Tag Archives: transistor

Single-electron Molecular Switch 4nm Across

A molecule rotating on the surface of a crystal can function as a tunnel-gate of a transistor, as shown by researchers from the Paul-Drude-Institut für Festkörperelektronik (PDI) and the Freie Universität Berlin (FUB), Germany, the NTT Basic Research Laboratories (NTT-BRL), Japan, and the U.S. Naval Research Laboratory (NRL). Their complete findings are published in the 13 July 2015 issue of the journal Nature Physics. The team used a highly stable scanning tunneling microscope (STM) to create a transistor consisting of a single organic molecule and positively charged metal atoms, positioning them with the STM tip on the surface of an indium arsenide (InAs) crystal.
Dr. Stefan Fölsch, a physicist at the PDI who led the team, explained that “the molecule is only weakly bound to the InAs template. So, when we bring the STM tip very close to the molecule and apply a bias voltage to the tip-sample junction, single electrons can tunnel between template and tip by hopping via nearly unperturbed molecular orbitals, similar to the working principle of a quantum dot gated by an external electrode. In our case, the charged atoms nearby provide the electrostatic gate potential that regulates the electron flow and the charge state of the molecule.”

(Top) STM images of phthalocyanine (H2Pc) molecule rotated from a neutral (50 pA, 60 mV; left) to −1 charged states (50 pA, −60 mV; centre and right) on InAs(111) surface using a ~4nm across hexagonal array of charged indium adatoms surrounding the H2Pc to create rotational energy minima, and (Bottom) schematic model of H2Pc rotation relative to the InAs lattice resulting in the electrostatic gating of tunneling to an STM tip vertical to the device. (Source: Nature Physics)

(Top) STM images of phthalocyanine (H2Pc) molecule rotated from a neutral (50 pA, 60 mV; left) to −1 charged states (50 pA, −60 mV; centre and right) on InAs(111) surface using a ~4nm across hexagonal array of charged indium adatoms surrounding the H2Pc to create rotational energy minima, and (Bottom) schematic model of H2Pc rotation relative to the InAs lattice resulting in the electrostatic gating of tunneling to an STM tip vertical to the device. (Source: Nature Physics)

The Figure shows that the diameter of the device is ~4nm, so by conservative estimation we may take this as the half-pitch of closest-packed devices in IC manufacturing, which leads to pitch of 8nm. As a reminder, today’s “22nm- to 14nm-node” devices feature ~80nm transistor gate pitches (with “10nm node” planning to use ~65nm gate pitch, and “5nm node” ICs expected with ~36nm gate pitch). Thus, these new prototypes prove the concept that ICs with densities 100x more than today’s state-of-the-art chips could be made…if on-chip wires can somehow connect all of the needed circuitry together reliably and affordably.
—E.K.

ALD of Crystalline High-K SHTO on Ge

Alternative channel materials (ACM) such as germanium (Ge) will need to be integrated into future CMOS ICs, and one part of the integration was shown at the recent Materials Research Society (MRS) spring meeting by John Ekerdt, Associate Dean for Research in Chemical Engineering at the University of Texas at Austin, in his presentation on “Atomic Layer Deposition of Crystalline SrHfxTi1-xO3 Directly on Ge (001) for High-K Dielectric Applications.”

Strontium hafnate, SrHfO3 (SHO), and strontium titanate, SrTiO3 (STO), with dielectric constants of ~15 and ~90 (respectively) can be grown directly on Ge using atomic layer deposition (ALD). Following a post-deposition anneal at 550-590°C for 5 minutes, the perovskite films become crystalline with epitaxial registry to the underlying Ge (001) substrate. Capacitor structures using the crystalline STO dielectric show a k~90 but also high leakage current. In efforts to optimize electrical performance including leakage current and dielectric constant, crystalline SrHfxTi1-xO3 (SHTO) can be grown directly on Ge by ALD. SHTO benefits from a reduced leakage current over STO and a higher k value than SHO. By minimizing the epitaxial strain and maintaining an abrupt interface, the SHTO films are expected to reduce dielectric interface-traps (Dit) at the oxide-Ge interface.

Much of the recent conference has been archived, and can now be accessed online.

—E.K.