan, R.O.C.; 2Institute of Physics, Academia Sinica, 128, Sec. 2, Academia Rd., Nangang Dist., Taipei, 11529, Taiwan, 3P.N. Lebedev Physical Institute, Russian Academy of Sciences, 53 Leninskiy Prospekt, Moscow, 119991, Russia
Nanodiamonds (ND) are emerging as a promising candidate for the multimodal bioimaging due to their optical and spectroscopic properties. Fluorescence properties of ND are determined by defects and admixtures in the crystal lattice. The most developed bioapplications of the ND fluorescence are using nitrogen-vacancy centers. However they emit fluorescence in the visible region which overlaps with the autofluorescence from biological objects.
The aim of the study was to analyze the fluorescence of nickel-related color center in nanodiamond with emission in the near-infrared range (883-885 nm) in terms of its applications for bioimaging using one-photon and two-photon excitations.
Materials and Methods. Synthetic diamond powders (Kay Diamond, USA) of sizes in the range from 100 nm to 2.5 |m were carboxylated and characterized with Raman and photoluminescence spectroscopy at one-photon and two-photon excitation. Baby hamster kidney cells were treated with 500 nm ND for 8 h and subjected to microscopic investigations using laser confocal fluorescence scanning microscopy and photoluminescence mapping.
Results. The effects of the particles size, temperature and excitation conditions on the fluorescence of Ni-related center are studied. Variability of the emission with sizes (as well as with excitation wavelength and temperature) gives the possibility to select the most suitable nano- or microparticles to use as a fluorescent probe. The two-photon excitation of Ni centers in nano- and microdiamond are demonstrated. The possibility to use Ni color center for bioimaging is presented using confocal fluorescence imaging and fluorescence mapping of distribution of 500 nm ND in baby hamster kidney cells. The emission of Ni-related center (885 nm) showing no photobleaching and no damage to the baby hamster kidney cells and the location of ND is clearly observed relatively the cells.
Conclusion. Fluorescence from Ni-related color center at one-photon and two-photon excitation can be an option in biological imaging to avoid cell autofluorescence and to shift the excitation to lower energy laser excitation which is safer and transparent for biological objects.
Key words: nanodiamond; Ni-related defects; near-infrared emission; color center; fluorescence; bioimaging.
How to cite: Lin Y.-C., Tsai L.-W., Perevedentseva E., Karmenyan A., Cheng C.-L. Near-infrared fluorescence from nanodiamond for multimodal bioimaging. Sovremennye tehnologii v medicine 2018; 10(1): 49-56, https://doi.org/10.17691/stm2018.10.1.06
Russian
Флюоресценция наноалмазов в ближнем инфракрасном диапазоне. Использование для мультимодального биоимиджинга
Оптические и спектральные свойства наноалмазов в настоящее время рассматриваются с точки зрения применения в биомедицинских исследованиях, в частности как флюоресцентные метки для биоимиджинга. Флюоресценция наноалмазов определяется в первую очередь дефектами и примесями в кристаллической решетке. Наиболее хорошо изученными и используемыми флюорес-центыми центрами в наноалмазах являются азотные вакансии. Однако они излучают в видимой области спектра и их излучение перекрывается с автофлюоресценцией большинства биологических объектов.
Цель исследования — изучение флюоресценции никелевого центра в наноалмазе, излучающего в ближнем инфракрасном диапазоне (883-885 нм), с точки зрения возможностей его применения для биоимиджинга при однофотонном и двухфотонном возбуждении.
Corresponding author: Chia-Liang Cheng, e-mail: [email protected]
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Материалы и методы. Использованы синтетические наноалмазы (Kay Diamond, США) с размером частиц от 100 нм до 2,5 мкм и с карбоксилированной поверхностью. Спектральные свойства частиц изучались методами комбинационного рассеяния и люминесцентной спектроскопии при однофотонном и двухфотонном возбуждении. Также изучалось взаимодействие наноалмазов размером 500 нм с клетками baby hamster kidney (BHK). Клетки инкубировались с наноалмазами в течение 8 ч, затем анализировались их изображения, полученные с помощью лазерной конфокальной флюоресцентной сканирующей микроскопии, а также распределение интенсивности фотолюминесценции по изображению.
