The mechanism of using the anisotropic Purcell factor to control the spontaneous emission linewidths in a four-level atom is theoretically demonstrated; if the polarization angle bisector of the two dipole moments lies along the axis of large/small Purcell factor, destructive/constructive interference narrows/widens the fluorescence center spectral lines. Large anisotropy of the Purcell factor, confined in the subwavelength optical mode volume, leads to rapid spectral line narrowing of atom approaching a metallic nanowire, nanoscale line width pulsing following periodically varying decay rates near a periodic metallic nanostructure, and dramatic modification on the spontaneous emission spectrum near a custom-designed resonant plasmon nanostructure. The combined system opens a good perspective for applications in ultracompact active quantum devices. KEYWORDS: Surface plasmon, spontaneous emission, Purcell factor, quantum emitter, quantum interference R ecent developments in nanotechnology and information technologies have made nanoscale light-matter interaction a tremendous research focus. 1 Small optical mode area in nanofiber-based photonic structures plays a significant role allowing low-light level quantum optical phenomena, such as electromagnetically induced transparency in the nanowatt regime, 2,3 four wave mixing with great gain, 4 and two-photon absorption with sharp peaks in the Rubidium vapor. 5 Ultrasmall optical mode volume in plasmon nanostructures 6 leads to strong coupling between surface plasmons and quantum emitters, which enables the vacuum Rabi splitting, 7,8 the Fano lineshapes in the absorption spectrum, 9−12 and its obvious influence on the two-photon statistics. 13 Superior to many available photonic nanostructures, associated with ultrasmall optical mode volume, 6 plasmonic structures present the key advantage of a large subwavelengthconfined anisotropic vacuum, that is, large anisotropic Purcell factor, 14,15 which originates from an anisotropic electric mode density of collective oscillations of free electrons in metals. 16−19 Another advantage is strong evanescent field of metallic nanostructures, which has promoted many applications, for example, SERS, 20 nanometer biosensors and waveguides, 21 nonlinear optical frequency mixing, 22−24 solar cell, 25,26 and so forth. Through modifying the population of excited states and decay rate of quantum emitters near plasmon structure, the fluorescence enhancement and quenching of fluorescent molecules and semiconductor quantum dots can be controlled well. 27−32 By confining the light into nanoscale volumes, plasmonic elements allow for a nanoscale realization of Mollow triplet of emission spectra and antibunching of emission photons of single molecules that traditional technique can not be accessible. 1,33,34 Through the nanoscale coupling between the surface plasmon modes and single quantum emitter, the directional and efficiency generation of single photons 17−19 and entanglement of two qubits 35 were proposed. These advantages, t...