97 research outputs found
Electron and hole g-factors and spin dynamics of negatively charged excitons in CdSe/CdS colloidal nanoplatelets with thick shells
We address spin properties and spin dynamics of carriers and charged excitons
in CdSe/CdS colloidal nanoplatelets with thick shells. Magneto-optical studies
are performed by time-resolved and polarization-resolved photoluminescence,
spin-flip Raman scattering and picosecond pump-probe Faraday rotation in
magnetic fields up to 30 T. We show that at low temperatures the nanoplatelets
are negatively charged so that their photoluminescence is dominated by
radiative recombination of negatively charged excitons (trions). Electron
g-factor of 1.68 is measured and heavy-hole g-factor varying with increasing
magnetic field from -0.4 to -0.7 is evaluated. Hole g-factors for
two-dimensional structures are calculated for various hole confining potentials
for cubic- and wurtzite lattice in CdSe core. These calculations are extended
for various quantum dots and nanoplatelets based on II-VI semiconductors. We
developed a magneto-optical technique for the quantitative evaluation of the
nanoplatelets orientation in ensemble
Addressing the exciton fine structure in colloidal nanocrystals: the case of CdSe nanoplatelets
We study the band-edge exciton fine structure and in particular its
bright-dark splitting in colloidal semiconductor nanocrystals by four different
optical methods based on fluorescence line narrowing and time-resolved
measurements at various temperatures down to 2 K. We demonstrate that all these
methods provide consistent splitting values and discuss their advances and
limitations. Colloidal CdSe nanoplatelets with thicknesses of 3, 4 and 5
monolayers are chosen for experimental demonstrations. The bright-dark
splitting of excitons varies from 3.2 to 6.0 meV and is inversely proportional
to the nanoplatelet thickness. Good agreement between experimental and
theoretically calculated size dependence of the bright-dark exciton slitting is
achieved. The recombination rates of the bright and dark excitons and the
bright to dark relaxation rate are measured by time-resolved techniques
Intervalley Scattering of Interlayer Excitons in a MoS/MoSe/MoS Heterostructure in High Magnetic Field
Degenerate extrema in the energy dispersion of charge carriers in solids,
also referred to as valleys, can be regarded as a binary quantum degree of
freedom, which can potentially be used to implement valleytronic concepts in
van der Waals heterostructures based on transition metal dichalcogenides. Using
magneto-photoluminescence spectroscopy, we achieve a deeper insight into the
valley polarization and depolarization mechanisms of interlayer excitons formed
across a MoS/MoSe/MoS heterostructure. We account for the
non-trivial behavior of the valley polarization as a function of the magnetic
field by considering the interplay between exchange interaction and phonon
mediated intervalley scattering in a system consisting of Zeeman-split energy
levels. Our results represent a crucial step towards the understanding of the
properties of interlayer excitons, with strong implications for the
implementation of atomically thin valleytronic devices.Comment: just accepted in Nano Letters, DOI: 10.1021/acs.nanolett.8b0148
Site-selective measurement of coupled spin pairs in an organic semiconductor
From organic electronics to biological systems, understanding the role of
intermolecular interactions between spin pairs is a key challenge. Here we show
how such pairs can be selectively addressed with combined spin and optical
sensitivity. We demonstrate this for bound pairs of spin-triplet excitations
formed by singlet fission, with direct applicability across a wide range of
synthetic and biological systems. We show that the site-sensitivity of exchange
coupling allows distinct triplet pairs to be resonantly addressed at different
magnetic fields, tuning them between optically bright singlet (S=0) and dark
triplet, quintet (S=1,2) configurations: this induces narrow holes in a broad
optical emission spectrum, uncovering exchange-specific luminescence. Using
fields up to 60 T, we identify three distinct triplet-pair sites, with exchange
couplings varying over an order of magnitude (0.3-5 meV), each with its own
luminescence spectrum, coexisting in a single material. Our results reveal how
site-selectivity can be achieved for organic spin pairs in a broad range of
systems.Comment: 8 pages, article, 7 pages, supporting informatio
Zeeman Splitting and Inverted Polarization of Biexciton Emission in Monolayer WS2
Atomically thin semiconductors provide an ideal testbed to investigate the physics of Coulomb-bound many-body states. We shed light on the intricate structure of such complexes by studying the magnetic-field-induced splitting of biexcitons in monolayer WS2 using polarization-resolved photoluminescence spectroscopy in out-of-plane magnetic fields up to 30 T. The observed g factor of the biexciton amounts to about -3.9, closely matching the g factor of the neutral exciton. The biexciton emission shows an inverted circular field-induced polarization upon linearly polarized excitation; i.e., it exhibits preferential emission from the high-energy peak in a magnetic field. This phenomenon is explained by taking into account the hybrid configuration of the biexciton constituents in momentum space and their respective energetic behavior in magnetic fields. Our findings reveal the critical role of dark excitons in the composition of this many-body state
