Optical absorption, induced bleaching, and photoluminescence of CdSe nanoplatelets grown in cadmium octanoate matrix
© Lyashchova et al.; licensee Springer. 2014
Received: 9 December 2013
Accepted: 11 February 2014
Published: 20 February 2014
CdSe nanoparticles (NPs) are chemically synthesized in thermotropic ionic liquid crystalline (LC) phase of cadmium octanoate that was used as a nanoreactor. The nanocomposite samples are obtained by the rapid cooling of the LC phase to room temperature. Observed doublet structure in absorption spectra of the nanocomposites is characteristic for the two-dimensional CdSe nanoplatelets (NPLs). The thicknesses of the CdSe NPLs are 1.6, 1.9 and 2.3 nm as determined from the absorption spectra, and correspond to 4, 5 and 6 CdSe monolayers, respectively. Induced simultaneous bleaching of the doublet components observed under femtosecond laser excitation, as well as photoluminescence spectra and their kinetics are found compatible with the model of excitons with heavy- and light-hole valence bands confined in nanoplatelets.
Many representatives of metal alkanoate salts form the thermotropic ionic liquid crystalline phase that has the structure of the smectic A at relatively high temperatures (about +100°C and higher). The mesophase of metal alkanoates can be used as a nanoreactor for synthesis and stabilization of semiconductor and metal NPs with small dispersion of their sizes. The LC mesophase of pure metal alkanoates, as well as LC mesophase of nanocomposites with NPs, can be supercooled that leads to the subsequent formation of an anisotropic glass at the room temperature, in which the layered structure of the smectic A phase is retained .
Earlier, structural and optical properties of cadmium alkanoate composites with CdS quantum dots have been studied and it was shown that the template-controlled synthesis of semiconductor CdS in metal alkanoate matrix is very promising in creating nanocrystals with small dispersion of their sizes and uniformity on their shapes [2, 3]. They are new perspective materials for many applications including lasers and sensors of near-ultraviolet and blue visible spectral range. It has been found that the thermo-optical nonlinearity of cadmium octanoate composites containing CdSe NPs are characterized by extremely large value of the nonlinear refractive index, n2, under relatively low-powered CW laser irradiation .
As for colloids, progress in synthesis has resulted in methods of formation of CdSe nanostructures with the atomic precision, namely, magic-sized clusters of exact number of constituting atoms  and CdSe nanoplatelets with two-dimensional electronic structure [6, 7]. In the present paper, we discuss optical absorption and photoluminescence properties of CdSe nanocomposites prepared in cadmium octanoate matrix.
The cadmium octanoate (Cd+2(C7H15COO)2-, the abbreviation CdC8) exists in a form of the polycrystalline powder at room temperature. The smectic A mesophase of the cadmium octanoate occurs in the temperature range 98°C to 180°C. CdSe nanoparticles (NPs) are synthesized in cadmium octanoate matrix by the following manner : The polycrystalline powder of CdC8, impregnated with a saturated aqueous-alcoholic solution of the selenourea (starting amount of selenourea is 4 mol%), was held in a furnace (at 100°C, 180°C, or 220°C) in argon atmosphere for 30 min. The size and shape of the CdSe NPs were determined by a certain condition of the synthesis. The synthesized nanocomposites were cooled down to room temperature. As the result, the colored polycrystalline powders of CdC8 with CdSe NPs were obtained. As follows, from the experiments described below, CdSe NPs synthesized in CdC8 at various temperatures (100°C, 180°C, and 220°C) have different sizes.
The samples of glassy nanocomposites are prepared by the following method: The polycrystalline powder of the nanocomposite was placed between two flat quartz substrates. The thickness of the sample was set by a polytetrafluoroethylene stripe (10 or 30 μm). Such cell was heated up to the temperatures of the mesophase. After that, the cell was rapidly cooled down to room temperature, forming the anisotropic glassy nanocomposite .
Details of TEM studies of the samples will be published elsewhere
The absorption spectrum measurements of the CdSe NPLs were carried out with the automated spectral complex KSVU-6 (LOMO). High optical quality of the samples resulted in low scattering level, and allowed us to neglect the scattering.
Measurements of photoluminescence (PL) and PL excitation (PLE) spectra of the nanocomposites were performed by spectrometer, which consisted of two monochromators (LOMO), 100-W tungsten halogen lamp, a photomultiplier tube, and necessary electronics controlled by PC. GaN laser excitation (CW, 406 nm, 75 mW) was employed also for measurements of PL spectra.
For PL kinetics, studies in nano-microsecond time interval, N2 pulsed laser excitation (337 nm, 6 ns, 20 Hz repetition rate, approximately 1 mJ of energy in a pulse) was used. RIGOL DS5202MA digital storage oscilloscope (200 MHz, 1GS/s) acquired signal directly from the PMT, digitized it, fitted the data by exponential decay curve, and, optionally, transferred digitized data to PC for advanced data processing.