Результаты. Максимум излучения флюоресценции Ni-центра наблюдается на длине волны около 885 нм. Показано, что на флюоресценцию влияют размер частиц наноалмазов, температура, а также условия возбуждения. Вариабельность излучения в зависимости от размеров частиц, температуры, длины волны возбуждения дает возможность выбирать оптимальные нано- или микрочастицы и условия для использования наноалмазов в качестве флюоресцентного зонда. Продемонстрирована возможность наблюдать флюоресценцию Ni-центров в нано- и микроалмазных частицах при двухфотонном возбуждении. Возможность использования Ni-центра в наноалмазах как флюоресцентного зонда при конфокальной флюоресцентной микроскопии, а также для флюоресцентного картирования показана для клеток BHK с наноалмазами размером 500 нм, которые хорошо заметны в цитоплазме клеток. Отмечено отсутствие фотообесцвечивания излучения Ni-центра и повреждение клеток при их взаимодействии с наноалмазами.
Заключение. Использование флюоресценции Ni-центра в наноалмазе при однофотонном и двухфотонном возбуждении в качестве маркера для биоимиджинга позволяет наблюдать их вне области автофлюоресценции клеток и в так называемом окне прозрачности биологического объекта. Кроме того, флюоресценция Ni-центра может быть возбуждена более безопасным лазерным излучением в ближней ИК-области.
Ключевые слова: наноалмазы; Ni-дефекты; флюоресцентные центры свечения; ближнее инфракрасное излучение; флюоресценция; биоимиджинг.
Introduction
Nanodiamond (ND) has been identified as a promising candidate for the multifunctional applications in biomedical researches for its physical/chemical properties and numerous confirmed biocompatible studies. Particularly, optical and spectroscopic properties of ND are considered for the purposes of multimodal bioimaging (including drug delivery tracing) and biosensing [1, 2].
The defect-originated color centers in ND are suitable for numerous possible applications ranging from quantum information processing as single-photon sources [3-5] to optical markers for cellular imaging [1, 2, 6]. The most well-studied and utilized defect to date is nitrogen-vacancy (NV) color centers which appear in neutral (NV0) and negative (NV-) charge states with zero-phonon lines (ZPL) at 575 nm (2.156 eV) and 637 nm (1.945 eV), respectively [3, 5, 7]. NV color centers emit stable emission with broad spectral ranges at room temperature and are recently used for bioimaging and biosensing [8]. However, the limitation is the fluorescence wavelength predominantly are between 400 to 550 nm, this overlaps with most biomolecules that absorb light between 280 to 500 nm ranges [9], some obstacles do exist for bioapplications using NV centers. Therefore, for an improved biolabelling, there is a need the emission be shifted above this wavelength region.
To circumvent the obvious limitation associated with the use of NV centers, the potential use of fluorescence in the near-infrared region from silicon-vacancy (with ZPL at 737 nm) [6] or some of nickel (Ni) centers [10] would be an alternative for the detection, as its emission is far away from most of the biomolecules and commercial dyes. Synthetic diamond grown by the high-pressure high-
temperature technique uses a nickel-containing metallic catalyst, and nickel is usually inevitably included in the resulting diamond. Particularly, dispersed nickel atoms can be incorporated in diamond producing color centers with emission in the infrared region, result in the 1.4 eV Ni-related center (with ZPL near 885 nm) with negative nickel ion in the center of a diamond divacancy, and nickel-nitrogen complex NE8 with ZPL at 796 nm formed by a substitutional nickel atom with four adjacent nitrogen atoms using chemical vapor deposition (CVD) method. It is also possible to fabricate single nickel-nitrogen defects in diamond [11]. Recently, the near-infrared emitting Ni-related centers are produced in ND [11, 12]. Ni-related optical centers are considered as alternatives to the NV. A number of schemes are available for creating Ni-related optical centers in diamond, such as incorporation of Ni during CVD growth or by ion implantation. Ion implantation promises the best control over the location, density and proximity to the surface of the optical center [13]. Note that Ni centers from Ni-enriched ND can be excited with different wavelength, including wavelength in the red region [11, 12] and that increases their interest for bioimaging. Additional imaging opportunity is opened due to the observed two-photon excitation of ND demonstrated previously for NV centers [14]. It allows shifting the excitation to the infrared region for deeper penetration of the excitation light into the tissue, increasing the spatial resolution and the laser penetration depth. Also it decreases the out of focus effects on the bio-object and results in decreased photobleaching and photodamage of the sample [15].
