Patent Application
20180005795
This section is intended to introduce the reader to various aspects of art that may be related to various aspects of the present disclosure, which are described and/or claimed below. This discussion is believed to be helpful in providing the reader with background information to facilitate a better understanding of the various aspects of the present disclosure. Accordingly, it should be understood that these statements are to be read in this light, and not as admissions of prior art.
A variety of medical diagnostic, laboratory, security screening, and industrial quality control imaging systems, along with certain other types of systems (e.g., radiation-based treatment systems), utilize X-ray tubes as a source of radiation during operation. Typically, the X-ray tube includes a cathode and an anode. An electron beam emitter within the cathode emits a stream of electrons toward an anode that includes a target that is impacted by the electrons.
A large portion of the energy deposited into the target by the electron beam produces heat within the target, with another portion of the energy resulting in the production of X-ray radiation. Indeed, only about 1% of the energy from the electron beam X-ray target interaction is responsible for X-ray generation, with the remaining 99% resulting in heating of the target. The X-ray flux is, therefore, highly dependent upon the amount of energy that can be deposited into the source target by the electron beam within a given period of time. However, the relatively large amount of heat produced during operation, if not mitigated, can damage the X-ray source (e.g., melt the target). Accordingly, conventional X-ray sources are typically cooled by either rotating or actively cooling the target. However, when rotation is the means of avoiding overheating, the amount of deposited heat along with the associated X-ray flux is limited by the rotation speed (RPM), target heat storage capacity, radiation and conduction cooling capability, and the thermal limit of the supporting bearings. Tubes with rotating targets also tend to be larger and heavier than stationary target tubes. When the target is actively cooled, such cooling generally occurs relatively far from the electron beam impact area, which in turn significantly limits the electron beam power that can be applied to the target. In both situations, the restricted heat removal ability of the cooling methods markedly lowers the overall flux of X-rays that are generated by the X-ray tube.
Certain embodiments commensurate in scope with the originally claimed subject matter are summarized below. These embodiments are not intended to limit the scope of the claimed subject matter, but rather these embodiments are intended only to provide a brief summary of possible embodiments. Indeed, the invention may encompass a variety of forms that may be similar to or different from the embodiments set forth below.
In one implementation, an X-ray source is provided. In such an implementation, the X-ray source includes: an emitter configured to emit an electron beam and a target configured to generate X-rays when impacted by the electron beam. The target includes a thermally-conductive substrate; two or more X-ray generating layers, wherein X-ray generating layers are separated by at least one intervening thermally-conductive layer; and one or more interface layers formed between a respective X-ray generating layer and one or both of the first thermally conductive layer or a respective intervening thermally-conductive layer.
In a further implementation, an X-ray source is provided. In such an implementation, the X-ray source includes: an emitter configured to emit an electron beam and a target configured to generate X-rays when impacted by the electron beam. The target includes: a first thermally-conductive layer; a first interface layer formed over the first thermally-conductive layer; a first X-ray generating layer formed over the first interface layer; a second thermally-conductive layer formed over the first X-ray generating layer; a second interface layer formed over the second thermally-conductive layer; and a second X-ray generating layer formed over the second interface layer.
In a further implementation, an X-ray source is provided. In such an implementation, the X-ray source includes: an emitter configured to emit an electron beam and a target configured to generate X-rays when impacted by the electron beam. The target includes: a first thermally-conductive layer; a first X-ray generating layer formed over the first thermally-conductive layer; a first interface layer formed over the first X-ray generating layer; a second thermally-conductive layer formed over the first interface layer; and a second X-ray generating layer formed over the second thermally-conductive layer.
These and other features, aspects, and advantages of the present invention will become better understood when the following detailed description is read with reference to the accompanying drawings in which like characters represent like parts throughout the drawings, wherein:
One or more specific embodiments will be described below. In an effort to provide a concise description of these embodiments, all features of an actual implementation may not be described in the specification. It should be appreciated that in the development of any such actual implementation, as in any engineering or design project, numerous implementation-specific decisions must be made to achieve the developers' specific goals, such as compliance with system-related and business-related constraints, which may vary from one implementation to another. Moreover, it should be appreciated that such a development effort might be complex and time consuming, but would nevertheless be a routine undertaking of design, fabrication, and manufacture for those of ordinary skill having the benefit of this disclosure.
