Selection of the bandedge lasing mode of a photonic crystal laser has been realized in a fluorescent dye doped chiral nematic liquid crystal by exerting electrical control over the mode competition. The bandedge lasing can be reversibly switched from the short-wavelength edge mode to the long-wavelength edge mode by applying a voltage of only 20 V, without tuning the bandgap. The underlying mechanism is the field-induced change in the order parameter of the fluorescent dye in the liquid crystal. The orientation of the transition dipole moment determines the polarization state of the dye emission, thereby promoting lasing in the bandedge mode that favors the emission polarization. Moreover, the dynamic mode-selection capability is retained upon polymer-stabilizing the chiral nematic liquid crystal laser. In the polymer-stabilized system, greatly improved stability and lasing performance are observed. The lasing behavior in chiral nematic liquid crystals (CLC) has been extensively studied over the past decades due to its favorable properties, such as low threshold, high tunability, and the ease of fabrication. [1][2][3] CLC is a particular class of liquid crystals in which the molecules self-assemble into one-dimensional helices, typically formed by mixing a nematic liquid crystal with a chiral agent. The concentration and twisting power of the chiral agent determine the helical pitch (p). Such a periodic chiral structure can be regarded as a one-dimensional photonic crystal for a circularly polarized probe with the same handedness as that of the structure. The associated photonic bandgap (PBG) is located at λ c = n c ⋅p with a bandwidth Δλ = Δn⋅p, where n c and Δn are the average refractive index and birefringence of the CLC, respectively. Resonances occur at the two bandedges: long wavelength edge (LWE) and short wavelength edge (SWE); the corresponding wavelengths are λ LWE = n e ⋅p and λ SWE = n o ⋅p, respectively, where n e is the extraordinary refractive index and n o is the ordinary refractive index. At the bandedge, the group velocity of light approaches zero, and hence the density of states is significantly enhanced. 4,5 In the presence of a gain medium, laser action can occur at the photonic bandedge(s) through optical excitation-usually termed the bandedge lasing. To date, a great deal of effort has been devoted to achieve a wide dynamic tuning range of the lasing wavelength with the aid of external inputs, such as electric field 6,7 , heat 8,9 , light 10 , and mechanical stress 11 . However, the post-