Colloidal III–V Nitride Quantum Dots

Colloidal quantum dots (QDs) have attracted intense attention in both fundamental studies and practical applications. To date, the size, morphology, and composition-controlled syntheses have been successfully achieved in II–VI semiconductor nanocrystals. Recently, III-nitride semiconductor quantum dots have begun to draw significant interest due to their promising applications in solid-state lighting, lasing technologies, and optoelectronic devices. The quality of nitride nanocrystals is, however, dramatically lower than that of II–VI semiconductor nanocrystals. In this review, the recent development in the synthesis techniques and properties of colloidal III–V nitride quantum dots as well as their applications are introduced

Exciton-optical phonon coupling in II-VI semiconductor nanocrystals.

This perspective reviews the topic of exciton-phonon coupling (EPC) in II-VI semiconductor nanocrystals. First, EPC is defined and its relevance is discussed, both as it influences the properties of the materials relevant to applications and as a probe of electronic structure. Different experimental and theoretical methods for probing EPC are outlined. Results for several different classes of II-VI nanocrystals are summarized. Finally, possible future directions are outlined

Evolution of the electronic structure with size in II-VI semiconductor nanocrystals

In order to provide a quantitatively accurate description of the band gap variation with sizes in various II-VI semiconductor nanocrystals, we make use of the recently reported tight-binding parametrization of the corresponding bulk systems. Using the same tight-binding scheme and parameters, we calculate the electronic structure of II-VI nanocrystals in real space with sizes ranging between 5 and 80 {\AA} in diameter. A comparison with available experimental results from the literature shows an excellent agreement over the entire range of sizes.Comment: 17 pages, 4 figures, accepted in Phys. Rev.

Understanding the Magnetic Properties of II-VI Semiconductor Nanocrystals

Semiconductor nanocrystals (NC) are well known for their unique size tunable optical properties making them suitable candidates for devices such as light emitting diodes (LEDs), solar cells, and cellular labels. II-VI semiconductors in the bulk form behave diamagnetically, but can inherit paramagnetic (PM) or ferromagnetic (FM) properties at the nanoscale. Reports suggest that the emergence of weak PM or FM behavior in undoped NCs are attributed to the increased surface to volume ratio compared for NCs. Traditionally, these NCs only obtain magnetic properties after doping with certain transition metals, such as Co, Mn, or Fe. Many mechanisms have been proposed to determine the source of magnetism in undoped NCs, ranging from dangling bonds, surface vacancies, and ligand exchange interactions. This thesis focuses on the role of dangling bonds and atomic vacancies on the surface of colloidal CdSe and ZnO NCs via controlled ligand removal along with CdS and CdS/ZnS core/shell nanoplatelets doped with Mn. Through magnetic measurements we show that for CdSe and ZnO NCs, the surface ligand density can drastically affect the magnetization results through a liquid phase post processing technique. For CdSe NCs the exact source of magnetism is complex and can arise from the uncoordinated surface atoms as seen with varying total angular momentum, J, values. In general, modification of magnetism in ZnO NCs can be attributed to the formation of oxygen vacancies as seen from consistent J values. Lastly, CdS and CdS/ZnS NPLs inherently possess surface defects, such as Cd or Zn vacancies, which coupled with Mn dopants can promote strong spin coupling between the core and NC surface

Special issue “II-VI semiconductor nanocrystals and hybrid polymer–nanocrystal systems”

: The continuous need to improve the performance of photonic, electronic and optoelectronic devices has stimulated research toward the development of innovative semiconducting materials which display better properties with respect to standard bulk semiconductors [...]

Photovoltaic Performance of Ultrasmall PbSe Quantum Dots

We investigated the effect of PbSe quantum dot size on the performance of Schottky solar cells made in an ITO/PEDOT/PbSe/aluminum structure, varying the PbSe nanoparticle diameter from 1 to 3 nm. In this highly confined regime, we find that the larger particle bandgap can lead to higher open-circuit voltages (~0.6 V), and thus an increase in overall efficiency compared to previously reported devices of this structure. To carry out this study, we modified existing synthesis methods to obtain ultrasmall PbSe nanocrystals with diameters as small as 1 nm, where the nanocrystal size is controlled by adjusting the growth temperature. As expected, we find that photocurrent decreases with size due to reduced absorption and increased recombination, but we also find that the open-circuit voltage begins to decrease for particles with diameters smaller than 2 nm, most likely due to reduced collection efficiency. Owing to this effect, we find peak performance for devices made with PbSe dots with a first exciton energy of ~1.6 eV (2.3 nm diameter), with a typical efficiency of 3.5%, and a champion device efficiency of 4.57%. Comparing the external quantum efficiency of our devices to an optical model reveals that the photocurrent is also strongly affected by the coherent interference in the thin film due to Fabry-Pérot cavity modes within the PbSe layer. Our results demonstrate that even in this simple device architecture, fine-tuning of the nanoparticle size can lead to substantial improvements in efficiency