When introducing elements of various embodiments of the present invention, the articles “a,” “an,” “the,” and “said” are intended to mean that there are one or more of the elements. The terms “comprising,” “including,” and “having” are intended to be inclusive and mean that there may be additional elements other than the listed elements. Furthermore, any numerical examples in the following discussion are intended to be non-limiting, and thus additional numerical values, ranges, and percentages are within the scope of the disclosed embodiments.
As noted above, the X-ray flux produced by an X-ray source may depend on the energy and intensity of an electron beam incident on the source's target region. The energy deposited into the target produces, in addition to the X-ray flux, a large amount of heat. Accordingly, during the normal course of operation, a source target is capable of reaching temperatures that, if not tempered, can damage the target. The temperature rise, to some extent, can be managed by convectively cooling, also referred to as “direct cooling”, the target. However, such cooling is macroscopic and does not occur immediately adjacent to the electron beam impact area where damage i.e. melting, can occur. Without microscopic localized cooling, the overall flux of X-rays produced by the source is limited, potentially making the source unsuitable for certain applications, such as those requiring high X-ray flux densities. Rotating the target such that the electron beam distributes the energy over a larger area can reduce the target temperature locally but it typically requires larger evacuated volumes and the additional complexity of rotating components such as bearings. Further, vibrations associated with rotating targets become prohibitive for high resolution applications where the required spot size is on the order of the amplitude of the vibration. Accordingly, it would be desirable if the source could be operated in a substantially continuous basis in a manner that enables the output of high X-ray flux.
One approach for addressing thermal build-up is to use a layered X-ray source having one or more layers of thermal-conduction material (e.g., diamond) disposed in thermal communication with one or more layers of an X-ray generating material (e.g., tungsten). The thermal-conduction materials that are in thermal communication with the X-ray generating materials generally have a higher overall thermal conductivity than the X-ray generating material. The one or more thermal-conduction layers may generally be referred to as “heat-dissipating” or “heat-spreading” layers, as they are generally configured to dissipate or spread heat away from the X-ray generating materials impinged on by the electron beam to enable enhanced cooling efficiency. The interfaces between X-ray generating and thermal-conduction layers are roughened to improve adhesion between the adjacent layers. Having better thermal conduction within the source target (i.e., anode) allows the end user to operate the source target at higher powers or smaller spot sizes (i.e., higher power densities) while maintaining the source target at the same target operational temperatures. Alternatively, the source target can be maintained at lower temperatures at the same X-ray source power levels, thus increasing the operational lifetime of the source target. The former option translates into higher throughput as higher X-ray source power results in quicker measurement exposure times or improved feature detectability as smaller spot sizes results in smaller features being distinguishable. The latter option results in lower operational (variable) expenses for the end user as targets or tubes (in the case where the target is an integral part of the tube) will be replaced at a lower frequency.
One challenge for implementing such a multi-layered target is delamination of the layers, such as at the tungsten/diamond interface, due to weak adhesion and high stress levels within the layers. As discussed herein, various approaches for improving adhesion between layers and/or reducing internal stress levels in a multi-layer X-ray target are provided. In accordance with certain aspects of these approaches, material density within one or more of the layers may be graded (e.g., have a gradient stress or density profile) or otherwise varied, such as via varying deposition conditions to reduce internal stress within the layer. These effects may vary based on the deposition technique employed and the parameters, either constant or varied, during the deposition. For example, varying deposition parameters in chemical vapor deposition (CVD) and sputtering have varying degrees of influence on the stress and density of the deposited material. Thus, deposition technique and corresponding parameters may be selected so as to obtain the desired internal stress and/or density profile. For example, more energetic processes, such as sputtering or some forms of plasma CVD, can have a large effect on stress within the deposited material.
