Rapid mixing is essential for achieving effective chemical and biological reactions. Because passive diffusion is a slow process, it is often necessary to agitate or stir a solution. Generating such disturbance must involve an external input of energy, for example, transduction of magnetic field energy through the use of commercial magnetic stir bars. But such use is impractical for the tiny channels and droplets, which are of great importance for lab-on-chip applications [1] and microliter bioassay. [2] The main challenge lies in the fabrication of low-cost stir bars that are sufficiently small but still able to transduce external energy for the mixing. Moreover, the stir bars should be introduced, operated, and extracted with ease.In microfluidic research, a number of methods have been developed to improve mixing. For a lamellar flow confined in a channel, turbulence can be induced by forcing the solution through a complex winding channel, [1b, 3] or by pulsed injection of additional solution/bubbles from the side channels, [4] thermal gradients can be used to induce convection, [2c, 5] direct physical agitation can be achieved using ultrasound or piezoelectric transducers, [6] and in-channel stirring was achieved using magnetic turbines that were fabricated by lithographic methods. [7] These mixing schemes were often fabricated together with the channel systems, because it is too difficult to introduce them after the fabrication.In static microdroplets, however, transducing external energy for mixing remains a challenge, particularly in arrays of microdroplets. Ultrasonication and violent stirring can break up the droplets, while thermal gradients across tiny droplets are impractical. To date, magnetic stirring is still the most convenient option. Micro-sized stir bars have been reported, for example, linear chains of polymer beads embedded with magnetic nanoparticles (NPs), [8] star-shaped micro-stirrers made by soft lithography, [9] and cobalt-based magnetic bars cut by laser micromachining. [10] Because of gravitational and magnetic attraction, micro-sized stir bars tend to stir only at the bottom of the vessel, [10] leaving most part of the solution unstirred. While facile and scalable synthesis remains a challenge, the main problem of microsized stir bars is still their size: they are too large to remain suspended, but too small to churn up the whole solution.Herein, we report a simple and scalable method for fabricating magnetic stir bars, which are tunable from 75 nm-1.4 mm in width and up to around 17 mm in length (Figure 1). They are straight single-line chains assembled from 40 nm magnetic NPs and then preserved in silica shells of variable thickness. These rigid magnetic chains showed immediate response to a common magnetic stir plate and can be easily recovered. Being small and in large number, they can remain suspended and stir independently in all parts of the solution. These nano stir bars can be readily dispensed for parallel stirring of droplets down to picoliter in volume (4 picoliter). ...