Pump-probe measurements of transient absorption were performed at the Center for collective use ‘Laser Femtosecond Complex’ at the Institute of Physics of NASU . The pump pulse parameters were the following: 400 nm, 130 fs, 1 kHz, approximately 10 μJ. The probe pulse was ‘white continuum’ generated in LiF or sapphire plate. The pump and the probe pulses overlapped on the sample. Transient spectrum of the probe was measured by Acton Research SP2500i spectrometer (Princeton Instruments, Trenton, NJ, USA) equipped with a Spec 10 CCD detector.
Results and discussion
The doublets in the absorption spectra prompt to suppose the nanoplatelet shape of the formed CdSe nanoparticles, as it was proposed in the paper . The absorption bands at 366 nm (3.390 eV) and 384 nm (3.221 eV) of sample 1, 430 nm (2.883 eV) and 454 nm (2.731 eV) of sample 2, as well as the bands at 483 nm (2.567 eV) and 514 nm (2.412 eV) of sample 3 can be associated with electron transitions from light-hole (LH) and heavy-hole (HH) energy levels of valence band into the lowest energy level of conduction band, respectively [6, 7]. Corresponding excitons in bulk crystals are known also as B- and A-excitons, respectively.
Calculated thicknesses of CdSe NPLs
Supposed number of CdSe monolayers
From eHH-exciton band position
From eLH-exciton band position
Formation of the nanoplatelet shape CdSe nanoparticles in the thermotropic ionic liquid crystalline phase of cadmium octanoate is confirmed by the doublet in the absorption spectrum, simultaneous to the induced bleaching of its components, as well as by photoluminescence properties. The two sharp peaks of optical absorption can be associated with electron transitions from light-hole and heavy-hole energy levels of valence band into the lowest energy level of conduction band. Thanks to the large oscillator strength of optical transitions and huge nonlinearity, these CdSe NPL nanocomposites are new perspective materials for many applications.
The work has been funded in part by the projects of the state target scientific and technical program ‘Nanotechnologies and Nanomaterials’ for 2010 to 2014 years (No. 188.8.131.52, 184.108.40.206).
- Mirnaya TA, Volkov SV: Ionic liquid crystals as universal matrices (solvents): main criteria for ionic mesogenicity. In Green industrial application of ionic liquids. Edited by: Rogers RD, Seddon KR, Volkov SV. London: Kluwer Academic Publishers; 2002:439–456.Google Scholar
- Mirnaya TA, Asaula VN, Volkov SV, Tolochko AS, Melnik DA, Klimusheva GV: Synthesis and optical properties of liquid crystalline nanocomposites of cadmium octanoate with CdS quantum dots. J Phys Chem Solid State 2012, 13: 131–135.Google Scholar
- Klimusheva G, Dmitruk I, Mirnaya T, Tololchko A, Bugaychuk S, Naumenko A, Melnik D, Asaula V: Monodispersity and ordering of semiconductor quantum dots synthesized in ionic liquid crystalline phase of cadmium alkanoates. Liq Cryst 2013, 40: 980–988. 10.1080/02678292.2013.786794View ArticleGoogle Scholar
- Lyashchova A, Fedorenko D, Garbovskiy Y, Klimusheva G, Mirnaya T, Asaula V: Strong thermal optical nonlinearity caused by CdSe nanoparticles synthesised in smectic ionic liquid crystal. Liq Cryst 2013, 40: 1377–1382. 10.1080/02678292.2013.811548View ArticleGoogle Scholar
- Kasuya A, Sivamohan R, Barnakov Y, Dmitruk I, Nirasawa T, Romanyuk VR, Kumar V, Mamykin SV, Tohji K, Jeyadevan B, Shinoda K, Kudo T, Terasaki O, Liu Z, Belosludov RV, Sundararajan V, Kawazoe Y: Ultra-stable nanoparticles of CdSe revealed from mass spectrometry. Nat Mater 2004, 3: 99–102. 10.1038/nmat1056View ArticleGoogle Scholar
- Ithurria S, Dubertret S: Quasi 2D colloidal CdSe platelets with thicknesses controlled at the atomic level. J Am Chem Soc 2008, 130: 16504–16505. 10.1021/ja807724eView ArticleGoogle Scholar
- Ithurria S, Tessier MD, Mahler B, Lobo RPS, Dubertret N, Efros AL: Colloidal nanoplatelets with two-dimensional electronic structure. Nat Mater 2011, 10: 936–941. 10.1038/nmat3145View ArticleGoogle Scholar
- Blonskii IV, Dmitruk IM, Kadan VM, et al.: Time-separated methods for femto photonic nanostructures. Nanosyst, Nanomater, Nanotechnolo 2008, 6: 45–47.Google Scholar
- Landau LD, Lifshitz EM: Theoretical Physics: Quantum Mechanics (Non-relativistic Theory). Moscow: Nauka; 1989.Google Scholar
- Norris DJ, Bawendi MG: Measurement and assignment of the size-dependent optical spectrum in CdSe quantum dots. Phys Rev B 1996, 53: 16338–16346. 10.1103/PhysRevB.53.16338View ArticleGoogle Scholar
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.