In this report we discuss the Ni-related (1.4 eV) center observed in the as-received ND [16, 17] excited with ultraviolet light and with two-photon femtosecond
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excitation in infrared range with fluorescence detected in the near-infrared range (with peak near 885 nm). The effects of ND size, temperature and excitation conditions on the emission are discussed. The application of Ni center as a biolabel using fluorescence mapping technique is demonstrated. The possibility to use this color center for bioimaging applications is presented using fluorescence mapping of distribution of 500 nm ND in baby hamster kidney cells (BHK). The emission of Ni-related center (885 nm) showing no photobleaching and no damage to the BHK cells and the location of ND is clearly observed relatively the cells.
Materials and Methods
In this study, synthetic ND powders (Kay Diamond, USA) of sizes in the range from 100 nm to 2.5 |jm were used. The ND powders were carboxylated, resulting in carboxylated ND, using strong acid treatments to remove the metallic impurities, non-diamond carbon and forming carboxyl groups on the surface as reported in detail earlier [18]. For characterizations, the obtained ND powders of various sizes were separately dispersed in de-ionized water in a concentration of 2 mg/ml. From each suspension, 20 |jl was dropped onto single crystal silicon (100) wafer and dried. Raman spectra and photoluminescence (PL) of ND's were measured using confocal micro-Raman spectrometer (Jobin Yvon, T64000; HORIBA Ltd, Japan) equipped with a liquid N2 cooled charge-coupled device detector at 532 nm (solid state; Elforlight, UK) and 325 nm (He-Cd gas phase; Kimmon Koha, Japan) wavelength laser excitations. The laser power through the objective lens was estimated to be 2 mW (532 nm excitation, measured from objective) and 20 mW (325 nm excitation, measured from laser's output), which did not raise the sample temperature significantly. For low-temperature measurements, the samples were mounted in a Linkam variable temperature microscope stage (THMS 600; Linkam Scientific, UK) and the temperature was allowed to stabilize for at least 5 min before acquiring the spectra.
Two-photon excited spectra measurements were measured using Shamrock 303i Spectrograph (Andor Technology Ltd, UK) at femtosecond tunable excitation of Chameleon Ultra II Ti:Sapphire laser (Coherent, USA), excitation wavelength 760 nm, repetition rate 80 MHz, pulse duration 140 fs, input laser power 96 mW, with band-pass filter FF01-716_43-25. The registration was done in 800-1000 nm spectroscopic range with single photon counting system PicoHarp 300 (PicoQuant, Germany) and cooled photomultiplier tube connected with optical microscope Olympus IX71 (Olympus, Japan), objective magnification was 40*.
Baby hamster kidney cells were cultured in complete DMEM (Dulbecco's modification of Eagle's medium) medium with 2% fetal bovine serum (Invitrogen Co., USA), at 37°C and 5% CO2 in a humidified incubator (310/Thermo; Forma Scientific, Inc., USA). The cells
were grown on coverslips in a 22 mm Petri dish for 16 h before treatment with ND, and then co-incubated with 500 nm ND for 8 h. After the treatment, the cells were washed with isotonic PBS (phosphate buffer saline, pH 7.4) and then fixed with 4% paraformaldehyde solution in PBS for 1 h at 37°C. The samples of cells with ND adhered to the coverslips were used for microscopic investigations. Laser confocal scanning microscope (Leica TCS SP5; Leica Microsystems, Germany) equipped with argon laser (458/476/488/ 514 nm wavelength) was employed for fluorescence studying of the interactions of ND and BHK.
