109 results about "Trapping region" patented technology

A transistor structure, such as a Double-gated FET (DG FET), that has been modified to include a charge-trapping region used to store either 2- or 4-bits of information. The charge-trapping region can, for example, be embedded in the gate dielectric stack underneath each gate electrode, or placed on the sidewalls of each gate electrode.

The invention includes a non-volatile memory cell comprising a field effect transistor construction having a body region within a crystalline material. The body region includes a charge trapping region. The memory cell can be TFT-SOI based, and can be supported by a substrate selected from a diverse assortment of materials. The top portion of the substrate can be a conductive layer separated from the memory device by the SOI-oxide insulator film. The charge trapping region can be, for example, silicon enriched silicon nitride or silicon enriched silicon oxide. The crystalline material can include silicon and germanium. The transistor comprises first and second diffusion regions within the body region, and also comprises a channel region between the first and second diffusion regions. The entirety of the body region within the crystalline material can be within a single crystal of the material.

A mass spectrometer is disclosed comprising an ion trap wherein ions which have been temporally separated according to their mass to charge ratio or ion mobility enter the ion trap. Once at least some of the ions have entered the ion trap, a plurality of ion trapping regions are created along the length of the ion trap in order to fractionate the ions. Alternatively, the ions may be received within one or more axial trapping regions which are translated along the ion trap with a velocity which is progressively reduced to zero.

A tandem mass spectrometer includes a two-dimensional ion trap that has an elongated ion-trapping region extending along a continuously curving path between first and second opposite ends thereof. The elongated trapping region has a central axis that is defined substantially parallel to the curved path and that extends between the first and second opposite ends. The two-dimensional ion trap is configured for receiving ions through the first end and for mass selectively ejecting the ions along a direction that is orthogonal to the central axis, such that the ejected ions are directed generally toward a common point. The tandem mass spectrometer also includes a collision cell having an ion inlet that is disposed about the common point for receiving the ions that are ejected therefrom and for causing at least a portion of the ions to undergo collisions and form product ions by fragmentation. A mass analyzer in communication with the collision cell receives the product ions from the collision cell and obtains product ion mass spectra with a rapid scan rate. In this way, a plurality of product ion spectra may be obtained for a large number of precursor ions in a sample without the need for data-dependent operation.

A non-volatile memory cell able to be written in a first direction and read in a second direction is described. The memory cell includes one or two charge trapping regions located near either the source or the drain, or both the source and the drain. During a programming operation, electrons can be injected into the charge trapping region by hot electron injection. During an erasing operation, holes can be injected into the charge trapping region. Embodiments of the invention include a charge trapping region that is overlapped by the control gate only to an extent where the electrons that were injected during a programming operation can be erased later by injecting holes in the charge trapping region.

An ion trap device comprises a wafer that supports at least one plate forming an ion trapping region therebetween. The plate has an electrically insulating surface and a multiplicity of electrodes disposed on the insulating surface. The electrodes form at least one ion trap in the trapping region when suitable voltages are applied to the electrodes via conductors coupled to the wafer. The device has a multiplicity of ports for introducing ions into the trapping region and for extracting ions from that region. In embodiments that include a multiplicity of such plates, a first one of the plates is oriented at a non-zero angle to the major surface of the wafer and is rotateably mounted on that surface. In one embodiment, at least two of the plates form an elongated micro-channel having an axis of ion propagation, and the electrodes on at least one of the two plates are segmented along the direction of the axis, thereby forming a multiplicity of ion traps along the axis. A controller applies suitable voltage (e.g., sequentially) to the segmented electrodes, thereby shifting ions from one trap to another. Preferably, the electrodes on the two plates are segmented. Applications to mass spectrometers and shift registers are described.

According to an aspect of the invention, a device structure is provided where charging and discharging occur in a trapping region formed by a stack of films that is placed on the back of a thin silicon channel. Uncoupling the charging mechanisms that lead to the memory function from the front gate transistor operation allows efficient scaling of the front gate. But significantly more important is a unique character of these devices: these structures can be operated both as a transistor and as a memory. The thin active silicon channel and the thin front oxide provide the capability of scaling the structure to tens of nanometers, and the dual function of the device is obtained by using two voltage ranges that are clearly distinct. At small voltages the structure operates as a normal transistor, and at higher voltages the structure operates as a memory device.

