Patent Description:
Superconducting quantum computing is an implementation of a quantum computer in superconducting electronic circuits. Quantum computation studies the application of quantum phenomena for information processing and communication. Various models of quantum computation exist, and the most popular models include the concepts of qubits and quantum gates. A qubit is a generalization of a bit that has two possible states, but can be in a quantum superposition of both states. A quantum gate is a generalization of a logic gate, however the quantum gate describes the transformation that one or more qubits will experience after the gate is applied on them, given their initial state. Various quantum phenomena, such as superposition and entanglement, do not have analogs in the world of classical computing and therefore may involve special structures, techniques, and materials. An example of prior art may be found in <CIT> which discloses providing a method for easily and inexpensively producing a NbAl alloy thin sheet for a superconductive material by lamination rolling without needing any special apparatus for forming, going through multiple working processes and needing any particular working condition.

According to a first aspect of the present invention, a superconductor device includes a first metal layer on top of a substrate. A second metal layer is on top of the first metal layer. A superconducting alloy of the first metal layer and the second metal layer is between the first metal layer and the second metal layer. There is no oxide layer between the superconducting alloy and the first metal layer.

According to the present invention, the first metal layer is Niobium (Nb), the second metal layer is Aluminum (Al), and the superconducting alloy is Al<NUM>Nb.

In one embodiment, an orientation of crystal grains of the superconducting alloy is substantially aligned with a (<NUM>) plane parallel to a surface of the substrate metal layer.

In one embodiment, there is an electrode on top of the second metal layer.

In one embodiment, the electrode is a Josephson Junction electrode.

In one embodiment, the superconducting alloy is operative to protect the first metal layer from oxidation or contamination that could affect a performance of the superconductor device.

According to another aspect of the present invention, a method of fabricating a superconductor device includes providing a first metal layer on top of a substrate. An oxidation of a top surface of the first metal layer is rejected. A second metal layer is deposited on top of the second metal layer. A superconducting alloy of the first metal layer and the second metal layer is created between the first metal layer and the second metal layer. There is no oxide layer between the superconducting alloy and the first metal layer.

In one embodiment, rejecting the oxidation of the top surface of the first metal layer includes the second metal layer being placed on top of the first metal layer before a top surface of the first metal layer is exposed to air, after the deposition of the first metal layer.

In one embodiment, rejecting the oxidation of the top surface of the first metal layer further includes maintaining the superconductor device in a vacuum between a deposition of the first metal layer and a deposition of the second metal layer.

In one embodiment, rejecting the oxidation of the top surface of the first metal layer includes the second metal layer being deposited on top of the first metal layer after a top surface of the first metal layer being exposed to air, and subsequent to a cleaning of the top surface of the first superconductor metal, to remove any oxidation therefrom.

In one embodiment, the second metal layer is etched away after the creation of the superconducting alloy.

In one embodiment, the creation of the superconducting alloy includes annealing the first metal layer and the second superconductor metal at a predetermined temperature.

In one embodiment, the superconducting alloy creates an electrical path from the first metal layer to the second metal layer.

In one embodiment, an orientation of a lattice of the superconducting alloy is (<NUM>), (<NUM>), or (<NUM>), depending on a temperature of an anneal of the first metal layer and the second metal layer, to create the superconducting alloy.

In one embodiment, an electrode is deposited on top of the second metal layer.

In one embodiment, the second metal layer is removed and an electrode is deposited on top of the superconducting alloy.

According to yet another aspect of the present invention, a method of fabricating a superconductor device includes providing a first metal layer on top of a substrate. An initial oxide layer is provided on a top surface of the first metal layer. A second metal layer is deposited on top of the second metal layer. A superconducting alloy of the first metal layer and the second metal layer is created between the first metal layer and the second metal layer. The initial oxide layer is moved to a top surface of the superconducting alloy during the creation of the superconducting alloy.

In one embodiment, the initial oxide on the top surface of the superconducting alloy and the second metal layer are removed. An electrode is deposited on top of the superconducting alloy.

These and other features will become apparent from the following detailed description of illustrative embodiments thereof, which is to be read in connection with the accompanying drawings.

The drawings are of illustrative embodiments. They do not illustrate all embodiments. Other embodiments may be used in addition or instead. Details that may be apparent or unnecessary may be omitted to save space or for more effective illustration. Some embodiments may be practiced with additional components or steps and/or without all the components or steps that are illustrated. When the same numeral appears in different drawings, it refers to the same or like components or steps.

In the following detailed description, numerous specific details are set forth by way of examples to provide a thorough understanding of the relevant teachings. However, it should be apparent that the present teachings may be practiced without such details. In other instances, well-known methods, procedures, components, and/or circuitry have been described at a relatively high-level, without detail, to avoid unnecessarily obscuring aspects of the present teachings.

