Abstract: The present invention discloses a hexagonal programmable array based on a silicon nanowire field effect transistor and a method for fabricating the same. The array includes a nanowire device, a nanowire device connection region and a gate connection region, wherein, the nanowire device has a cylinder shape, and includes a silicon nanowire channel, a gate dielectric layer, and a gate region, the nanowire channel being surrounded by the gate dielectric layer, and the gate dielectric layer being surrounded by the gate region; the nanowire devices are arranged in a hexagon shape to form programming unit, the nanowire device connection region is a connection node of three nanowire devices and secured to a silicon supporter. The present invention can achieve a complex control logic of interconnections and is suitable for a digital/analog and a mixed-signal circuit having a high integration degree and a high speed.

Abstract: Proposed is a method for testing the density and location of a gate dielectric layer trap of a semiconductor device. The testing method tests the trap density and two-dimensional trap location in the gate dielectric layer of a semiconductor device with a small area (the effective channel area is less than 0.5 square microns) using the gate leakage current generated by a leakage path. The present invention is especially suitable for testing a device with an ultra-small area (the effective channel area is less than 0.05 square microns). The present method can obtain trap distribution scenarios of the gate dielectric layer in the case of different materials and different processes.

Abstract: A method for testing trap density in a gate dielectric layer of a semiconductor device having no substrate contact is provided in the invention. A source and a drain of the device are bilateral symmetric, and probes and cables of a test instrument connecting to the source and the drain are bilateral symmetric. Firstly, bias settings at the gate, the source and the drain are controlled so that the device is under an initial state that an inversion layer is not formed and traps in the gate dielectric layer impose no confining effects on charges.

Abstract: Proposed is a method for testing the density and location of a gate dielectric layer trap of a semiconductor device. The testing method tests the trap density and two-dimensional trap location in the gate dielectric layer of a semiconductor device with a small area (the effective channel area is less than 0.5 square microns) using the gate leakage current generated by a leakage path. The present invention is especially suitable for testing a device with an ultra-small area (the effective channel area is less than 0.05 square microns). The present method can obtain trap distribution scenarios of the gate dielectric layer in the case of different materials and different processes.

Abstract: The present invention discloses a hexagonal programmable array based on a silicon nanowire field effect transistor and a method for fabricating the same. The array includes a nanowire device, a nanowire device connection region and a gate connection region, wherein, the nanowire device has a cylinder shape, and includes a silicon nanowire channel, a gate dielectric layer, and a gate region, the nanowire channel being surrounded by the gate dielectric layer, and the gate dielectric layer being surrounded by the gate region; the nanowire devices are arranged in a hexagon shape to form programming unit, the nanowire device connection region is a connection node of three nanowire devices and secured to a silicon supporter. The present invention can achieve a complex control logic of interconnections and is suitable for a digital/analog and a mixed-signal circuit having a high integration degree and a high speed.

Abstract: A method for testing trap density in a gate dielectric layer of a semiconductor device having no substrate contact is provided in the invention. A source and a drain of the device are bilateral symmetric, and probes and cables of a test instrument connecting to the source and the drain are bilateral symmetric. Firstly, bias settings at the gate, the source and the drain are controlled so that the device is under an initial state that an inversion layer is not formed and traps in the gate dielectric layer impose no confining effects on charges.