In addition, in some instances a layer or surface may be etched or otherwise roughened prior to deposition of a subsequent layer in order to improve adhesion between the layers. In addition, in certain implementations one or more interlayers (such as a carbide interlayer) may be deposited between X-ray generating and thermal-conduction layers to improve adhesion, such as to facilitate or provide chemical bonding. With respect to the various deposition steps discussed herein, any suitable deposition technique for a given layer and/or material (e.g., ion-assisted sputtering deposition, chemical vapor deposition, plasma vapor deposition, electro-chemical deposition, and so forth) may be employed.
Multi-layer x-ray sources as discussed herein may be based on a stationary (i.e., non-rotating) anode structure or a rotating anode structure and may be configured for either reflection or transmission X-ray generation. As used herein, a transmission-type arrangement is one in which the X-ray beam is emitted from a surface of the source target opposite the surface that is subjected to the electron beam. Conversely, in a reflection arrangement, the angle at which X-rays leave the source target is typically acutely angled relative to the perpendicular to the source target. This effectively increases the X-ray density in the output beam, while allowing a much larger thermal spot on the source target, thereby decreasing the thermal loading of the target.
By way of an initial example, in one implementation an electron beam passes through a thermally conductive layer (e.g., a diamond layer) and is preferentially absorbed by an underlying X-ray generating (e.g., tungsten) layer. Alternatively, in other implementations an X-ray generating layer may be the first (i.e., top) layer, with a thermally-conductive layer underneath. In both instances, additional alternating layers of X-ray generating and thermally-conductive material may be provided as a stack within the X-ray source target (with either the X-ray generating or thermally-conductive layer on top), with successive alternating layers adding X-ray generation and thermal conduction capacity. As will be appreciated, the thermally conductive and X-ray generating layers do not need to be the same thickness (i.e., height) with respect to the other type of layer or with respect to other layers of the same type. That is, layers of the same type or of different types may differ in thickness from one another. The final layer on the target can be either the X-ray generating layer or the thermally-conductive layer.
With the preceding in mind, and referring to
The subject may, for example, attenuate or refract the incident X rays 16 and produce the projected X-ray radiation 20 that impacts a detector 22, which is coupled to a data acquisition system 24. It should be noted that the detector 22, while depicted as a single unit, may include one or more detecting units operating independently or in conjunction with one another. The detector 22 senses the projected X-rays 20 that pass through or off of the subject 18, and generates data representative of the radiation 20. The data acquisition system 24, depending on the nature of the data generated at the detector 22, converts the data to digital signals for subsequent processing. Depending on the application, each detector 22 produces an electrical signal that may represent the intensity and/or phase of each projected X-ray beam 20. While the depicted system 10 depicts the use of a detector 22, in certain implementations the produced X-rays 16 may not be used for imaging or other visualization purposes and may instead be used for other purposes, such as radiation treatment of therapy. Thus, in such contexts, no detector 22 or data acquisition subsystems may be provided.
An X-ray controller 26 may govern the operation of the X-ray source 14 and/or the data acquisition system 24. The controller 26 may provide power and timing signals to the X-ray source 14 to control the flux of the X-ray radiation 16, and to control or coordinate with the operation of other system features, such as cooling systems for the X-ray source, image analysis hardware, and so on. In embodiments where the system 10 is an imaging system, an image reconstructor 28 (e.g., hardware configured for reconstruction) may receive sampled and digitized X-ray data from the data acquisition system 24 and perform high-speed reconstruction to generate one or more images representative of different attenuation, differential refraction, or a combination thereof, of the subject 18. The images are applied as an input to a processor-based computer 30 that stores the image in a mass storage device 32.
The computer 30 also receives commands and/or scanning parameters from an operator via a console 34 that has some form of operator interface, such as a keyboard, mouse, voice activated controller, or any other suitable input apparatus. An associated display 40 allows the operator to observe images and other data from the computer 30. The computer 30 uses the operator-supplied commands and parameters to provide control signals and information to the data acquisition system 24 and the X-ray controller 26.
