strategy is to replace Pb 2+ cations with the divalent Sn 2+ or Ge 2+ cations by equivalent substitution during the nanocrystal (NC) synthetic process. [4] However, the Sn 2+ and Ge 2+ ions in the perovskite NCs are easily oxidized to their tetravalent states under ambient conditions, resulting in defects induced photoluminescence (PL) quenching of this kind of lead-free halide perovskite NCs. [5] Another strategy to synthesize lead-free halide perovskite NCs is the substitution of three Pb 2+ ions by two trivalent ions such as Sb 3+ and Bi 3+ to form low-dimensional perovskite NCs. [6] Unfortunately, these kinds of bismuth/ antimony-based perovskite NCs have poor optical properties due to reduced band dispersion and low carrier mobility. [7] Beyond above single metal ion substitution, a promising strategy for the synthesis of lead-free halide perovskite NCs is using one monovalent M + and one trivalent M 3+ cations to replace two divalent Pb 2+ ions. This strategy leads to the formation of lead-free double perovskite (DP) AMMʹX 6 (A = Cs, CH 3 NH 3 ; M = Ag, Au, Na; Mʹ = Bi, Sb, In; X = Cl, Br, I) structure. The lead-free DP maintains both the 3D perovskite structure and the charge neutrality, which will have a great potential to explore new optoelectronic properties. [8] For instance, the metal halide DP Cs 2 AgBiCl 6 and Cs 2 AgBiBr 6 NCs with good stability under ambient conditions have been synthesized, but the optical properties of the pure phase lead-free double halideThe exploration of lead-free halide perovskite nanocrystals (NCs) with intriguing optical properties is highly desirable owing to the toxicity and instability of lead halide perovskite NCs. Here, a new kind of uniform lead-free double perovskite Cs 2 NaBiCl 6 NCs are reported as versatile hosts to accommodate ionic dopants for improving optical properties especially the photoluminescence (PL). In contrast to the low deep-blue PL with a quantum yield of only 1.7% of the as-synthesized pristine Cs 2 NaBiCl 6 NCs, the PL of the Cs 2 NaBiCl 6 NCs can be impressively regulated and enhanced via doping Ag + , Mn 2+ , or Eu 3+ ions in the double perovskite lattices. The femtosecond time-resolved transient absorption spectroscopy is adopted to unravel the PL enhancement mechanism of the ion doping in the Cs 2 NaBiCl 6 NCs. For the Ag + -doping, the excitonic absorption energy of the Cs 2 NaBiCl 6 NCs can be tuned from 3.82 to 3.48 eV with the significant improvement of the PL quantum yield (PLQY) from 1.7% to 20%. The Mn 2+ -doped Cs 2 NaBiCl 6 NCs show broad orange-red emission peak centered at 585 nm with a PLQY of 3%, owing to the 4 T 1 → 6 A 1 transition of octahedrally coordinated Mn 2+ . Eu 3+ -doped Cs 2 NaBiCl 6 NCs are endowed with strong Eu 3+5 D 0 → 7 F J ( J = 1, 2) orange-red emission at 591 and 615 nm.