Embodiments of the present invention are directed to systems and methods for trapping and holding airborne particles. In the various embodiments, an optical trap is provided which uses a focused hollow-beam for trapping and holding both absorbing and non-absorbing airborne particles. The optical trap comprises: a trapping region where a particle can be present to be trapped; a light source for generating a coherent beam of light; optics for forming a hollow beam having a ring geometry from the coherent beam of light; and a focusing element for focusing the hollow beam to a point in the trapping region. In this arrangement, the particle is trapped at or near the focal point of the focused hollow beam.

There is provided in accordance with embodiments of the present invention a method of reducing the neighbor effect in reading data in a non-volatile memory array by sensing adjacent memory cells in a virtual ground array of memory cells comprising sensing substantially simultaneously a state of adjacent memory cells, wherein a bit stored in a charge trapping region of each cell of the adjacent memory cells is in an identical state.

Systems and methods of fabricating a U-shaped memory device with a recessed channel and a segmented / separated ONO layer are provided. Multibit operation is facilitated by a separated ONO layer, which includes a charge trapping region on sidewalls of polysilicon gate structures adjacent to source / drain regions. Programming and erasing of the memory cells is facilitated by the relatively short distance between acting source regions and the gate. Additionally, short channel effects are mitigated by a relatively long U-shaped channel region that travels around the recessed polysilicon gate thereby adding a depth dimension to the channel length.

A non-volatile electrically erasable programmable read only memory (EEPROM) capable of storing two bit of information having a nonconducting charge trapping dielectric, such as silicon nitride, sandwiched between two silicon dioxide layers acting as electrical insulators is disclosed. The invention includes a method of programming, reading and erasing the two bit EEPROM device. The nonconducting dielectric layer functions as an electrical charge trapping medium. A conducting gate layer is placed over the upper silicon dioxide layer. A left and a right bit are stored in physically different areas of the charge trapping layer, near left and right regions of the memory cell, respectively. Each bit of the memory device is programmed in the conventional manner, using hot electron programming, by applying programming voltages to the gate and to either the left or the right region while the other region is grounded. Hot electrons are accelerated sufficiently to be injected into the region of the trapping dielectric layer near where the programming voltages were applied to. The device, however, is read in the opposite direction from which it was written, meaning voltages are applied to the gate and to either the right or the left region while the other region is grounded. Two bits are able to be programmed and read due to a combination of relatively low gate voltages with reading in the reverse direction. This greatly reduces the potential across the trapped charge region. This permits much shorter programming times by amplifying the effect of the charge trapped in the localized trapping region associated with each of the bits. In addition, both bits of the memory cell can be individually erased by applying suitable erase voltages to the gate and either left or right regions so as to cause electrons to be removed from the corresponding charge trapping region of the nitride layer.

An ion trap is provided with at least two discrete trapping regions or segments. Both segments are located in a vacuum chamber of a mass spectrometer system. An entrance of the ion trap is disposed downstream to a laser based ionization source to receive the ions with a wide range of kinetic energies that have been generated by the laser-based ionization source. Once sufficient ions have been accumulated in the first segment and sufficient time has passed to cool the ions, they are transferred to the second segment and ultimately ejected through an aperture or slot to a detector arrangement to produce a mass spectrum.

A quadrupole ion trap device has a field adjusting electrode located outside the trapping region adjacent the aperture in the entrance end cap electrode, and optionally adjacent the aperture in the exit end cap electrode. The field adjusting electrode(s) controls field distortion in the vicinity of the apertures. By appropriately setting the voltages on the field adjusting electrodes the efficiency and resolution of operational processes such as ion introduction, precursor ion isolation and mass scanning can be improved.