Referring now to
The electron beam 52 incident on the X-ray generating material 56 generates X-rays 16 that are directed toward the detector 22 and which are incident on the detector 22, the optical spot 23 being the area of the focal spot projected onto the detector plane. The electron impact area on the X-ray generating material 56 may define a particular shape, thickness, or aspect ratio on the source target (i.e., anode 54) to achieve particular characteristics of the emitted X-rays 16. For example, the emitted X-ray beam 16 may have a particular size and shape that is related to the size and shape of the electron beam 52 when incident on the X-ray generating material 56. Accordingly, the X-ray beam 16 exits the source target 54 from an X-ray emission area that may be predicted based on the size and shape of the impact area. In the depicted example the angle between the electron beam 52 and the normal to the target is defined as α. The angle β is the angle between the normal of the detector and the normal to the target. Where b is the thermal focal spot size at the target region 56 and c is optical focal spot size, b=c/cos β. Further, in this arrangement, the equivalent target angle is 90-β.
As discussed herein, certain implementations employ a multi-layer source target 54 having two or more X-ray generating layers in the depth or z-dimension (i.e., two or more layers incorporating the X-ray generating material) separated by respective thermally conductive layers (including top layers and/or substrates 58). Such a multi-layer source target 54 (including the respective layers and/or intra-layer structures and features discussed herein) may be fabricated using any suitable technique, such as suitable semiconductor manufacturing techniques including vapor deposition (such as chemical vapor deposition (CVD), sputtering, atomic layer deposition), chemical plating, ion implantation, or additive or reductive manufacturing, and so on. In particular, certain fabrication approaches discussed herein may be utilized to make a multi-layer source target 54.
Referring again to
It should be noted that the different thermally-conductive layers, structures, or regions within a source target 54 may have correspondingly different thermally-conductive compositions, different thicknesses, and/or may be fabricated differently from one another, depending on the respective thermal conduction needs at a given region within the source target 54. However, even when differently composed, such regions, if formed so as to conduct heat from the X-ray generating materials, still constitute thermally-conductive layers (or regions) as used herein. For the purpose of the examples discussed herein, diamond is typically referenced as the thermally-conductive material. It should be appreciated however that such reference is merely employed by way of example and to simplify explanation, and that other suitable thermally-conductive materials, including but not limited to those listed above, may instead be used as a suitable thermally-conductive material.
As discussed herein, in various implementations respective depth (in the z-dimension) within the source target 54 may determine the thickness of an X-ray generating layer found at that depth, such as to accommodate the electron beam incident energy expected at that depth. That is, X-ray generating layers or regions at different depths within a source target 54 may be formed so as to have different thicknesses. Similarly, depending on heat conduction requirements at a given depth, the differing thermal-conductive layers may also vary in thickness, either based upon their depth in the source target 54 or for other reasons related to optimizing heat flow and conduction.
By way of example of these concepts,
With the preceding in mind, and as noted above, one issue in fabricating and using multi-layer X-ray source targets 54 is the delamination of different layers of the source target 54. To address these delamination issues, and as discussed in greater detail below, adhesion between X-ray generating layers (e.g., tungsten layers) and thermal-conduction layers (e.g., diamond layers) is improved via one or more of mechanical or structural approaches, chemical approaches, and/or use of one or more interface layers. By way of example, mechanical adhesion improvements may include increasing surface area of the X-ray generating layer (e.g., tungsten) for a higher degree of interlocking at the micrometer-level between the X-ray generating and thermal conduction layers.
In other approaches, an interface layer may be optionally provided between X-ray generating and thermally-conductive layers to promote bonding between the layers. For example, improved bonding between diamond and tungsten layers may be accomplished by depositing a thin carbide layer, such as tungsten carbide, between tungsten and diamond layers. In such an approach, the carbide interlayer provides a chemical bonding of the diamond and tungsten layers and serves as a barrier layer that limits the inter-diffusion of tungsten and carbon. The tungsten carbide layer can be formed by treating the tungsten surface in a carbon rich environment at high temperatures, by depositing diamond on a tungsten layer at high temperatures using a CVD method, for example, or by post-deposition annealing. In an example of such an approach, it may be desirable that the tungsten carbide layer has the tungsten carbide stoichiometry with a thickness of approximately 100 nm to minimize local heating. In addition to tungsten carbide, other carbides such as silicon carbide, titanium carbide, tantalum carbide, and so forth can be used to improve adhesion between tungsten and diamond layers.