In one aspect, spatially related terminology such as "front," "back," "top," "bottom," "beneath," "below," "lower," above," "upper," "side," "left," "right," and the like, is used with reference to the orientation of the Figures being described. Since components of embodiments of the disclosure can be positioned in a number of different orientations, the directional terminology is used for purposes of illustration and is in no way limiting. Thus, it will be understood that the spatially relative terminology is intended to encompass different orientations of the device in use or operation in addition to the orientation depicted in the figures. Thus, for example, the term "below" can encompass both an orientation that is above, as well as, below. The device may be otherwise oriented (rotated <NUM> degrees or viewed or referenced at other orientations) and the spatially relative descriptors used herein should be interpreted accordingly.

As used herein, the terms "lateral" and "horizontal" describe an orientation parallel to a first surface of a chip.

As used herein, the term "vertical" describes an orientation that is arranged perpendicular to the first surface of a chip, chip carrier, or semiconductor body.

As used herein, the terms "coupled" and/or "electrically coupled" are not meant to mean that the elements must be directly coupled together-intervening elements may be provided between the "coupled" or "electrically coupled" elements. In contrast, if an element is referred to as being "directly connected" or "directly coupled" to another element, there are no intervening elements present. The term "electrically connected" refers to a low-ohmic electric connection between the elements electrically connected together.

For example, a first element could be termed a second element, and, similarly, a second element could be termed a first element, without departing from the scope of example embodiments.

Example embodiments are described herein with reference to cross-sectional illustrations that are schematic illustrations of idealized or simplified embodiments (and intermediate structures). As such, variations from the shapes of the illustrations as a result, for example, of manufacturing techniques and/or tolerances, may be expected. Thus, the regions illustrated in the figures are schematic in nature and their shapes do not necessarily illustrate the actual shape of a region of a device and do not limit the scope.

It is to be understood that other embodiments may be used and structural or logical changes may be made without departing from the scope of the present invention defined by the claims. The description of the embodiments is not limiting. In particular, elements of the embodiments described hereinafter may be combined with elements of different embodiments.

As used herein, certain terms are used indicating what may be considered an idealized behavior, such as, for example, "lossless," "superconductor," or "superconducting," which are intended to cover functionality that may not be exactly ideal but is within acceptable margins for a given application. For example, a certain level of loss or tolerance may be acceptable such that the resulting materials and structures may still be referred to by these "idealized" terms.

The concepts herein relate to quantum technology and quantum chips. Regarding quantum technology, the electromagnetic energy associated with a qubit can be stored, for example, in so-called Josephson junctions and in the capacitive and inductive elements that are used to form the qubit. In other examples, there may be spin qubits coupled to resonators or topological qubits, microfabricated ion traps, etc. Other types of superconducting components are supported by the teachings herein as well, including (without limitation), circulators, isolators, amplifiers, filters, active control electronics such as rapid single flux quantum (RSFQ), etc..

In one example, to read out the qubit state, a microwave signal is applied to the microwave readout cavity that couples to the qubit at the cavity frequency. The transmitted (or reflected) microwave signal goes through multiple thermal isolation stages and low-noise amplifiers that are used to block or reduce the noise and improve the signal-to-noise ratio. The amplitude and/or phase of the returned/output microwave signal carries information about the qubit state, such as whether the qubit has dephased to the ground or excited state. The microwave signal carrying the quantum information about the qubit state is usually weak (e.g., on the order of a few microwave photons). Various circuits and techniques can be used to measure this weak signal. For example, low-noise quantum-limited amplifiers (QLAs), such as Josephson amplifiers and travelling-wave parametric amplifiers (TWPAs), may be used as preamplifiers at the output of the quantum system to boost the quantum signal, while adding the minimum amount of noise as dictated by quantum mechanics, in order to improve the signal to noise ratio of the output chain. In addition to Josephson amplifiers, certain Josephson microwave components that use Josephson amplifiers or Josephson mixers such as Josephson circulators, Josephson isolators, and Josephson mixers can be used in scalable quantum processors. Accordingly, Josephson Junctions are salient circuit elements of a superconducting quantum computer. A Josephson Junction may include a thin layer of insulator, sometimes referred to as a barrier or a tunnel barrier, between two layers of superconductor. The Josephson Junction acts as a superconducting tunnel junction.

