One embodiment relates to a solid-state charged-particle detector. The detector includes a PIN diode and a conductive coating on the front-side of the PIN diode, wherein the front-side receives incident charged particles to be detected. In addition, the detector includes a metal layer on the backside of the PIN diode and electrical connections to the metal layer and to the conductive coating. Other embodiment are also disclosed.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present disclosure relates to electron beam detection.

2. Description of the Background Art

One type of electron beam apparatus is a scanning electron microscope (SEM). SEMs obtain an image of a sample by scanning a primary electron beam over the sample and detecting secondary electrons emitted from the sample. The image may be used, for example, for inspection or measurement of a micropattern in a semiconductor device, or for other purposes.

SEMs typically employ scintillator-type detectors for detecting secondary electrons emitted from the object being observed. When electrons impact material within the scintillator-type detector, the material emits light. The light is detected by a photon detector, such as a photomultiplier tube, which converts the light into an electric signal.

It is highly desirable to improve electron detectors for scanning electron microscopes and other apparatus.

SUMMARY

One embodiment relates to a solid-state charged-particle detector. The detector includes a PIN diode and a conductive coating on the front-side of the PIN diode, wherein the front-side receives incident charged particles to be detected. In addition, the detector includes a metal layer on the backside of the PIN diode and electrical connections to the metal layer and to the conductive coating.

Another embodiment relates to a method of detecting electrons using a solid state detector. Electrons are received by a continuous conductive coating, and transmitted through the conductive coating to a PIN diode. Electron-hole pairs are generated within the diode, and an electrical current is formed through electrical connections to the conductive coating and to a backside metal layer.

Another embodiment pertains to a solid-state electron detector which includes at least the following: a PIN diode; a metal layer on the backside of the PIN diode; an oxide coating on the front-side of the PIN diode; a continuous conductive coating over the oxide coating; and electrical connections to the metal layer and to the conductive coating.

Another embodiment pertains to a solid-state electron detector which includes at least the following: a PIN diode; a metal layer on the backside of the PIN diode; an oxide coating on the front-side of the PIN diode; a continuous conductive coating over the oxide coating; conductive vias through the oxide coating; and electrical connections to the metal layer and to the conductive coating.

Other embodiments and features are also disclosed.

These drawings are used to facilitate the explanation of embodiments of the present invention. The drawings are not necessarily to scale.

DETAILED DESCRIPTION

FIG. 1is a cross-sectional diagram depicting a conventional solid-state detector100. The conventional solid-state detector100includes a silicon chip including a P+ doped region102near the front surface and an N+ doped region104near the back surface, and an intrinsic region106therebetween to form a PIN (positive-intrinsic-negative) diode. In some cases, the N+ and P+ regions may be reversed. The front surface is typically coated with a thin protective layer of silicon dioxide or silicon nitride (not shown). A backside metal layer108and a front-side metal contact110are connected to electrically (see electrical connections112). When incident photon radiation114of sufficiently high energy impinges upon the detector, electron-hole pairs are created in the semiconductor. The electron-hole pairs created in a depleted region separate and create an electrical current through the electrical connections112. Ideally, the electrical current produced is proportional to the incoming photon flux.

Disadvantages of Using Conventional Solid-State Detector to Detect Electrons

The speed of a detector relates to its response time, or the time needed to respond to the incoming radiation and produce an external current. In order to increase the speed of the detector, the area of the detector is conventionally decreased. However, as a detector's area becomes smaller, then its efficiency typically suffers. For example, under high intensity irradiation, a large voltage drop can develop across the diode which results in a saturation effect.

In order to maintain high efficiency, a large-area detector is desirable. Unfortunately, the speed of a large-area detector is limited by the combination of diode junction capacitance and resistance through the P+ and N+ collection regions. As such, there is a trade-off between detector speed and efficiency.

FIG. 2is a cross-sectional diagram depicting an electron detector200in accordance with a first embodiment of the invention. In this embodiment, the electron detector200comprises a PIN diode which includes a thin conductive coating202over the top surface (the surface receiving the incident electrons). The thickness of the coating202is preferably uniform over the top surface.