Energy Transfer Dynamics and Dopant Luminescence in Mn-Doped CdS/ZnS Core/Shell Nanocrystals

Mn-doped II-VI semiconductor nanocrystals exhibit bright dopant photoluminescence that has potential usefulness for light emitting devices, temperature sensing, and biological imaging. The bright luminescence comes from the 4T1→6A1 transition of the Mn2+ d electrons after the exciton-dopant energy transfer, which reroutes the exciton relaxation through trapping processes. The driving force of the energy transfer is the strong exchange coupling between the exciton and Mn2+ due to the confinement of exciton in the nanocrystal. The exciton-Mn spatial overlap affecting the exchange coupling strength is an important parameter that varies the energy transfer rate and the quantum yield of Mn luminescence. In this dissertation, this correlation is studied in radial doping location-controlled Mn-doped CdS/ZnS nanocrystals. Energy transfer rate was found decreasing when increasing the doping radius in the nanocrystals at the same core size and shell thickness and when increasing the size of the nanocrystals at a fixed doping radius. In addition to the exciton-Mn energy transfer discussed above, two consecutive exciton-Mn energy transfers can also occur if multiple excitons are generated before the relaxation of Mn (lifetime ~10^-4 - 10^-2 s). The consecutive exciton-Mn energy transfer can further excite the Mn2+ d electrons high in conduction band and results in the quenching of Mn luminescence. The highly excited electrons show higher photocatalytic efficiency than the electrons in undoped nanocrystals. Finally, the effect of local lattice strain on the local vibrational frequency and local thermal expansion was observed via the temperature-dependent Mn luminescence spectral linewidth and peak position in Mn-doped CdS/ZnS nanocrystals. The local lattice strain on the Mn2+ ions is varied using the large core/shell lattice mismatch (~7%) that creates a gradient of lattice strain at various radial locations. When doping the Mn2+ closer to the core/shell interface, the stronger lattice strain softens the vibrational frequency coupled to the 4T1→6A1 transition of Mn2+ (Mn luminescence) by ~50%. In addition, the lattice strain also increases the anharmonicity, resulting in larger local thermal expansion observed from the nearly an order larger thermal shift of the Mn luminescence compared to the Mn-doped ZnS nanocrystals without the core/shell lattice mismatch

Plasmonic Enhancement of Mn2+ Luminescence and Application of Temperature-Dependent Mn2+ Luminescence

Doping semiconductor nanocrystals, commonly known as quantum dots (QDs), has attracted significant attention from the scientific community due to the highly tunable nature of the physical properties, such as optical, electrical, opto-magnetic properties, with respect to both size and dopant type/concentration. In this dissertation, Mn-doped CdS/ZnS (core/shell) QDs were used as a model system to study the characteristics of dopant luminescence coupled with plasmonic metal nanoparticles (MNPs) and its application as a nano-thermometer using temperature dependent Mn luminescence. In the first part of this dissertation, plasmon-enhanced Mn luminescence from the Mn-doped CdS/ZnS QDs near plasmonic MNPs was studied. Rapid intraparticle energy transfer between exciton and Mn, occurring on a few picoseconds time scale, separates the absorber (exciton) from the emitter (Mn), whose emission is detuned far from the plasmonic absorption of the MNP. The rapid temporal separation of the absorber and emitter combined with the reduced spectral overlap between Mn and plasmonic MNP suppresses the quenching of the luminescence while taking advantage of the plasmon-enhanced excitation. The plasmon enhancement of exciton and Mn luminescence intensities in undoped and doped QDs were simultaneously compared as a function of the distance between MNP and QD layers in a multilayer structure to examine the expected advantage of the reduced quenching in the sensitized luminescence. At the optimum MNP-QD layer distance, Mn luminescence exhibits stronger net enhancement (ca. twice) than that of the exciton, which can be explained with a model incorporating fast sensitization along with reduced emitter-MNP spectral overlap. In the second part, ratiometric thermometry on Mn luminescence spectrum was performed using Mn-doped CdS/ZnS core/shell QDs that have a large local lattice strain on Mn site, which results in the enhanced temperature dependence of the bandwidth and peak position. Mn luminescence spectral lineshape is highly robust with respect to the change in the polarity, phase and pH of the surrounding medium and aggregation of the QDs, showing great potential in temperature imaging under chemically heterogeneous environment. The temperature sensitivity (ΔIR/IR = 0.5%/K at 293 K, IR = intensity ratio at two different wavelengths) is highly linear in a wide range of temperatures from cryogenic to above-ambient temperatures. Surface temperature imaging was demonstrated on a cryo-cooling device showing the temperature variation of ~200 K (77–260 K) by imaging the luminescence of the QD film formed by simple spin coating, taking advantage of the environment-insensitive luminescence