Photoluminescence mapping was recorded using an avalanche photodiodes detector at 325 nm He-Cd gas phase laser excitation (Kimmon Koha, Japan). The laser power passed through a 40* objective lens was measured to be 100 jW. Near-infrared edge long pass filter (Semrock, Canada) which transmitted wavelength from 800 nm to 1200 nm was used. Each figure captured area 30*30 |jm with 100*100 pixels resolution.
Result and Discussion
Figure 1 depicts the photoluminescence spectra from 500 nm ND measured with 532 nm (a)-(c) and 325 nm (d)-(f) wavelength laser excitations. Due to the ND luminescence defect nature and abundant defect centers of ND, varying excitations can excite different color centers. As shown in Figure 1 (a), at 532 nm wavelength laser excitation the emission from NV- center predominates with the sideband centered near 690 nm and ZPL at 638 nm. This is more clear and pronounced at low-temperature (110 K) measurements. In Figure 1 (d) with 325 nm wavelength laser excitation the luminescence is mostly in the 470-600 nm range, where N3, H4, NV0 centers emit [19, 20]; the shoulder at higher wavelengths of this peak can be attributed to the emission from NV0 center (ZPL at 575 nm isn't visible here) and the sideband near 600 nm.
At ultraviolet excitation, an isolated peak at 885 nm is observed, both at room temperature and at 110 K (Figure 1 (e)), while at 532 nm wavelength laser excitation this weak peak in this range is observed only at low temperature (Figure 1 (b)). The peak at 885 nm is attributed to Ni-related center with Ni+ ion in the center of a diamond divacancy, where Ni is probably not bonded to the carbon neighbors, described also as 1.4 eV center. For this center emission, the doublet with maximums near 1.401 and 1.404 eV have been previously observed [11], originates from a transition between an excited state and two ground states with the lines splitting, from the C and Ni isotopic structure. The exact positions of the 1.4-eV lines depend on the strain in the sample [11]. Despite the variability of some characteristic, the Ni-related centers can be observed for many synthetic and natural diamonds [21, 22] including high-temperature high-pressure ND [17, 23].
In addition to the 1.4 eV center in the studied ND, at ultraviolet excitation we can clearly observe doubled
Nanodiamond's Near-Infrared Fluorescence for Bioimaging СТМ J 2018 — vol. 10, No.1 51
(b)
LÜuijj^j^uiMkiL,. 295 K
550 600 650 700 750 800 850 900 860 870 880 890 900
Wavelength (nm)" Wavelength (nm)
d Aex=325 nm
to
e
to
(e) П.
f
to
638 nm
570
600 630
Wavelength (nm)
484 nm
400 500 600 700 800 900 860 870 880 890 900
Wavelength (nm) Wavelength (nm)
450 480 510
Wavelength (nm)
540
Figure 1. Photoluminescence spectra from 500 nm nanodiamond measured at (a)-(c) 532 nm and (d)-(f) 325 nm wavelength excitations
The weak peak at 880 nm is expanded in (b) and (e) shown the 1.4 eV Ni center emission. In (c) and (f), the region near the excitation is magnified revealing details of the fluorescence emission
Aex=532 nm
b
c
peaks at 484 nm (2.56 eV) and 488 nm (2.54 eV), considered as also Ni-related centers with Ni- occupies a tetrahedral position, substituting for a carbon atom, and nickel-nitrogen defect (NE2), described as Ni+ ion bound to divacancy surrounded by two or three nitrogen atoms in nearest coordination sphere, correspondingly [24]. Observed in both natural and synthetic diamond (including ND), the Ni centers have been studied with PL spectroscopic analysis [23] as well as with electron paramagnetic resonance technique [25] and with analysis of cathodoluminescence [17, 26]. The correlation between 1.4 eV center and 2.56 eV center has been established before [27]. The doublets at 484/488 nm are although strong enough are excited only at low temperature (160 K) and in the blue-green range. This may have photonic applications, but may not be suitable for bioimaging purposes. Along with the PL, diamond Raman signal (1332 cm-1, phonon mode of sp3-bound carbon) is observed in the spectra. The narrow peaks appear at 572.5 nm (at 532 nm
wavelength laser excitation) and near 340 nm (at 325 nm wavelength laser excitation), but are not the focus for this study. At room temperature, the doublet 1.401/1.404 eV (885/883 nm) is not resolved. With the temperature decreasing to 110 K (see Figure 1 (e)), the peak splits into doublet. Note that we didn't observe the fine structure of the lines, determined by the isotopes (Ni, C) composition [13, 27].