In addition, in certain implementations a non-carbide interlayer can be deposited or formed on the carbide interlayer to further limit carbide growth at the interface. The attributes of this non-carbide interlayer, when present, are ductile behavior (by itself or alloyed with tungsten) and little or no carbide formation in a carbon rich environment. Examples of materials suitable for forming such a non-carbide interlayer include, but are not limited to: rhenium, platinum, rhodium, iridium, and so forth.
With these approaches in mind,
In the present examples,
In
As will be appreciated, the respective examples shown in
As discussed herein, other aspects of the fabrication process may also be controlled so as to reduce or eliminate delamination. By way of example, the layer deposition processes may also play a role in addressing delamination. For instance, conventional sputtering or ion-assisted sputtering techniques can be used to deposit a tungsten film with desired stress profiles in the film to reduce internal stress within the layer. In particular, the level of stress can be controlled by deposition pressure and power. To achieve better film conformality and reduce the overall stress in the tungsten film, one may initiate the deposition at a lower pressure, then increase the pressure as the deposition progresses to either partially or completely relieve the internal stress. Alternatively, one may initiate the deposition at a lower pressure, increase the pressure as the deposition progresses to either partially or completely relieve the stress, then increase the pressure near the end of the deposition to further tailor the stress profile so that the stress in the film and tungsten density are high at both interfaces but low in the middle of the film. Similarly, deposition temperature may be adjusted in addition to or instead of pressure to achieve the desired internal stress profile. Such deposition and/or temperature mediated internal stress profiles are also depicted in the context of
Additionally, ion assisted sputtering can be used to increase the film density as well as atom intermingling at the interface so as to assure good contact and adhesion between two dissimilar materials at the interface. Furthermore, biasing the substrate during growth independently can increase this intermingling while having deposition under low stress deposition conditions.
Further, CVD can also be used to fabricate the X-ray generating (e.g., tungsten) films. In particular, chemical vapor deposition produces films conformal to a rough surface as it is a non-line-of-sight deposition technique. Thus, it may be used in deposition steps such as those shown in
With the preceding discussion in mind,
In the depicted example, a diamond substrate 98 is initially provided and this substrate 98 undergoes a cleaning process 100 to prepare the surface of the substrate 98 for further processing. In the depicted example, the surface of the diamond substrate undergoes roughening operation 102.
In the depicted example, an optional interlayer deposition step 106 may be performed on the diamond surface at either room temperature or elevated temperatures by plasma vapor deposition, RF sputtering, or other suitable film deposition techniques. By way of example, the interlayer can be a carbide layer only, or a combination of a carbide layer followed by a non-carbide ductile layer (by itself or alloyed with tungsten).
A layer of tungsten is then deposited (step 108) on the interlayer covered diamond substrate at either room temperature or elevated temperatures by plasma vapor deposition, RF sputtering, or other suitable film deposition techniques. In one plasma vapor deposition implementation the conditions of the operation are changed over time so as to vary the stress and the density of the deposited tungsten layer, such as creating a density gradient from higher density to lower as deposition proceeds. By way of example, the first stage of the deposition is conducted at a lower pressure, resulting in approximately 0.1 μm of tungsten being deposited, the second stage of the deposition is conducted at an intermediate pressure, resulting in approximately 1.0 μm of tungsten being deposited, and the third stage of the deposition is conducted at a higher pressure, resulting in approximately 10 μm of tungsten being deposited, with the tungsten deposited in the different stages being at different densities. Thus, at the end of step 108, a roughened diamond substrate is present on which a layer of tungsten has been deposited having a graded or gradient density profile.
