Their advantages included cost-effectiveness and improved capability in miniaturization and in making flexible devices. [2] In the future, it is expected that OLED will be pivotal for emerging applications such as sensing and imaging, [3] phototherapy, [4] and even security identification, [5] to which the nearinfrared (NIR) emissions are both invisible to human eyes and with an increased penetration depth into our tissue. Therefore, electroluminescence (EL) with peak wavelengths beyond 700 nm will be needed in the successful fabrication of this class of OLED. [6] Moreover, an emission peak max. (λ max ) of over 800 nm (1.6 eV) is essential for achieving an emission onset at 700 nm (1.8 eV) and to be fully invisible to human. However, when the emission gap is shifted toward the deep red and NIR regions, the vibrational relaxation can be facilitated through the overlap between the zero vibration level of the lowest-lying singlet (S 1 ) or triplet (T 1 ) state and the higher vibration levels of the ground (S 0 ) state. Therefore, NIR emitting materials typically suffer from inferior emission efficiency, according to the above mentioned energy gap law. [7] Generally speaking, fluorescent emitters, [8] thermally activated delayed fluorescent (TADF) molecules [9] and transitionmetal complexes [10] have been promising candidates for NIR emission. To name a few, the BF 2 curcuminoid derivatives were employed in fabrication of NIR TADF OLED, showing Near-infrared (NIR) emitting Os(II) complexes [Os(L1) 2 (PPhMe 2 ) 2 ] (tz1), [Os(L2) 2 (PPhMe 2 ) 2 ] (tz2), and [Os(L3) 2 (PPhMe 2 ) 2 ] (tz3), bearing dual (1H-1,2,4-triazol-5-yl)pyrazine chromophoric chelates, are successfully developed. These pyrazine chelates tzn (n = 1, 2, 3) differ by the location and number of 4-(trifluoromethyl)phenyl appendage(s) on pyrazine, and the associated Os(II) complexes exhibit bathochromic shifted emission, higher quantum yield, and increased radiative lifetime in comparison to parent complex [Os(fprtz) 2 (PMe 2 Ph) 2 ] (tz0). Moreover, partially deuterated pyrazine chelate L1-d is prepared using post-synthetic deuteration, from which the Os(II) complex tz1 shows a photoluminescence quantum yield (PLQY) of 12.2% in co-doped 4,4′-bis(N-carbazolyl)biphenyl (CBP) thin film at 3 wt%. Further, the partially deuterated tz1-d exhibits a notable increase in PLQY to 17.8% upon co-deposited into CBP thin film, confirming the influence of C-H(D) stretching vibrations on the non-radiative transition processes. Finally, tz1-d is demonstrated to be suitable in the fabrication of efficient NIR organic light-emitting diodes (OLEDs), from which max. external quantum efficiency of 3.77% and max. radiance of 24.1 W sr -1 m -2 are recorded for emission with peak maximum at 776 nm. These experiments confirm the suppression of C-H vibration caused quenching by deuteration, which should be broadly applicable to the OLED emitters, especially in the NIR region.