Despite significant technological advances in miniaturization and operational speed, modern electronic devices suffer from unescapably increasing rates of Joule heating and power consumption. Avoiding these limitations sparked the quest to identify alternative, chargeneutral information carriers. Thus, spin waves, the collective precessional motion of spins in permanent magnets, were proposed as a promising alternative system for encoding information. In order to surpass the speed, efficiency, functionality and integration density of current electronic devices, magnonic devices should be driven by electric-field induced methods. This review highlights recent progress in the development of electric-fieldcontrolled magnonic devices, including present challenges, future perspectives and the scope for further improvement. S pin waves (SWs) are the dynamic eigen modes of magnetically ordered systems, such as ferromagnetic (FM) metals 1,2 , ferrimagnetic insulators 3,4 and antiferromagnets 5. In other words, SWs are phase coherent collective precessional motion of ordered magnetic spins 6 (Fig. 1a). These SWs may serve as a potential information carrier in future microwave signalprocessing devices, by using its amplitude, phase, and polarization, at significantly lower power consumption as SWs are not associated with translational motion of electronic charges 4,7. Therefore, SWs can be used as an alternative to modern charge current-based complementary metal-oxide-semiconductor (CMOS) technology, which is now suffering from increased rate of power consumption due to Joule heating. The quanta of SWs are called "magnon". Following this name, a new research field, known as "magnonics" 6,8 , is rapidly developing. When magnonics meets spintronics, the field is known as magnon spintronics 9. The aim of magnonics is to control and manipulate SW properties so that they can be utilized in future spintronics technology 8,9. Apart from lower energy consumption, another advantage of SWs is that they can have wide variety of wavelengths ranging from few tens of micrometer down to few tens of nanometer with the corresponding frequency ranging from few Gigahertz to few Terahertz, which can be even controlled by tuning various internal and external parameters, such as saturation magnetization, various magnetic anisotropies, magnetostatic interactions, exchange interaction, magnetic field, and electric field 8,10,11. Although, SWs have much smaller group