A qubit system may include one or more readout resonators coupled to the qubit. A readout resonator may be a transmission line that includes a capacitive connection to ground on one side and is either shorted to the ground on the other side, such as for a quarter wavelength resonator, or may have a capacitive connection to ground, such as for a half wavelength resonator, which results in oscillations within the transmission line, with the resonant frequency of the oscillations being close to the frequency of the qubit. For example, the readout resonator affects a pulse coming from the control/measurement instruments at the readout resonator frequency. The pulse acts as a measurement that decoheres the qubit and makes it collapse into a state of "one" or "zero," thereby imparting a phase shift on that measurement pulse.

Between qubits there may be a coupling resonator, which allows coupling different qubits together in order to realize quantum logic gates. The coupling resonator is typically structurally similar to the readout resonator in that it is a transmission line that includes capacitive connections to ground on both sides, which also results in oscillations within the coupling resonator. When a qubit is implemented as a transmon, each side of the coupling resonator is coupled (e.g., capacitively or inductively) to a corresponding qubit by being in adequate proximity to (e.g., the capacitor of) the qubit. Since each side of the coupling resonator has coupling with a respective different qubit, the two qubits are coupled together through the coupling resonator. In this way, there is mutual interdependence in the state between coupled qubits, thereby allowing a coupling resonator to use the state of one qubit to control the state of another qubit. Entanglement occurs when the interaction between two qubits is such that the states of the two cannot be specified independently, but can only be specified for the whole system. In this way, the states of two qubits are linked together such that a measurement of one of the qubits, causes the state of the other qubit to collapse.

Typical materials to make the interconnects include, without limitation, niobium (Nb), aluminum (Al), niobium nitride (NbN), titanium nitride (TiN), niobium titanium nitride (NbTiN), etc., sometimes referred to herein as superconductors. It will be understood that other suitable materials that have superconducting properties can be used as well.

Applicants have recognized that to increase the computational power and reliability of a quantum computer in general, and superconductor structures in particular, improvements can be made in superconductor device structure and manufacture of the same. Achieving low error rates and better reliability is relevant, among other aspects, to manipulate qubit states accurately and perform sequential operations that provide consistent results and not merely unreliable data. Quantum technology is still a developing field and providing structures with highly predictable and more ideal performance is a challenge.

In one aspect, the teachings herein are based on Applicants' insight that protecting specific interfaces of superconductors used in superconducting quantum circuits from oxidation can improve the decoherence and signal integrity of superconducting qubits. Applicants have further recognized that directly applying conventional integrated circuit techniques for protecting materials from oxidation to superconducting quantum circuits may not be effective because of the unique challenges presented by quantum circuits that are not presented in classical computing architectures. Accordingly, embodiments of the present disclosure are further based on recognition that issues unique to quantum circuits have been taken in consideration when evaluating applicability of conventional integrated circuit techniques to building superconducting quantum circuits, and, in particular, to electing materials and processes used for protecting superconducting materials of such circuits from oxidation.

The surface of the superconductor of a quantum circuit include possible lossy material due to oxide growth or surface contamination that reduces the resonator quality. In this regard, <FIG> illustrates a first superconductor layer <NUM> on top of a substrate <NUM>. The surface oxide <NUM> may grow naturally and is therefore sometimes referred to herein as native oxide. As illustrated in <FIG>, when another superconductor layer <NUM> is placed on top (e.g., in the formation of a Josephson Junction), there is a remaining residual oxide <NUM>.

Contact between superconducting elements, for example a capacitor pad and a Josephson Junction electrode that may be implemented by superconductor layers <NUM> and <NUM>, is salient for good qubit performance. However, the residual oxides or surface contamination <NUM> in the contact area can lower qubit coherence. For example, semiconductor processes often involve different chambers for different depositions and vacuum is often broken, which immediately may result in the native oxide <NUM> discussed herein. One way of removing the native oxide <NUM> is by way of in situ cleaning (e.g., ion mill, sputter clean, vacuum bake, vapor HF, etc.,). However, there are limitations to the level of cleanliness that can be achieved. For example, Vapor HF is not typically done in vacuum (but can be), so the removal of oxide is followed by some time in air before load in a deposition chamber. Oxide formation may thus be limited but not eliminated. As to ion milling, it is performed in vacuum but, since it is a sputtering removal of oxide, it may also lead to some redeposition.

Accordingly, the teachings herein provide methods and systems of mitigating loss in contact superconductors of quantum circuits. The techniques described herein may be implemented in a number of ways. Example implementations are provided below with reference to the following figures.

Reference now is made to <FIG>, which is a simplified cross-section view of a superconducting structure <NUM>, consistent with an illustrative embodiment. Superconductor structure <NUM> can be used to implement various superconducting circuits, including, without limitation, a Josephson Junction (JJ), superconducting capacitors, circulators, isolators, amplifiers, filters, etc. To facilitate the present discussion, the superconducting structures herein will sometimes be discussed in the context of a JJ, while it will be understood that other superconducting structures are supported as well.

