Kinetic simulations of magnetotail reconnection have revealed electromagnetic whistlers originating near the exhaust boundary and propagating into the inflow region. The whistler production mechanism is not a linear instability, but rather is Čerenkov emission of almost parallel whistlers from localized moving clumps of charge (finite-size quasiparticles) associated with nonlinear coherent electron phase space holes. Whistlers are strongly excited by holes without ever growing exponentially. In the simulation the whistlers are emitted in the source region from holes that accelerate down the magnetic separatrix towards the x line. The phase velocity of the whistlers v φ in the source region is everywhere well matched to the hole velocity v H as required by the Čerenkov condition. The simulation shows emission is most efficient near the theoretical maximum v φ ¼ half the electron Alfven speed, consistent with the new theoretical prediction that faster holes radiate more efficiently. While transferring energy to whistlers the holes lose coherence and dissipate over a few local ion inertial lengths. The whistlers, however, propagate to the x line and out over many 10's of ion inertial lengths into the inflow region of reconnection. As the whistlers pass near the x line they modulate the rate at which magnetic field lines reconnect. Electromagnetic (EM) whistler waves are commonly found in space [1][2][3][4], and in laboratory experiments [5] and are often observed during magnetic reconnection [6][7][8][9]. Various kinetic electron distributions have been found which drive whistlers unstable. The most commonly cited unstable distributions are electron temperature anisotropy [10] and electron beams [11,12], although there are other unstable distributions [13]. The quasiparticle Čerenkov emission of EM whistler waves found in the reconnection simulations in this Letter via both simulation and theory is a fundamentally different physical mechanism, in which the whistlers do not exponentiate from noise, as in kinetic instabilities.Quasiparticle Čerenkov emission [14] is an unusual process which can be understood simply in terms of an inhomogenous nonlinear current J 0 , in a spatially uniform background plasma. Let J 0 ðξ ∥ − v 0 t; ξ ⊥ Þ ¼ v 0 ρ 0 ðξ ∥ − v 0 t; ξ ⊥ Þ represent a finite-sized spatial clump of coherent charge density ρ 0 moving at speed v 0 along a background magnetic field B 0 in the spatial direction ξ jj . In its own frame ρ 0 ðξ jj ; ξ ⊥ Þ is assumed here to be the stationary charge density of a moving electron phase space hole, found from Poisson's equation in terms of the trapping potential whose parallel gradient is the bipolar electrostatic field associated with phase space holes. Such holes have been observed as bipolar parallel electrostatic field structures in space physics [15][16][17] for over 12 years. They are often associated with magnetic reconnection in magnetospheric [6,18] and laboratory plasmas [19].The spatial transform of the finite-sized hole current iswhich, for a given k jj , osc...