192 results about "Voltage contrast" patented technology

Disclosed is a semiconductor die having a lower test structure formed in a lower metal layer of the semiconductor die. The lower conductive test structure has a first end and a second end. The first end is coupled to a predetermined voltage level. The semiconductor die also includes an insulating layer formed over the lower metal layer. The die further includes an upper test structure formed in an upper metal layer of the semiconductor die. The upper conductive test structure is coupled with the second end of the lower conductive test structure. The upper metal layer is formed over the insulating layer. In a specific implementation, the first end of the lower test structure is coupled to ground. In another embodiment, the semiconductor die also includes a substrate and a first via coupled between the first end of the lower test structure and the substrate. In yet another aspect, the lower test structure is an extended metal line, and the upper test structure is a voltage contrast element. Methods for inspecting and fabricating such semiconductor die are also disclosed.

A multi-column electron beam inspection system is disclosed herein. The system is designed for electron beam inspection of semiconductor wafers with throughput high enough for in-line use. The system includes field emission electron sources, electrostatic electron optical columns, a wafer stage with six degrees of freedom of movement, and image storage and processing systems capable of handling multiple simultaneous image data streams. Each electron optical column is enhanced with an electron gun with redundant field emission sources, a voltage contrast plate to allow voltage contrast imaging of wafers, and an electron optical design for high efficiency secondary electron collection.

Disclosed is a semiconductor die having an upper layer and a lower layer. The die includes a lower test structure formed in the lower metal layer of the semiconductor die. The lower conductive test structure has a first end and a second end, wherein the first end is coupled to a predetermined voltage level. The die also has an insulating layer formed over the lower metal layer and an upper test structure formed in the upper metal layer of the semiconductor die. The upper conductive test structure is coupled with the second end of the lower conductive test structure, and the upper metal layer being formed over the insulating layer. The die further includes at least one probe pad coupled with the upper test structure. Preferably, the first end of the lower test structure is coupled to a nominal ground potential. In another implementation, the upper test structure is a voltage contrast element. In another embodiment, a semiconductor die having a scanning area is disclosed. The semiconductor die includes a first plurality of test structures wherein each of the test structures in the first plurality of test structures is located entirely within the scanning area. The die includes a second plurality of test structures wherein each of the test structures in the first plurality of test structures is located only partially within the scanning area. The first plurality of test structures or the second plurality of test structures has a probe pad coupled to at least one test structure.

Semiconductor integrated test structures are designed for electron beam inspection of semiconductor wafers. The test structures include pattern features that are formed in designated test regions of the wafer concurrently with pattern features of integrated circuits formed on the wafer. The test structures include conductive structures that are designed to enable differential charging between defective and non-defective features (or defective and non-defection portions of a given feature) to facilitate voltage contrast defect detection of CMOS devices, for example, using a single, low energy electron beam scan, notwithstanding the existence of p/n junctions in the wafer substrate or other elements/features.

A new test structure to locate bridging defects in a conductive layer of an integrated circuit device is achieved. The test structure comprises a line comprising a conductive layer overlying a substrate. The line is coupled to ground. A plurality of rectangles comprises the conductive layer. The rectangles are not connected to the line or to other rectangles. Near edges of the rectangles and of the line are parallel. The rectangles are floating. The test structure is used with a passive voltage contrast test in a scanning electron microscope. A test structure and method to measure critical dimensions is disclosed.

A test structure and method thereof for determining a defect in a sample of semiconductor device includes at least one transistor rendered grounded. The grounded transistor is preferably located at least one end of a test pattern designed to be included in the sample. When the test structure is inspected by charged particle beam inspection, the voltage contrast (VC) of the transistors in the test pattern including the grounded transistor is observed for determination of the presence of defect in the sample.

Disclosed are techniques for efficiently inspecting defects on voltage contrast test. In one embodiment, methodologies and test structures allow inspection to occur entirely within a charged particle system. In a specific embodiment, a method of localizing and imaging defects in a semiconductor test structure suitable for voltage contrast inspection is disclosed. A charged particle beam based tool is used to determine whether there are any defects present within a voltage contrast test structure. The same charged particle beam based tool is then used to locate defects determined to be present within the voltage contrast test structure. Far each localized defect, the same charged particle beam based tool may then be used to generate a high resolution image of the localized defect whereby the high resolution image can later be used to classify the each defect. In one embodiment, the defect's presence and location are determined without rotating the test structure relative to the charged particle beam.

A method for determination of tunnel oxide weakness is provided. A tunnel oxide layer is formed on a semiconductor wafer. At least one poly gate is formed on the tunnel oxide layer in a flash memory region of the semiconductor wafer. At least one poly island, which is substantially larger than the poly gate, is formed on the tunnel oxide layer in a voltage contrast cell region of the semiconductor wafer. The poly island and the tunnel oxide layer therebeneath form a voltage contrast tunnel oxide cell. A voltage contrast measurement is performed on the voltage contrast tunnel oxide cell. The voltage contrast measurement is then compared with prior such voltage contrast measurements on other such voltage contrast tunnel oxide cells. The tunnel oxide weakness of the tunnel oxide layer is then determined from the voltage contrast measurement comparisons.

An improved voltage contrast test structure is disclosed. In general terms, the test structure can be fabricated in a single photolithography step or with a single reticle or mask. The test structure includes substructures which are designed to have a particular voltage potential pattern during a voltage contrast inspection. For example, when an electron beam is scanned across the test structure, an expected pattern of intensities are produced and imaged as a result of the expected voltage potentials of the test structure. However, when there is an unexpected pattern of voltage potentials present during the voltage contrast inspection, this indicates that a defect is present within the test structure. To produce different voltage potentials, a first set of substructures are coupled to a relatively large conductive structure, such as a large conductive pad, so that the first set of substructures charges more slowly than a second set of substructures that are not coupled to the relatively large conductive structure. Mechanisms for fabricating such a test structure are also disclosed. Additionally, searching mechanisms for quickly locating defects within such a test structure, as well as other types of voltage contrast structures, during a voltage contrast inspection are also provided.

The electron beam is irradiated several times at predetermined intervals to the wafer surface on which the plugs are exposed in the course of the manufacturing process so that the pn junction is in the reverse bias state. Then, the irradiation conditions of the electron beam are changed while monitoring the charging voltage on the plug surface, and the secondary electron signals of the circuit pattern are obtained under the irradiation conditions that the charging is within a desired range, thereby evaluating the leakage property. Since the charging voltage of the pn junction is relaxed depending on the magnitude of the leakage current during the interval, the leakage property is evaluated based on the luminance signals of the voltage contrast image. By measuring the charging voltage and setting it within a desired range, the evaluation result reflects the state in the actual operation. Therefore, the accuracy is enhanced.