We observed the characteristic emission of ND of different sizes from 100 nm to 2.5 ^m. In Figure 2 (a) the spectra measured with 325 nm wavelength laser excitation at room temperature (normalized to the peak height at 500 nm wavelength) are shown. As seen from the spectra the PL intensity of the 1.4 eV center relative to other color centers is higher when the size of particles is larger. Variability of the emission with ND sizes (as well as with excitation wavelength and temperature) give the possibility to select the most suitable ND to use as a fluorescent probe. In Figure 2 (b) the spectra excited with 325 nm wavelength laser excitation are compared with
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52 СТМ J 2018 — vol. 10, No.1 Y.-C. Lin, L.-W. Tsai, E. Perevedentseva, A. Karmenyan, C.-L. Cheng
Figure 2. Measurements of photoluminescence spectra
(a) Photoluminescence spectra measured with a 325 nm wavelength laser excitation at room temperature. The sizes of nanodiamond are (1) 100 nm, (2) 500 nm, and (3) 25 pm. (b) Photoluminescence spectra measured with a two-photon excitation with femtosecond laser, at 760 nm wavelength at room temperature from 500 nm and 25 pm diamond particles in comparison with one-photon excitation
Figure 3. Laser confocal image and photoluminescence mapping of 500 nm carboxylated nanodiamond with baby hamster kidney cells
(a) Optical image of single cell containing 500 nm carboxylated nanodiamond excited using 488 nm wavelength laser. Photoluminescence mapping of 500 nm carboxylated nanodiamond focused on (b) NV- center (620640 nm) and (c) Ni-related center (885 nm) under 325 nm wavelength laser excitation exposure; each pixel exposure time 0.1 s, total integral time 17 min, scanning area from the red square in (a). Lower photon counts are the cells edges and higher photon counts are the respective centers
the spectra measured with two-photon excitation using a 760 nm wavelength femtosecond laser. The maximum of emission at 883-885 nm coincides at one- and two-photon excitations for both diamond powders of sizes 500 nm and 2.5 pm. However, in the spectrum from 2.5 pm microdiamond additional peaks are observed. Interestingly, that their peaks also can be attributed as Ni-containing defects with luminescence maximums in the 845-855 nm range (or 1.448-1.466 eV, Ni- and O-containing defect) and 996 (1.245 eV) [24]. It has
been shown for the first time that two-photon excited luminescence of Ni-containing defects from diamond nano- and microparticles opens opportunities for further development of these particles.
The fluorescence imaging and mapping (distribution of signal at certain wavelength) are widely used for biological cells and tissues visualization. ND has been proposed as an alternative to fluorescence dye due to its biocompatibility, chemical stability, easy surface modification and functionalization, and useful
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Size (pm)
Figure 4. Laser confocal image and photoluminescence mapping of 500 nm carboxylated nanodiamond with baby hamster kidney cells
(a) Optical image of single cell containing 500 nm carboxylated nanodiamond excited using a 488 nm wavelength laser; (b) photoluminescence of 500 nm carboxylated nanodiamond detects H3 center (495-550 nm); (c) merged images from (a) and (b). (d) Zoom in from the red square in (c). (e) Photoluminescence mapping of Ni-related center (885 nm) under 325 nm wavelength laser excitation exposures; each pixel exposure time 0.1 s, total integral time 17 min. Lower photon counts are the cells edges and higher photon counts are the respective centers
spectroscopic properties [1, 2]. Nitrogen-vacancy centers have been demonstrated to be useful for bioimaging, and the methods to increase the number of NV centers in ND to enhance the fluorescence have also been developed [9]. However, autofluorescence from biological objects overlaps with the emission of NV centers (~500-800 nm); this hinders the observation of using ND for imaging. Using the color centers with emission in red and near-infrared range would be advantageous as alternative to molecular dyes and NV centers fluorescence. In practice, there is indeed the necessity to separate the ND signal from the cell autofluorescence to improve the imaging, delivery tracing, monitoring, and corresponding methods [28]. Imaging using Ni center (1.4 eV system) fluorescence allows separation from autofluorescence.
