Several methods of harvesting singlet excitons via delayed fl uorescence have been introduced in OLED so far. These methods include up-conversion to singlet excitons by triplet-triplet annihilation (TTA) [ 3,4 ] or triplet fusion in materials that show a strong singlet fi ssion. [ 5 ] A different approach for enhancing the singlet emission that involves triplet excitons was introduced recently, whereby the triplet excitons may undergo reverse intersystem crossing (RISC) to singlet excitons and consequently give rise to thermally activated delayed fl uorescence (TADF). [6][7][8][9][10][11][12] This occurs in compounds with small electron exchange energy, and thus small singlet-triplet energy splitting, Δ E ST that enables triplet excitons to undergo thermally activated RISC to the singlet manifold. [ 13 ] A fi rm indication for TADFrelated emission in compounds that possess RISC is that the EL in these OLED is thermally activated, with activation energy E act ≈ Δ E ST Ͻ Ͻ 0.7 eV (which is Δ E ST in traditional organic semiconductors). During the last few years there has been a large interest in magnetic fi eld effect (MFE) in conjugated organic compounds, mainly because of the possibility to enhance the electroluminescence effi ciency, which was dubbed magneto-EL (MEL). [ 11,[14][15][16][17][18][19][20][21] In this effect, the magnetic fi eld changes the exchange rate between PP singlet (PP S ) and triplet (PP T ), which can be detected through the induced change in the EL emission intensity (MEL) or the current density (MC) in the device. This occurs if the PP S and PP T recombination rates ( R S , R T ) and/or dissociation rates ( d S , d T ) differ from each other. [ 17,22 ] So far the MEL maximum value, MEL max at room temperature (RT) has been less than ≈20% in OLEDs.In conventional OLEDs, spin mixing occurs within the PP states rather than at the exciton levels because the electron-hole orbitals strongly overlap in the latter species leading to large exchange energy, J , that consequently causes large energy gap, Δ E ST (=2 J ) between singlet and triplet states. In contrast, materials showing RISC may allow spin-mixing among the PP spin levels and in the exciton levels because Δ E ST is small. [ 23 ] In this case, possible spin-mixing mechanism may be the hyperfi ne interaction [ 24,25 ] and/or the Δ g mechanism, [ 26 ] where the difference, Δ g in the g -values of positive and negative carrier in the pair may promote intersystem crossing. The obtained full width Reverse intersystem crossing (RISC) from triplet to singlet states has been recently introduced to photophysics of organic chromophores. One type of RISC occurs in donor (D)-acceptor (A) composites that form an exciplex manifold in which the energy difference, Δ E ST between the lowest singlet (S 1 ) and triplet (T 1 ) levels of the exciplex is small (<100 meV) thus allowing RISC at room temperature. This adds a delayed component to the photoluminescence emission that is widely known as thermally activated delayed fl uorescence. Here, it is found t...