The second boom in superconductivity during the last two decades has been powered up by the discovery of MgB 2 having the transition temperature (T c ) of 39 K [1] as well as a strong market potential for applications. The strongest impact on the development of this superconductor has been made by the discovery of the significant enhancement of the critical current density (J c ) as a function of the applied magnetic field (B a ) that results from SiC nanodoping.[2] Since then, a large variety of dopants have been attempted in order to achieve or improve on the attained enhancement. [3][4][5][6][7][8][9][10][11] In the vast majority of these doping works the nanodopants have been introduced via a solid-state reaction; [12][13][14][15][16][17] however, an important challenge is achieving homogeneity between a small amount of nanoadditives and matrix materials, because any dry mixing poses the major problem of nanoparticle agglomeration. In this Communication, we have chosen sugar (C 6 H 12 O 6 ) as the dopant. This is the most readily available carbohydrate that enables liquid homogeneous mixing. We have demonstrated that sugar doping resulted in an effective substitution of carbon for boron in MgB 2 , so that a significant enhancement of the J c performance over the entire applied field range is readily achievable. This method is applicable to the fabrication of a wide range of carbon-based compounds and composites. The MgB 2 superconductor has a strong potential for various applications because of its high T c , strong connectivity between the grains, and low anisotropy.[18] One major problem is posed by the relatively weak pinning in the pure material, which leads to rather rapid degradation of J c as a function of B a . Different approaches, such as irradiation and chemical doping, have been used to enhance the pinning strength in MgB 2 . [2,[4][5][6]10,11,17,19] . Chemical doping is a desirable, relatively easy, and cheap method to introduce pinning sites into the superconductor. Nanometer-size SiC has been found to be the most effective dopant for J c enhancement. [2,5,6,15,[20][21][22] The carbon-based materials introduce the strongest enhancement of J c (B a ) performance in MgB 2 , owing to the fact that carbon can be incorporated into the MgB 2 crystal lattice by replacing boron. This substitution results in the enhancement of chargecarrier scattering occurring on C-substituted sites and Mgvacancies in two energy bands discovered in this material. [23] This scattering has been shown to be responsible for the considerable upper critical field increase.[24] Generally, nanometer-sized particles are necessary to ensure a homogeneous doping procedure, which in our case should provide a strong enhancement of the pinning force. However, regardless of how well mixing, grinding, [2,5] milling, or ultrasonic dispersion [16] is carried out, the doping process is usually impeded by the formation of large agglomerates of particles. In addition, the precursor materials are commonly in their passivated state, which can...