Hole and electron effective masses in single InP nanowires with a Wurtzite-Zincblende homojunction
The formation of wurtzite (WZ) phase in III–V nanowires (NWs) such as GaAs and InP is a complication hindering the growth of pure-phase NWs, but it can also be exploited to form NW homostructures consisting of alternate zincblende (ZB) and WZ segments. This leads to different forms of nanostructures, such as crystal-phase superlattices and quantum dots. Here, we investigate the electronic properties of the simplest, yet challenging, of such homostructures: InP NWs with a single homojunction between pure ZB and WZ segments. Polarization-resolved microphotoluminescence (μ-PL) measurements on single NWs provide a tool to gain insights into the interplay between NW geometry and crystal phase. We also exploit this homostructure to simultaneously measure effective masses of charge carriers and excitons in ZB and WZ InP NWs, reliably. Magneto-μ-PL measurements carried out on individual NWs up to 29 T at 77 K allow us to determine the free exciton reduced masses of the ZB and WZ crystal phases, showing the heavier character of the WZ phase, and to deduce the effective mass of electrons in ZB InP NWs (me= 0.080 m0). Finally, we obtain the reduced mass of light-hole excitons in WZ InP by probing the second optically permitted transition Γ7C ↔ Γ7uV with magneto-μ-PL measurements carried out at room temperature. This information is used to extract the experimental light-hole effective mass in WZ InP, which is found to be mlh = 0.26 m0, a value much smaller than the one of the heavy hole mass. Besides being a valuable test for band structure calculations, the knowledge of carrier masses in WZ and ZB InP is important in view of the optimization of the efficiency of solar cells, which is one of the main applications of InP NWs
Exciton-phonon coupling in InP quantum dots with ZnS and (Zn, Cd) Se shells
InP-based colloidal quantum dots are promising for optoelectronic devices such as light-emitting diodes and lasers. Understanding and optimizing their emission process is of scientific interest and essential for large-scale applications. Here we present a study of the exciton recombination dynamics in InP QDs with various shells: ZnS, ZnSe, and (Zn,Cd)Se with different amounts of Cd (5, 9, 12%). Phonon energies extracted from Raman spectroscopy measurements at cryogenic temperatures (4-5 K) are compared with exciton emission peaks observed in fluorescence line narrowing spectra. This allowed us to determine the position of both the bright F = +/- 1 state and the lowest dark F = +/- 2 state. We could identify the phonon modes involved in the radiative recombination of the dark state and found that acoustic and optical phonons of both the core and the shell are involved in this process. The Cd content in the shell increases electron wave-function delocalization, and thereby enhances the exciton-phonon coupling through the Frohlich interaction
Room Temperature Optically and Magnetically Active Edges in Phosphorene Nanoribbons
Nanoribbons - nanometer wide strips of a two-dimensional material - are a
unique system in condensed matter physics. They combine the exotic electronic
structures of low-dimensional materials with an enhanced number of exposed
edges, where phenomena including ultralong spin coherence times, quantum
confinement and topologically protected states can emerge. An exciting prospect
for this new material concept is the potential for both a tunable
semiconducting electronic structure and magnetism along the nanoribbon edge.
This combination of magnetism and semiconducting properties is the first step
in unlocking spin-based electronics such as non-volatile transistors, a route
to low-energy computing, and has thus far typically only been observed in doped
semiconductor systems and/or at low temperatures. Here, we report the magnetic
and semiconducting properties of phosphorene nanoribbons (PNRs). Static (SQUID)
and dynamic (EPR) magnetization probes demonstrate that at room temperature,
films of PNRs exhibit macroscopic magnetic properties, arising from their edge,
with internal fields of ~ 250 to 800 mT. In solution, a giant magnetic
anisotropy enables the alignment of PNRs at modest sub-1T fields. By leveraging
this alignment effect, we discover that upon photoexcitation, energy is rapidly
funneled to a dark-exciton state that is localized to the magnetic edge and
coupled to a symmetry-forbidden edge phonon mode. Our results establish PNRs as
a unique candidate system for studying the interplay of magnetism and
semiconducting ground states at room temperature and provide a stepping-stone
towards using low-dimensional nanomaterials in quantum electronics.Comment: 18 pages, 4 figure
An unforeseen polymorph of coronene by the application of magnetic fields during crystal growth
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