Colloidal Synthesis of I-III-VI Semiconductor Nanocrystals and Study of Their Optical Properties

Semiconductor nanocrystals (NCs) have emerged as promising fluorophores in a plethora of applications including lighting and display technologies. Cd/Pb-chalcogenide-based NCs are by far the most studied classes of semiconductor NCs due to their exemplary luminescence properties. However, their toxicity poses a limit to their widespread application and use in biological systems, nanomedicine, as biomarkers, etc. Therefore, the search for alternatives that can replace Cd/Pb-chalcogenide-based NCs as fluorophores in various applications is a topic of rigorous research. This PhD thesis delves into the development of synthetic strategies for one such class of materials that can potentially replace Cd/Pb-chalcogenide-based NCs in various applications. I-III-VI semiconductor NCs, containing earth abundant metals which are comparatively less toxic than Cd and Pb have emerged as a suitable alternative. In this group, Cu-In-S/Se (CIS/Se) based NCs have gained significant interest due to their nontoxic nature and interesting optical properties. The principal aim of this thesis is to develop synthetic strategies to obtain morphologically vivid CIS/Se NCs and study their optical properties. Due to the multiple reactive species present in ternary /quaternary NCs, direct method of synthesis wherein all precursors are reacted at the same time exhibit problems of inhomogeneous size, shape, and compositions, along with binary byproducts formed in addition to the desired ternary/quaternary NCs. In view of this limitation of direct method of synthesis, a cation exchange (CE) pathway of synthesis has been developed. In this approach, a binary NC is first synthesized using a conventional direct method, which then serves as a host lattice for the incoming third or fourth cation thus leading to the synthesis of ternary or quaternary multicomponent NCs. Employing this route enables the preservation of the morphology and crystal structure of the host NC after the exchange process, leading to better control over size, shape, and composition of the desired NCs. In this thesis, 0D spherical Cu-Zn-In-Se (CZISe) NCs were synthesized using a CE approach starting with binary Cu2-xSe NCs and thereafter the composition dependence of their optical properties was studied. The synthesized quaternary CZISe NCs exhibited intensive tuneable photoluminescence (PL) in the near infrared (NIR) range and narrow PL band widths in comparison to the band widths generally observed in this class of materials. Long-chain organic ligands on the surface of colloidal NCs limit carrier mobility, and hence surface modification of the NCs becomes necessary for applications where carrier mobility is an important aspect, e.g., in solar cell fabrication. Thus, surface modification of the synthesized CZISe NCs was also explored to make the NCs compatible for prospective applications of solar energy harvesting. In addition to 0D NCs, two-dimensional (2D) NCs have gained significant interest due to their unique anisotropic optical properties. For example, extremely narrow PL band widths were exhibited for CdSe nanoplatelets (NPLs) due to the strong confinement of the NPLs in the thickness direction. These 2D NCs have also been utilized in a wide array of applications, particularly in thin film photovoltaics and optoelectronics, and therefore investigation of 2D morphologies of I-III-VI based NCs is also of utmost interest. In this thesis, 2D Cu-Zn-In-S (CZIS) NPLs were synthesized which exhibited rectangular morphology and were unstacked due to the synthetic strategy employed. CIS NPLs were synthesized using a seed-mediated approach and a subsequent CE with Zn enabled the synthesis of CZIS NPLs. Subsequently, a ZnS shell growth leading to the formation of CZIS/ZnS NPLs resulted in the enhancement of PL intensity. As compared to 2D CIS NCs the Se counterpart is less studied and very few reports of 2D CISe-based NCs are present in literature and the reported 2D CISe based NCs have not exhibited any PL. Due to the narrower band gap of CISe than CIS, it is possible to push the PL into the NIR range which unlocks new applications and therefore developing synthetic strategies for 2D CISe based NCs which exhibit PL in the NIR range was also explored in this synthesis. CISe NPLs were synthesized using a similar seed-mediated approach used for CIS NPLs, but the difference in reactivities of S and Se required significant optimization of the synthesis parameters. A subsequent CE with Zn resulted in the synthesis of CZISe NPLs with inherent PL in the NIR range with very narrow PL band widths