with various refractive indices are critical components in optical feedback systems for lasers [4] and also play an important role in high-performance light-emitting devices, [5,6] photodetectors, [7] and solar cells. [8,9] The optical properties of such systems can be precisely tailored by manipulating the chemical composition and architecture (thickness and porosity) of stacked layers. Recently, special research interests lie in responsive DBRs, in which dynamical changes of the optical properties (reflectivity, band-gap, structural color) in response to external stimuli (such as light, temperature, chemical species, and electrical field) have been demonstrated. [10][11][12][13] Among them, electrical field is the most easily controlled stimulus and simplifies integration into existing electronic components, finding new applications in active filters, tunable laser sources, and color manipulation for optical communication and display technologies.In this regard, redox-active polymers, [14][15][16] polyelectrolyte hydrogels, [17,18] liquid crystals, [19,20] or electrochromic materials [21,22] have been introduced into the periodic structure for realizing electrically tuned optical coatings. The shape and size manipulation using redox-active polymers, polyelectrolyte hydrogel, and liquid crystal usually cause large reflectance shifts, but slow response and poor durability, unsuitable for practical applications. By comparison, electrochromic materials can reversibly change their electronic structure and optical property (transmittance, reflectance, or absorption) under a small driving voltage and have been widely applied in energysaving smart windows, switchable mirrors, and displays. [23][24][25][26] This color change is mainly caused by the adjustable absorption as well as change of refractive index. Moreover, electrochormic materials have unique open-circuit memory effect (bistability in colored and bleached states), making it possible to prepare devices with low energy consumption and good stability. [27] DBRs employ two kinds of electrochromic materials with different refractive indices such as WO 3 and NiO and have shown electrically tunable reflectivity and photonic stop-band. [22] However, the preparation process was relatively complex with the requirement for high-temperature calcination at 450 C after depositing of each layer. In addition, complementary coloration effects of WO 3 (cathodic coloration) and NiO (anodic coloration)The electroresponsive WO 3 -based electrochromic distributed Bragg reflectors (ECDBRs) are fabricated by means of one-step, room temperature glancingangle electron-beam evaporation. The reflectance and Bragg wavelength of ECDBRs can be precisely and reversibly tailored on a large scale by simply applying a small bias voltage (±1.1 V) due to the electrochromic effect of the WO 3 layer, and this unique character is utilized to construct an electrically tunable microcavity luminescent device with embedded green CdSe@ZnS quantum dots (QDs). Therefore, large and reversible modulation i...