ライフサイエンスコーパス: quantum-confined

1 Here we report the synthesis of quantum confined all inorganic cesium lead halide nanopl

2 ystem is a means to include two discretized, quantum-confined, and complimentary semiconductor units

3 Together with the signatures of intrinsic quantum-confined bandgaps and high conductivities, our d

4 lectronic and spintronic properties, notably quantum-confined bandgaps and magnetic edge states.

5 ties and band energy structure, leading to a quantum-confined composite material with unique characte

6 ng confirms that the PL originating from the quantum confined core states can only exist in the red/n

7 Quantum-confined devices that manipulate single electron

8 ning this method with optical NMR, we imaged quantum-confined electron density in an individual AlGaA

9 ment of layered Sr2 IrO4 induces distinct 1D quantum-confined electronic states, as observed from opt

10 vercoming these challenges is to make use of quantum-confined excitonic emission in silicon nanocryst

11 conductor QDs allow realization of LSPRs and quantum-confined excitons within the same nanostructure,

12 Our observations demonstrate that a quantum-confined extrinsic electron in a semiconductor c

13 soluble and monodisperse particles that are quantum-confined in two of their dimensions.

14 t exciton transition and the appearance of a quantum-confined, low-energy intraband absorption featur

15 of novel thermoelectric properties from such quantum-confined materials, in which the boundary scatte

16 to understand electrical doping in strongly quantum-confined nanocrystals.

17 Colloidal quantum confined nanoheterostructures have emerged as pr

18 ntrolling the composition, size and shape of quantum-confined nanoheterostructures, the electron and

19 Quantum-confined nanostructures are considered 'artifici

20 rsistent incorporation of electrons into the quantum-confined NC states.

21 DEP bridges of quantum confined NPs can be used in fast parallel manufa

22 how that the as-prepared aerogels retain the quantum-confined optical properties of the nanoparticle

23 onoliths, and demonstrate the characteristic quantum-confined optical properties of their nanoparticl

24 ultiexciton dissociation from these strongly quantum confined QDs, consistent with recent reports of

25 We observe that in the quantum-confined regime, the Auger constant is strongly

26 In bulk and quantum-confined semiconductors, magneto-optical studies

27 nding of structure-property relationships in quantum-confined semiconductors.

28 Although light emission in quantum-confined silicon at sub-10 nm lengthscales has b

29 e and controls nanocrystal growth within the quantum confined size range.

30 n the dephasing dynamics of the exciton in a quantum-confined, solid-state system.

31 by enables additional degrees of control for quantum-confined spintronic devices.

32 hetero-NRs, including enhanced magnitude of quantum confined Stark effect and subnanosecond switchin

33 P and their alloys exhibit the much stronger quantum-confined Stark effect (QCSE) mechanism, which al

34 including Auger recombination rates, of the quantum-confined Stark effect in membrane-embedded semic

35 The quantum-confined Stark effect in single cadmium selenide

36 lloids can be made n-type, with electrons in quantum confined states.

37 The injection of electrons into the quantum-confined states of the nanocrystal leads to an e

38 ution from carrier hopping through localized quantum-confined states to band-like charge transport in

39 resonant stimulated Raman scattering between quantum-confined states within the active region of a qu

40 It traps the Dirac electrons in quantum-confined states, which are the graphene equivale

41 Here we present a technique that builds quantum-confined structures in suspended bilayer graphen

42 nets, lithographic patterning techniques, or quantum-confined structures.

43 oids suitable for subsequent processing into quantum-confined superstructures, materials, and devices

44 iency of this effect remain controversial in quantum-confined systems like semiconductor nanocrystals

45 e report that, counterintuitive to classical quantum-confined systems where photogenerated electrons

46 ling strengths at the nanoscale, even in non-quantum-confined systems, to values much higher than in

47 of the governing excitonic physics of these quantum-confined systems.

48 cost-effective, solution-based deposition of quantum-confined thin films for optoelectronics.

49 g(x)O nanocrystals to smaller (more strongly quantum confined) ZnO nanocrystals.