band gap (E g ) of 1.35 eV (at 300 K) and excitonic Bohr radius of 9.6 nm can afford most part of visible colors by means of size-mediated quantum confinement effects. Typical InP core sizes for green and red color are 2.2 ± 0.2 and 3.6 ± 0.2 nm, respectively, although the final PL wavelength becomes sensitively dependent on core/shell heterostructural details. Meanwhile, synthesis of highquality blue-emitting InP QDs is relatively challenging, being associated with their tiny core sizes well below 2 nm, usually resulting in only quasi-blue color (>475 nm in PL peak) beyond deep-blue territory (450−465 nm). [4,5] Therefore, InP QDs are regarded as the strongest candidates for green and red color, while blue emitters can be pursued from either ternary InGaP [6] or non-InP ZnSeTe QDs. [7][8][9] Earlier synthesis of InP QDs was implemented with a primitive heterostructure mostly based on single ZnS shell. Despite a great deal of effort toward bright, sharp emissivity, the resulting single-shelled InP/ ZnS QDs yielded only moderate PL outcomes (e.g., <80% in PLQY, >45 nm in FWHM). [10][11][12] Such limited PL performances are unambiguously ascribable to the substantial interfacial strain developed from a large InP−ZnS lattice mismatch (7.7%), which in turn not only prevents the formation of misfit defectfree, perfect heteroepitaxial interface but limits the shell growth to an extended thickness. Thus, notable improvements in PL could be achieved by inserting a larger-lattice constant inner shell (relative to ZnS) prior to ZnS outer shelling, enabling the effective alleviation of the interfacial strain. The common inner shell compositions are GaP, [13,14] alloyed or compositiongradient ZnSeS, [15][16][17][18][19] and ZnSe, [20][21][22][23][24] all of which are intermediate in lattice constant between InP and ZnS, while providing a stepwise type-I electronic band alignment in overall doubleshelled heterostructure. When GaP interlayer was generated via either cation exchange or direct overgrowth, the resulting InP/GaP/ZnS QDs exhibited 40−85% in PLQY and 41−64 nm in FWHM, highly depending on the emission color. [13,14] In such InP/GaP/ZnS heterostructure, the thickness of GaP inner shell was far below 0.5 nm. A difficulty of thicker GaP growth on InP core likely stems from a still large inequality in lattice constant (6.8%), which is only slightly better than that of