We tested the possibility of employing Ni color center for bioimaging using fluorescence mapping with 500 nm ND in BHK cells excited with 488 nm wavelength laser. Figure 3 (a) presents the confocal optical image of BHK cells with a single 500 nm ND, detected the N-V-N (H3) color center emission, and collected in the 495 to 550 nm wavelength region. Shown in Figure 3 (b), the NV- center fluorescence collected in the 600800 nm range. In Figure 3 (c), the Ni-related center (885 nm) excited with 325 nm wavelength laser and collected in the 800-1200 nm region of the red square
(see Figure 3 (a)) demonstrating the ND's 1.4 eV defect PL is applicable for bioimaging. When comparing the ND image between using NV-related center and Ni-related one can easily see the advantage of using the near-infrared emission of the Ni-related centers.
In Figure 4, we present the imaging using the 1.4 eV Ni, H3, and NV centers fluorescence. Figure 4 (a) is the confocal image of BHK cells with 500 nm ND, the green color shows the H3 color center emission, collected in 495 to 550 nm wavelength region (Figure 4 (b)) and excited by 488 nm wavelength laser. The distribution of the PL intensity that detects the NV- defect emission is in the 600-800 nm wavelength range with 325 nm wavelength laser excitation, shown in Figure 4 (e). The scanning area is in red square in Figure 4 (c). The combined 1.4 eV defect PL intensity in the 800-1200 nm wavelength range is mapped in Figure 4 (c). Lower photon counts are the cells edges and higher photon counts are the respective centers, demonstrating the ND's 1.4 eV defect PL is more clear for bioprobing than other defect centers of ND. Figure 4 (d) shows the zoom in from the red square in (c). The PL mapping of Ni-related center (885 nm) under 325 nm wavelength laser excitation exposures is displayed in Figure 4 (e). Lower photon counts are the cells edges and higher photon counts are the respective centers. Note that for the bioimaging it represents a major advantage that Ni-related center fluorescence does not overlap with the cell's autofluorescence.
Conclusion
In this work, we study the photoluminescence properties of nanodiamond of various sizes at different condition of temperature and excitation laser wavelength, focusing on the use of Ni-related center which the fluorescence is emitted in the 1.401/1.404 eV (885/883 nm) region. The PL intensity of the 1.4 eV center relative to other color centers is higher when the size of particles is larger. Variability of the emission with ND sizes (as well as with excitation wavelength and temperature) gives the possibility to select the most suitable ND for use as a fluorescent probe. The two-photon excitation of Ni centers luminescence in nano- and microdiamond particles is demonstrated. In terms of the ND applications we demonstrate the possibility to use the Ni color center
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for bioimaging at ambient conditions applying the ND in baby hamster kidney cells. The emission of Ni-related center (885 nm) showing no photo-bleaching and no damage to the baby hamster kidney cells and the location of ND is clearly observed relatively the cells as compared to using NV centers imaging. This demonstrates fluorescence from Ni-related color center at one-photon and two-photon excitation can be an alternative option in biological imaging applications to avoid cell autofluorescence and to shift the excitation in range of higher safety and higher transparency for biological objects.
Acknowledgements. The authors would like to thank the Ministry of Science and Technology of Taiwan for financially supporting this research under Contracts No. MOST 106-2112-M-259-009-MY3.
Conflict of interest. The authors have no conflict of interests to disclose.
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