A determination may be made (block 110) as to whether additional diamond and tungsten and diamond layers are to be added to the multi-layer source target being fabricated. If no additional layers are to be added, the stack is subjected to a curing step 126 to set or cure the layered assembly.
If more layers are to be added, the process returns to optional curing step 112 in preparation for the next film deposition step. In the depicted example, the diamond substrate and tungsten layer may, optionally, be cured under suitable conditions.
In the depicted example, an additional optional interlayer deposition step 114 may be performed on the tungsten surface at either room temperature or elevated temperatures by plasma vapor deposition, RF sputtering, or other suitable film deposition techniques. By way of example, the interlayer can be a non-carbide ductile layer (by itself or alloyed with tungsten) followed by a carbide layer formed the tungsten surface.
In the depicted example, the tungsten deposition 108 (or optional interlayer 114 and curing step 112) is followed by a surface preparation step 116 performed on the surface. In one implementation, the surface preparation step 116 involves a mechanical or chemical roughening process, or a combination of the two.
At step 118 a diamond deposition is performed on the roughened tungsten surface. In one implementation, the CVD diamond deposition involves exposing the roughened tungsten surface to a mixture of gases such as methane (or other carbon-containing gas species), hydrogen, and nitrogen at high temperature until the diamond film reaches a thickness of approximately 8 μm to 15 μm. The desired diamond thickness depends on the incident beam energy and cross section. In this case the beam energy is 300 keV and the cross section is elliptical with an average diameter of 50 μm.
A determination may be made (block 120) as to whether an additional tungsten layer is to be added to the multi-layer source target being fabricated. If no additional tungsten layer is to be added, the stack is instead cured at step 126 to set or cure the layered assembly.
An optional roughening and cleaning step 122 may be performed if additional layers (such as additional tungsten and diamond layers) are to be fabricated on top of the diamond layer so as to improve mechanical adherence and decrease delamination. Conversely, if no additional layers are to be fabricated on the diamond layer, step 122 may be omitted.
In the depicted example, an optional interlayer deposition step 124 may be performed on the diamond surface at either room temperature or elevated temperatures by plasma vapor deposition, RF sputtering, or other suitable film deposition techniques. By way of example, the interlayer can be a carbide layer only, or a combination of a carbide layer followed by a non-carbide ductile layer (by itself or alloyed with tungsten).
Upon completion steps 122 and 124, the multilayer stack goes back to step 108 for additional film deposition and treatment until the desired number of tungsten layers and diamond layers are reached.
If no additional layers are to be added, the stack of layers is instead subjected to a curing step 126 to set or cure the layered assembly.
As part of the X-ray source target fabrication, the multi-layer target assembly fabricated in accordance with these steps may be brazed (step 128) to a copper target and the excess brazing material removed. An identifier may be laser scribed (step 130) on the copper target as part of this fabrication process.
Technical effects of the invention include providing a multi-layer X-ray source target having increased heat dissipation in the target that allows increased X-ray production and/or smaller spot sizes. Increased X-ray production allows for faster scan times for inspection. Further, increased X-ray production would allow one to maintain dose for shorter pulses in the case where object motion causes image blur. Smaller spot sizes allow higher resolution or smaller feature detectability. In addition, the technology increases the throughput and resolution of X-ray inspection, and reduces the cost.
This written description uses examples to disclose the invention, including the best mode, and also to enable any person skilled in the art to practice the invention, including making and using any devices or systems and performing any incorporated methods. The patentable scope of the invention is defined by the claims, and may include other examples that occur to those skilled in the art. Such other examples are intended to be within the scope of the claims if they have structural elements that do not differ from the literal language of the claims, or if they include equivalent structural elements with insubstantial differences from the literal languages of the claims.
This application is a continuation of U.S. patent application Ser. No. 15/199,524, entitled “Multi-Layer X-Ray Source Target”, filed Jun. 30, 2016, which is herein incorporated by reference in its entirety for all purposes.
| Number | Date | Country | |
|---|---|---|---|
| Parent | 15199524 | Jun 2016 | US |
| Child | 15487236 | US |
