Abstract:
Provided are a memory cell structure, a memory array structure, and a voltage biasing method. The memory cell structure includes: a substrate layer, a well layer and a transistor. The substrate layer is configured to support the memory cell structure; the well layer is embedded in the substrate layer, an upper surface of the well layer is flush with an upper surface of the substrate layer, and a transistor is arranged on the well layer. In the present disclosure, a deep well bias is performed on the memory cell structure, so that the well voltage of the memory cell may be individually biased to a specific voltage, and in combination with the redesigned memory cell array structure, the applied programming voltage mostly falls on the memory cell structure. This reduces the programming voltage of the memory cell, and avoids a breakdown of the selecting transistor due to an excessively large voltage, thereby ensuring a great reliability of the device and a higher efficiency within the area of the memory cell array structure.
Abstract:
The present disclosure provides a method for fabricating an anti-reflective layer on a quartz surface by using a metal-induced self-masking etching technique, comprising: performing reactive ion etching to a metal material and a quartz substrate by using a mixed gas containing a fluorine-based gas, wherein metal atoms and/or ions of the metal material are sputtered to a surface of the quartz substrate, to form a non-volatile metal fluoride on the surface of the quartz substrate; forming a micromask by a product of etching generated by reactive ion etching gathering around the non-volatile metal fluoride; and etching the micromask and the quartz substrate simultaneously, to form an anti-reflective layer having a sub-wavelength structure.
Abstract:
A writing method and erasing method of a fusion memory are provided, and the fusion memory includes a plurality of memory cells, and each memory cell of the plurality of memory cells includes a bulk substrate; a source and a drain on the bulk substrate, a channel region extending between the source and the drain, and a ferroelectric layer and a gate stacked on the channel region; and the writing method includes: applying a first voltage between the gate of at least one memory cell and the bulk of at least one memory cell, in which the first voltage is less than a reversal voltage at which the ferroelectric layer is polarization reversed, and each of the source and the drain is grounded or in a floating state.
Abstract:
A transition metal oxide based selector, a method for preparing the same and resistive random access memory are provided. The method comprises: S1, forming a tungsten plug on a transistor; S2, using the tungsten plug to function as a lower electrode, and preparing a transition metal layer on the tungsten plug; S3, oxidizing the transition metal layer to convert the transition metal layer into a transition metal oxide layer; and S4, depositing an upper electrode on the transition metal oxide, patterning the upper electrode and the transition metal oxide. The selector of the present disclosure may provide a high current density and has a good uniformity. The formed 1S1R structure may effectively eliminate crosstalk phenomenon in a resistive random access memory array, and effectively increase the storage density without increasing the storage unit area, thereby increasing device integration. In addition, the selector for the resistive random access memory of the present invention has advantages of a simple structure, easy for integration, a low cost, a good uniformity, and compatibility with a CMOS process.
Abstract:
A method for collecting a signal with a frequency lower than a Nyquist frequency includes, by a data transmitting end, selecting a suitable transformation base matrix for an input signal, deriving a sparse representation of the signal using the transformation base matrix to determine a sparsity of the signal, calculating a number M of compressive sampling operations according to the sparsity, sampling the signal with fNYQ/M using M channels, and integrating sampling values of each channel to obtain M measurement values. A reconstruction end reconstructs an original signal by solving optimization problems. Based on theory, compressive sampling can be performed on a sparse signal or a signal represented in a sparse manner with a frequency much lower than the Nyquist frequency, overcoming restrictions of the typical Nyquist sampling theorem. The method can be implemented simply and decrease pressure on data collection, storage, transmission and processing.
Abstract:
The present disclosure provides a memristor, including a transistor and a resistive random access memory, where a drain electrode of the transistor is connected to a bottom electrode of the resistive random access memory; and the resistive random access memory includes: the bottom electrode, a resistive random access material layer, a current compliance layer and a top electrode from bottom to top, where the current compliance layer is configured to stabilize a fluctuation of a low resistance by reducing a surge current and optimizing a heat distribution, so as to improve a calculation accuracy of a Hamming distance.
Abstract:
An activation function generator based on a magnetic domain wall driven magnetic tunnel junction and a method for manufacturing the same are provided, including: a spin orbit coupling layer configured to generate a spin orbit torque; a ferromagnetic free layer formed on the spin orbit coupling layer and configured to provide a magnetic domain wall motion racetrack; a nonmagnetic barrier layer formed on the ferromagnetic free layer; a ferromagnetic reference layer formed on the nonmagnetic barrier layer; a top electrode formed on the ferromagnetic reference layer; antiferromagnetic pinning layers formed on two ends of the ferromagnetic free layer; a left electrode and a right electrode respectively formed at two positions on the antiferromagnetic pinning layers.
Abstract:
Provided are a spin orbit torque magnetic random access memory cell, a spin orbit torque magnetic random access memory array and a method for calculating a Hamming distance, wherein the spin orbit torque magnetic random access memory cell includes a magnetic tunnel junction; a first transistor, a drain terminal of the first transistor being connected to a bottom of the magnetic tunnel junction; and a second transistor, a drain terminal of the second transistor being connected to a top of the magnetic tunnel junction.
Abstract:
Provided are a symmetric memory cell and a BNN circuit. The symmetric memory cell includes a first complementary structure and a second complementary structure, the second complementary structure being symmetrically connected to the first complementary structure in a first direction, wherein the first complementary structure includes a first control transistor configured to be connected to the second complementary structure, the second complementary structure includes a second control transistor, a drain electrode of the second control transistor and a drain electrode of the first control transistor being symmetrically arranged in the first direction and connected to a bit line, and the symmetric memory cell is configured to store a weight value 1 or 0.
Abstract:
Provided is a cache memory, including: a first field-effect transistor, a field-like spin torque layer underneath a magnetic tunnel junction, an electrode, and a second field-effect transistor sequentially arranged and connected; wherein the first field-effect transistor is configured to provide a writing current and to control the on-off of the writing current through a gate electrode; the field-like spin torque layer is configured to generate field-like spin torques for switching a first ferromagnetic layer of the magnetic tunnel junction; the magnetic tunnel junction includes a first ferromagnetic layer, a tunneling layer, a second ferromagnetic layer and a pinning layer arranged sequentially; the electrode is configured to connect the cache memory with the second field-effect transistor; and the second field-effect transistor is configured to control the on-off of the second field-effect transistor through the gate electrode to read the resistive state of the magnetic tunnel junction.