In the specific implementation illustrated, the thin conductive coating comprises an aluminum coating. Other metals or alloys may be used instead of Aluminum. Lighter element metals are preferred, such as Beryllium or Aluminum, since they have smaller cross sections for absorbing or scattering the incident electrons204. Alternatively, non-metal conductive materials may be used, such as graphite (which also has a small cross section for electrons). Unlike the conventional metal contact, the thin conductive coating202is applied over all or most of the top surface of the PIN diode.

As a first consideration, the thin conductive coating202is configured to be of a sufficient thickness so as to substantially lower a series resistance of the device. This advantageously results in a higher speed for the detector200because the speed is limited by the series resistance and the junction capacitance.

As a second consideration, the think conductive coating202is configured to be sufficiently thin so that a large fraction of the incident electrons204pass through the coating202and into the PIN diode. This advantageously maintains a high efficiency for the detector200.

The above two considerations determine the desirable thickness of the coating202; thick enough to lower the series resistance for displacement current in the coating, while not too thick so as to avoid blocking most of the incident electrons204from passing through the coating. As such, the device200advantageously combines high-speed and high-efficiency capabilities. The high-speed capability of the device200is reflected in its improved frequency response.

Furthermore, a substantial displacement current may flow through the conductive coating202to the top electrical connection. This advantageously enables the device200to be able to handle a high current density (i.e. a high flux density) of incident electrons.

Such a conductive coating202cannot be applied effectively to PIN detectors used to detect photons. This is because the conductive coating202would typically absorb photons.

In an alternate approach, instead of the thin conductive coating202covering most or all of the top surface, a conductive grid may be used for an electron detector. Such a conductive grid is used, for example, in solar cells which generate electrical current from sunlight. The conductive grid spans the top surface but has openings to large areas of the top surface.

White such a conductive grid may be used, applicants believe such a device has disadvantages when the device is used as an electron detector. One disadvantage is that there is a variation in speed relative to the position at which an incident electron beam impinges upon the detector. In other words, the speed depends on how close the electrons land to the grid lines. In addition, there is a variation in collection efficiency across the device that can result in image artifacts when used for some applications. For example, a shadow image of the metal grid may appear in some scanning electron microscope applications. Furthermore, if the conductive grid is of a material and/or thickness so as to scatter or absorb a large fraction of the incident electrons impinging upon the grid material, then there is a loss of efficiency or quantum yield due to the scattered or absorbed electrons.

FIG. 3is a cross-sectional diagram depicting an electron detector300in accordance with a second embodiment of the invention. In this embodiment, the electron detector comprises a PIN detector which includes a thin oxide coating302and a thin conductive coating202over the top surface.

In this embodiment, the inclusion of the oxide coating302between the top surface of the PIN diode and the conductive coating202creates a capacitative layer in series with the junction capacitance of the diode. At high frequencies, this series capacitance decreases the RC time delay of the device300, and so enables higher-speed operation of the electron detector.

FIG. 4is a cross-sectional diagram depicting an electron detector in accordance with a third embodiment of the invention. Similar to the second embodiment inFIG. 3, the embodiment inFIG. 4comprises a PIN detector with a thin oxide coating302and a thin conductive coating202over the top surface. In addition, this embodiment includes conductive vias402through the oxide coating302.

In this embodiment, the conductive vias402provide a path for electrical current to flow directly from the top surface of the diode to the conductive coating202. Together, the conductive vias402and the conductive coating202lower the series resistance of the device400. The lower series resistance further enables high-speed operation.

FIG. 5is a planar diagram depicting an example layout of a layer in the third embodiment of the invention. The depicted layer is the layer which includes conductive vias402through the thin oxide coating302. The layout shown inFIG. 5is just one example layout with the conductive vias402distributed over the area of the detector400. Various other layouts of the conductive vias402may also be utilized in other implementations.

The embodiments of the high-speed high-efficiency solid-state detector described above may be preferably configured with a detector size range (for example, diameter range) of about 5 millimeters (mm) or larger. For example, the detector diameter may be 5 mm, or 8 mm, or 40 mm, or larger.

The embodiments of the high-speed high-efficiency solid-state detector described above may also be preferably configured to operate in a frequency range from 50 megahertz (MHz) to 1 gigahertz (1 GHz). This high frequency range is enabled as discussed above.

While the above discussion relates to an incident beam which comprises electrons, the embodiments of the high-speed high-efficiency solid-state detector described above may also be applied to detect other charged particles, besides electrons.