We demonstrate the formation of semimetal graphite/semiconductor Schottky barriers where the semiconductor is either silicon (Si), gallium arsenide (GaAs) or 4H-silicon carbide (4H-SiC). Near room temperature, the forward-bias diode characteristics are well described by thermionic emission, and the extracted barrier heights, which are confirmed by capacitance voltage measurements, roughly follow the Schottky-Mott relation. Since the outermost layer of the graphite electrode is a single graphene sheet, we expect that graphene/semiconductor barriers will manifest similar behavior.PACS numbers: 81.05. UW, 73.30.+y, Metal-semiconductor contacts are ubiquitous in semiconductor technology not only because they are unavoidable, but also because the associated (Schottky) barriers to electronic transport across the metal-semiconductor interface can be tuned by judicious choice of materials and processing techniques [1]. The most prominent property of a Schottky barrier is its rectifying characteristic; the barrier acts like a diode with large currents flowing for forward bias and significantly smaller currents flowing for reverse bias [2]. If low resistance and "ohmic" (linear) I-V characteristics are desired, then materials and/or processing techniques are chosen to assure that the Schottky barrier height (SBH) φ B is small compared to temperature (i.e., φ B << k B T ). Semimetal rather than metal electrodes can also be used. For example, epitaxial ErAs/InAlGaAs diodes fabricated by molecular beam epitaxy have barrier heights that can be tuned over a wide range by adjusting composition and doping[3].Here we report on the use of highly oriented pyrolytic graphite (HOPG) as the semimetal in semimetal/semiconductor Schottky barriers. We demonstrate rectifying characteristics on three different n-type semiconductors each of which is uniquely suited to specific applications: namely Si, with its robust oxide, to field gated transistors, GaAs, with its direct band gap, to spintronic and optical applications and SiC, with its high thermal conductivity and breakdown strength, to high power/frequency devices. Advantageously the HOPG contact, which can be applied at room temperature, causes minimal disturbance at the semiconductor surface for two reasons: the graphene sheets of the graphite are robustly impervious to diffusion of impurity atoms[4] and the Van der Waals force of attraction is relatively weak. Since φ B is related to an interfacial dipole layer associated with bond polarization[1], we infer that barrier properties are determined primarily by the outermost layer of the HOPG contact, i.e., a single layer graphene (SLG) sheet. Accordingly, our results anticipate similar phenomenology using two-dimensional (2D) graphene rather than three-dimensional (3D) graphite. * Corresponding author: afh@phys.ufl.eduOther examples demonstrating SLG-like properties in graphite include ARPES evidence for the precursor influence of K-point Dirac fermions[5] and a pronounced temperature-dependent upturn in the in-plane resistivity (ρ ab...