So far, all experimental tests of Bell inequalities which must be satisfied by all local realistic hidden-variable theories and are violated by quantum mechanical predictions have left at least one loophole open. We propose a feasible setup allowing for a loophole-free test of the Bell inequalities. Two electron spin qubits of donors 31 P in semiconductors in different cavities 300 m apart are entangled through a bright coherent light and postselections using homodyne measurements. The electron spins are then read out randomly and independently by Alice and Bob, respectively, with unity efficiency in less than 0.7µs by using optically induced spin to charge transduction detected by radio-frequency single electron transistor. A violation of Bell inequality larger than 37% and 18% is achievable provided that the detection accuracy is 0.99 and 0.95, respectively.PACS numbers: 03.65. Ud, 03.67.Mn, 42.50.Pq Most working scientists hold fast to the concepts of 'realism' according to which an external reality ezists independent of observation and 'locality' which means that local events cannot be affected by actions in space-like separated regions [1]. The significance of these concepts goes far beyond science. Based on these deep-rooted reasonable assumptions, in their seminal 1935 paper, Einstein, Podolsky, and Rosen (EPR) advocated that quantum mechanics is incomplete [2]. The EPR arguments about the physical reality of quantum systems is shifted from the realm of philosophy to the domain of experimental physics since 1964 when Bell and others constructed mathematical inequalities -one of the profound scientific discoveries of the 20th century [3,4], which must be satisfied by any theory based on the joint assumption of realism and locality and be violated by quantum mechanics. Many experiments [1,5,6,7,8,9,10,11,12] have since been done that are consistent with quantum mechanics and inconsistent with local realism. So far, however, all these tests suffered from "loopholes" allowing a local-realistic explanation of the experimental results by exploiting either the low detector efficiency [13,14] or the timelike interval between the detection events [15,16]. The first loophole names the detection loophole allowing the possibility that the subensemble of detected events agrees with quantum mechanics even though the entire ensemble is consistent with Bell inequalities. So a fair-sampling hypothesis that the detected events represent the entire ensemble must be assumed. The second refers the locality or 'lightcone' loophole allowing the correlations of apparently separate events resulting from unknown subluminal signals which propagate between space-like regions of the apparatus to take place.Several schemes were proposed closing these loopholes based on entangled photon pairs [17,18] [22,23], but all face a formidable experimental challenge. Here we propose a scheme for the loophole-free Bell test based on the Kane Si:P architecture [24], in which two qubits are encoded onto two electron spins of donor atoms 31 P in...