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1                             For example, the quantum-confined 2D electronic structure aligns the exci
2              Here we report the synthesis of quantum confined all inorganic cesium lead halide nanopl
3 ystem is a means to include two discretized, quantum-confined, and complimentary semiconductor units
4                                              Quantum-confined Au nanoclusters exhibit molecule-like p
5    Together with the signatures of intrinsic quantum-confined bandgaps and high conductivities, our d
6 lectronic and spintronic properties, notably quantum-confined bandgaps and magnetic edge states.
7 he dynamics of multiple electron transfer in quantum confined CdS nanorods with a Pt tip, in which th
8 lloidal quantum shells (g-QSs), comprising a quantum-confined CdSe shell grown over a large (~14 nm)
9 ties and band energy structure, leading to a quantum-confined composite material with unique characte
10 ng confirms that the PL originating from the quantum confined core states can only exist in the red/n
11 s, affect the circular dichroism of strongly quantum confined CsPbBr(3) nanocrystals.
12                                              Quantum-confined devices that manipulate single electron
13 ties of silicon nanowires with the effective quantum-confined dimension remains challenging.
14 ning this method with optical NMR, we imaged quantum-confined electron density in an individual AlGaA
15 ment of layered Sr2 IrO4 induces distinct 1D quantum-confined electronic states, as observed from opt
16 ficial atoms have large dipole moments and a quantum confined energy level structure, enabling the re
17 vercoming these challenges is to make use of quantum-confined excitonic emission in silicon nanocryst
18 conductor QDs allow realization of LSPRs and quantum-confined excitons within the same nanostructure,
19          Our observations demonstrate that a quantum-confined extrinsic electron in a semiconductor c
20  soluble and monodisperse particles that are quantum-confined in two of their dimensions.
21 to measure stimulated-emission efficiency in quantum confined inorganic perovskite CsPbBr(3) NCs, the
22                        The colocalization of quantum-confined interlayer excitons and terahertz inter
23 t exciton transition and the appearance of a quantum-confined, low-energy intraband absorption featur
24  alignment among the bands of these variably quantum confined materials remains a controversial topic
25 of novel thermoelectric properties from such quantum-confined materials, in which the boundary scatte
26                                              Quantum-confined nanoclusters can be described by the je
27                            These ultrasmall, quantum-confined nanoclusters function as highly sensiti
28 tum number to describe the band structure in quantum-confined nanocrystalline systems, which blur the
29  to understand electrical doping in strongly quantum-confined nanocrystals.
30      We discuss the electronic properties of quantum-confined nanocrystals.
31                                    Colloidal quantum confined nanoheterostructures have emerged as pr
32 ntrolling the composition, size and shape of quantum-confined nanoheterostructures, the electron and
33                                          For quantum-confined nanomaterials, size dispersion causes a
34                                              Quantum-confined nanostructures are considered 'artifici
35 hasing, all of which are consistent with the quantum confined nature of the moire excitons.
36 rsistent incorporation of electrons into the quantum-confined NC states.
37                               DEP bridges of quantum confined NPs can be used in fast parallel manufa
38 how that the as-prepared aerogels retain the quantum-confined optical properties of the nanoparticle
39 onoliths, and demonstrate the characteristic quantum-confined optical properties of their nanoparticl
40 control and subangstrom smooth layers enable quantum-confined photoluminescence of CsPbBr(3) from mon
41 ansfer interaction between the more strongly quantum-confined QD conduction band and catalyst LUMO le
42 ultiexciton dissociation from these strongly quantum confined QDs, consistent with recent reports of
43                       We observe that in the quantum-confined regime, the Auger constant is strongly
44                                   Similar to quantum-confined, semiconducting quantum dots, the elect
45 onstrate the proof of concept for the use of quantum confined semiconductor nanocrystals as photoinit
46                  The properties of colloidal quantum-confined semiconductor nanocrystals (NCs), inclu
47                                           In quantum-confined semiconductor nanostructures, electrons
48                                  In bulk and quantum-confined semiconductors, magneto-optical studies
49 nding of structure-property relationships in quantum-confined semiconductors.
50                   Although light emission in quantum-confined silicon at sub-10 nm lengthscales has b
51 e and controls nanocrystal growth within the quantum confined size range.
52 n the dephasing dynamics of the exciton in a quantum-confined, solid-state system.
53 , offer novel prospects to engineer coherent quantum confined spins(8,9), tunnel barriers down to the
54 by enables additional degrees of control for quantum-confined spintronic devices.
55  hetero-NRs, including enhanced magnitude of quantum confined Stark effect and subnanosecond switchin
56 eases from 10 to 100 mA, indicating that the quantum confined Stark effect is effectively suppressed
57 P and their alloys exhibit the much stronger quantum-confined Stark effect (QCSE) mechanism, which al
58 lation strategy, the simulation results of a quantum-confined Stark effect (QCSE) stack waveguide cou
59                                          The quantum-confined Stark effect actively modulates this vo
60  including Auger recombination rates, of the quantum-confined Stark effect in membrane-embedded semic
61                                          The quantum-confined Stark effect in single cadmium selenide
62 oluminescence emission is nearly free of the quantum-confined Stark effect, which is significant for
63 exciton - an effect opposite to conventional quantum-confined Stark shift.
64 mechanical tunnelling of particles between a quantum confined state and a nearby Fermi reservoir of d
65 lloids can be made n-type, with electrons in quantum confined states.
66          The injection of electrons into the quantum-confined states of the nanocrystal leads to an e
67 ution from carrier hopping through localized quantum-confined states to band-like charge transport in
68 resonant stimulated Raman scattering between quantum-confined states within the active region of a qu
69              It traps the Dirac electrons in quantum-confined states, which are the graphene equivale
70      Here we present a technique that builds quantum-confined structures in suspended bilayer graphen
71 nets, lithographic patterning techniques, or quantum-confined structures.
72 oids suitable for subsequent processing into quantum-confined superstructures, materials, and devices
73 iency of this effect remain controversial in quantum-confined systems like semiconductor nanocrystals
74 e report that, counterintuitive to classical quantum-confined systems where photogenerated electrons
75 ling strengths at the nanoscale, even in non-quantum-confined systems, to values much higher than in
76  of the governing excitonic physics of these quantum-confined systems.
77 cost-effective, solution-based deposition of quantum-confined thin films for optoelectronics.
78                                            A quantum confined transport based on a zinc oxide composi
79 g(x)O nanocrystals to smaller (more strongly quantum confined) ZnO nanocrystals.