This paper reports the study of the uncontrolled multiple tunnel junctions ͑MTJs͒ induced by the random dopants in heavily doped silicon single electron transistors ͑SETs͒. The SETs are fabricated by making dual lateral constrictions in the narrow doped silicon channel formed on a silicon on insulator substrate. The doped SETs with relatively long constriction regions invariably exhibit the MTJ characteristics. Silicon based single electron devices ͑SEDs͒ have attracted much attention because of their higher operating temperature, and their compatibility with the complementary metal oxide semiconductor technology. 1,2 Recently, these devices have been more actively studied for qubit 3,4 and nanoelectromechanical systems. 5 In particular, a suspended quantum dot cavity structure can be used to study the interaction of single electrons with phonons, the physics of decoherence mechanisms for quantum bits and electromechanical phenomena such as, phononic bandgaps, phonon confinement, quantization of nanomechanical motion, and a strong coupling of nanomechanical and electron motions. 5 These phenomena may lead to silicon quantum information devices. 6 One of the common approaches to realizing SEDs in silicon is to use a very narrow doped silicon channel with lateral constrictions in a silicon on insulator ͑SOI͒ substrate. 7 However, these devices often exhibit multiple tunnel junction ͑MTJ͒ behaviors irrelevant to their geometrical shapes. 8,9 These MTJs may smear out the fundamental physical phenomena. The theoretical study in Ref. 10 reports the basic mechanism of the electron island formation and electron transport properties in the heavily doped nanowires, but there has been no experimental work reported to address the MTJ issue in these devices. It is imperative to study the MTJ issue and to develop a fabrication method to avoid these unwanted MTJs to study the fundamental physics of nanodevices.In this article, we report the measurement results of three heavily doped single electron transistors ͑SETs͒ with different channel constriction lengths. It was found that longer channel constriction regions invariably lead to random dopant induced MTJs. The influence of the MTJs decreased with decreasing channel constriction length. Finally, it is demonstrated that it is possible to overcome the uncontrolled MTJ formation by fabricating extremely sharp constrictions with low surface disorder.The device formation process is the same as the SET patterning reported in Ref. 11. A scanning electron microscopy ͑SEM͒ image of a typical fabricated SET is shown in Fig. 1͑a͒. The bright regions indicate the SOI layer and the dark regions indicate the BOX layer of the substrate. The lithographically defined constrictions in the silicon channel act as tunnel barriers as a result of bandgap enlargement in the narrower regions. 11 Higher resolution SEM images of the dot region of devices A, B, and C are shown in Figs. 1͑b͒-1͑d͒, respectively. The approximate constriction lengths of devices A, B, and C are 75, 65, and 45 nm, respectiv...