Abrupt fluorescence intermittency or blinking is long recognized to be characteristic of single nano-emitters. Extended quantum-confined nanostructures also undergo spatially heterogeneous blinking;h owever,t here is no such precedent in dimensionally unconfined (bulk) materials. Herein, we report multi-level blinking of entire individual organo-lead bromide perovskitemicrocrystals (volume = 0.1-3 mm 3 )u nder ambient conditions.E xtremely high spatiotemporal correlation (> 0.9) in intracrystal emission intensity fluctuations signifies effective communication amongst photogenerated carriers at distal locations (up to ca. 4 mm) within each crystal. Fused polycrystalline grains also exhibit this intriguing phenomenon, whichi sr ationalized by correlated and efficient migration of carriers to af ew transient nonradiative traps,t he nature and population of whichd etermine blinking propensity.O bservation of spatiotemporally correlated emission intermittency in bulk semiconductor crystals opens the possibility of designing novel devices involving longrange (mesoscopic) electronic communication.Fluorescence intermittencyo rb linking, which refers to temporally random discrete jumps in intensity between bright and dark levels,has been considered as one of the main pieces of evidence for the detection of single nano-sized quantum emitters. [1][2][3][4][5][6][7][8] Apart from single molecules,b linking is commonly observed in various individual quantum-confined systems such as semiconductor nanocrystals (NCs), in which excitons/charge carriers are spatially restricted in more than one dimension. [4][5][6][7][8][9][10][11][12][13] In NCs,photoluminescence (PL) blinking is attributed to intermittent Auger ionization-recombination processes leading to charging-discharging of NCs or longlived carrier trapping in surface (defect) states. [4,5,14,15] However,P Li ntermittencyi ss eldom observed beyond the nanoscale (approaching bulk), as temporally uncorrelated intensity fluctuations from various emitters average out over the ensemble and contribution of surface states in radiative recombination becomes less significant compared to that of free carriers in the bulk. [7] Even for 1D-or 2D-confined extended nanostructures, blinking beyond the diffraction limit (ca. 250 nm) is uncommon, and such PL intermittencyi ss patially heterogeneous, that is,s patiotemporally uncorrelated. [9,16] There is ar are example of spatially concerted PL intensity fluctuations in an extended quantum-confined system; [10] asmall proportion (1-2%)o fe ntire single CdSe quantum wires were found to exhibit correlated multilevel blinking, attributed to delocalized 1D excitons.w hich allow efficient long-range carrier migration. More recently,i ndividual stacked-monolayers of transition metal dichalcogenides (MoSe 2 /WS 2 )were reported to undergo temporally anti-correlated blinking arising from mobile 2D excitons,w hich experience sporadic interlayer charge transport. [17] Owing to their exceptional carrier diffusion lengths and diffusivities, [18,19] or...