A semiconductor devices including non-volatile memories and methods of fabricating the same to improve performance thereof are provided. Generally, the device includes a memory transistor comprising a polysilicon channel region electrically connecting a source region and a drain region formed in a substrate, an oxide-nitride-nitride-oxide (ONNO) stack disposed above the channel region, and a high work function gate electrode formed over a surface of the ONNO stack. In one embodiment the ONNO stack includes a multi-layer charge-trapping region including an oxygen-rich first nitride layer and an oxygen-lean second nitride layer disposed above the first nitride layer. Other embodiments are also disclosed.

A method of changing the kinetic energy of ions is provided, comprising: trapping ions in a trapping region of an ion trap; and directing a beam of gas through the trapping region, so as to change the kinetic energy of the trapped ions thereby. Also provided is a method of separating ions, the method comprising: causing ions to enter a trapping region of an ion trap along a first axis of the trapping region; directing a beam of gas along the first axis and applying an electric potential in the direction of the first axis so as to cause separation of the ions based on their ion mobility. An ion trap and a mass spectrometer for performing the methods are also provided.

A linear ion trap includes at least two discrete trapping regions for processing ions, a RF electrical potential generator, a multi-output DC electrical potential generator, and a control unit. The RF electrical potential generator produces two RF waveforms each applied to a pair of pole electrodes of the linear ion trap forming a RF trapping field component to trap ions radially. The multi-output DC electrical potential generator produces multiple DC field components superimposed to the RF field component and distributed across the length of the linear ion trap to control ions axially. The control unit switches the DC electrical potentials and corresponding DC field components collectively forming a first trapping region populated with ions to alter ion potential energy from a first level to a second level, and enables a first ion processing step in at least one of the first and second levels.

A quadrupole ion trap includes a switch (3) for switching a trapping voltage between discrete voltage levels VH, VL. This creates a digital trapping field for trapping precursor ions and product ions in a trapping region of the ion trap. A gating voltage is applied to a gate electrode (12) to control injection of source electrons into the ion trap. Application of the gating voltage is synchronised with the switching so that electrons are injected into the trapping region while the trapping voltage is at a selected one of the voltage levels and can reach the trapping region with a kinetic energy suitable for electron capture dissociation to take place.

A micro-channel device has a micro-channel for flowing liquid therethrough and includes a first aperture held in communication with the micro-channel for the purpose of injecting liquid, a second aperture held in communication with the micro-channel for the purpose of discharging liquid and a bubble trapping region constituting a part of the micro-channel. The height of the bubble trapping region is greater than the height of the micro-channel at the position of liquid inflow into the micro-channel located downstream relative to the bubble trapping region.

A semiconductor memory device which more reliably retains electrons trapped in its charge-trapping regions. A high-dielectric gate insulating film is grown on a semiconductor substrate. This gate insulating film is composed of first and second oxides, where the second oxide has a smaller bandgap than that of the first oxide and is scattered in dot-like form, surrounded by the first oxide. The memory cell is programmed by injecting electrons into a local potential minimum that is produced due to the bandgap difference between the phase-separated first and second oxides.

A flash memory cell programming system and method that facilitate efficient and quick operation of a flash memory cell by providing a biasable well (e.g., substrate) is presented. The biasable well flash memory cell enables increases in electrical field strengths in a manner that eases resistance to charge penetration of a dielectric barrier (e.g., oxide) around a charge trapping region (e.g., a floating gate). The present biasable well system and method also create a self convergence point that increase control during programming operations and reduces the chances of excessive correction for over erased memory cells. The biasing can assist hard programming to store information and / or soft programming to correct the effects of over-erasing. The biasing can also reduce stress on a drain voltage pump, reduce leakage current and reduce programming durations. Some implementations also include a biasable control gate component, biasable source component and biasable drain component.

A charge trapping nonvolatile memory device includes a source region and a drain region disposed in an upper portion of a substrate and spaced apart from each other by a first trapping region, a channel region, and a second trapping region. A gate stack structure is disposed over the channel region. A first stack including a tunnel insulation layer, a first charge trap layer, and a first blocking insulation layer are disposed over the first trapping region. A second stack including a tunnel insulation layer, a second charge trap layer, and a second blocking insulation layer are disposed over the second trapping region. An interlayer insulation layer is disposed over the substrate and covers the gate stack structure. A first contact plug and a second contact plug penetrate the interlayer insulation layer and respectively contact the source region and the drain region. A third contact plug penetrates the interlayer insulation layer, contacts the gate stack structure, and overlaps with the first and the second charge trap layers.

A cell trapping device includes a housing that includes an inlet opening connected to an inlet line through which a cell dispersion liquid is introduced and an outlet opening connected to an outlet line through which the cell dispersion liquid is discharged; and a filter which is positioned within the housing and includes a trapping region for trapping cancer cells contained in the cell dispersion liquid. The filter is bonded to the housing, at least a part of the trapping region is formed of an observation region for observing the trapping region from the outside, the inlet line and the inlet opening are arranged at outer positions than the observation region when viewed from a normal line direction of the filter, and the inlet line is extended along an in-plane direction of the filter.

An inertial sensing system includes a magneto-optical trap (MOT) that traps atoms within a specified trapping region. The system also includes a cooling laser that cools the trapped atoms so that the atoms remain within the specified region for a specified amount of time. The system further includes a light-pulse atom interferometer (LPAI) that performs an interferometric interrogation of the atoms to determine phase changes in the atoms. The system includes a controller that controls the timing of MOT and cooling laser operations, and controls the timing of interferometric operations to substantially recapture the atoms in the specified trapping region. The system includes a processor that determines the amount inertial movement of the inertial sensing system based on the determined phase changes in the atoms. Also, a method of inertial sensing using this inertial sensing system includes recapture of atoms within the MOT following interferometric interrogation by the LPAI.

Provided is a cell trapping device with which a cell trapped on a filter can be observed without having to disassemble the device. The present invention comprises: a housing (120) that includes an inlet (130) to which an inlet pipe (125) is connected for the inflow of a cell dispersion liquid, and an outlet (140) to which an outlet pipe (135) is connected for the outflow of the cell dispersion liquidand a filter (105) that is disposed in the housing (120) and comprising a trapping region to trap a cancer cell in the cell dispersion liquid. The filter (105) is coupled with the housing (120). At least a portion of the trapping region serves as an observation region for the observation of the trapping region from outside. The inlet pipe (125) and the inlet (130) are disposed at a position further outward than the observation region when viewed in a normal direction of the filter (105). The inlet pipe (125) extends in an in-plane direction of the filter (105).

A thermally protective coveralls style suit having a plurality of separate water trapping regions between the suit and a user. The suit has a front slide fastener from crotch to neck with water entry retarding arm closures at the wrists and leg closures at ankles or thighs forming water trapping regions, leaving hands and feet free for swimming. Upper and lower chest straps cooperate forming water trapping regions by blocking pocket or water exchange between upper and lower torso regions. Permissive water entry at wrists, ankles or thighs, and neck or face, without circulation or exchange to surrounding water, allows separate pockets or thin film layers of water in the upper, lower, and central torso regions to insulate the body somewhat like a wetsuit where a single film provides insulation. An optional hood is provided to form another pocket or thin film layer without water circulation. Floatation pads assist buoyancy. A jacket embodiment is truncated at the lower chest strap.

A solar cell includes a transparent upper electrode for conducting electrons and for allowing incoming photons of light to pass therethrough. An exciton trapping region is disposed proximate the upper electrode, and includes graphene and an exciton trapping dye. The trapping dye traps captured excitons, and the graphene rapidly conducts freed electrons therefrom to the upper electrode. A pigment layer, in close proximity to the exciton trapping region, includes one or more pigment dyes that absorb light photons and emit excitons for transmission to the trapping dye. Excitons emitted by a first pigment dye can further trigger emission of excitons by a second pigment dye. A backing electrode is electrically coupled to the pigment layer via an anionic polyelectrolyte for transporting electrons to the pigment layer to replenish electrons conducted by the transparent upper electrode.