The superconductor structure <NUM> may include a substrate <NUM>. In various embodiments, the substrate <NUM> may comprise any suitable material or combination of materials, such as doped or undoped silicon, glass, dielectrics, etc. For example, the substrate may comprise a Silicon-on-insulator (SOI) structure, e.g., with a buried insulator layer, or a bulk material substrate, e.g., with appropriately doped regions, typically referred to as wells. In another embodiment, the substrate may be silicon with silicon oxide, nitride, or any other insulating films on top.

Other materials that may be used for the substrate include, without limitation, sapphire, aluminum oxide, germanium, gallium arsenide (GaAs) or any of the other III-V periodic table compounds, indium phosphide (InP), silicon carbide (SiC), a superconducting alloy of silicon and germanium, quartz, etc. Thus, as used herein, the term substrate <NUM> refers to a foundation upon which various superconducting structures can be built.

There is a superconducting first metal <NUM> on top of the substrate <NUM>. According to the present invention, the first metal layer <NUM> is niobium (Nb). There is a second metal layer <NUM> on top of the first metal layer <NUM>. According to the present invention, the second metal layer <NUM> is aluminum (Al). There is a superconducting alloy <NUM> of the first metal layer and the second metal layer between the first metal layer <NUM> and the second metal layer <NUM>. According to the present invention, the superconducting alloy is niobium aluminide Al<NUM>Nb. As used herein, the term niobium aluminides includes all stable aluminides present in a Nb-Al diagram. Niobium aluminide refers to any alloy of Al and Nb. Here three phases are possible: Al<NUM>Nb, AlNb<NUM> and NbsAl (i.e., the only three niobium aluminide phases present in the binary Nb-Al equilibrium phase diagram). Note, in embodiments having very thin films, it is possible that a non-stable Al-Nb phase could form with a crystal structure and composition not found in bulk phases.

In various embodiments, different grain orientations of the Al<NUM>Nb can be provided based on temperature and time conditions, discussed in more detail later. Significantly, there is no oxide layer between the superconducting alloy and the first metal layer <NUM> and the superconducting alloy <NUM>. Additionally, in one embodiment, there is no oxide layer between the second metal layer <NUM> and the superconducting alloy <NUM>.

Superconducting circuit elements, such as, without limitation, JJs, resonators, coupling pads, capacitor, gate electrodes, etc., are typically capped with a second conductor. In one embodiment, the second conductor (i.e., second metal layer <NUM>) is deposited on the first conductor (i.e., first metal layer <NUM>) before the first metal layer <NUM> is exposed to air to prevent oxidation thereon.

Alternatively, or in addition, the top surface of the first metal layer <NUM> is sufficiently cleaned before the second metal layer <NUM> is deposited. The two conducting layers comprising the first metal layer <NUM> and the second metal layer <NUM> are alloyed at their interface to create an electrical path from the base conductor (i.e., first metal layer <NUM>), through the superconducting alloy <NUM> and into the JJ electrode, represented in <FIG> by the second metal layer <NUM>. By virtue of not having an oxide layer between the metal layers <NUM> and <NUM>, as well as the superconducting alloy <NUM>, the quality of the contact improves (e.g., contact between the capacitor pad, represented by the second metal layer <NUM>, and the JJ <NUM> lead, for reduced loss), thereby producing a more ideal JJ. In various embodiments metal layer <NUM> can be a metal that is only used for creating the interfacial alloy <NUM>, in which case an electrode is deposited later. Alternatively, metal layer <NUM> could also be one (or even a double layer electrode) that is annealed later to form the superconducting alloy <NUM>. In some embodiments, the superconducting circuit is built before the anneal to form the interfacial alloy <NUM>.

With the foregoing description of an example superconductor structure <NUM>, it may be helpful to discuss an example process of manufacturing the same. To that end, <FIG> illustrate various steps in the manufacture of a superconductor structure, consistent with illustrative embodiments. More specifically, <FIG> illustrates a semiconductor structure 300A before formation of a superconducting alloy between metal layers, consistent with an illustrative embodiment. In various embodiments, the base first metal layer <NUM> is capped with the second metal layer <NUM> (i) either before air exposure or (ii) after air exposure, after which the native metal oxide is sufficiently removed before the second metal layer <NUM> coverage, collectively referred to herein as rejecting the native metal oxide. For example, in various embodiments, the second metal layer <NUM> is placed on top of the first metal layer <NUM> before oxidation occurs (e.g., while the chip is in a controlled environment, such as a vacuum, even when going from one deposition chamber to another) or by a sufficient cleaning of the top surface of the first metal layer <NUM> to remove any oxidation thereon before the second metal layer <NUM> is placed on top of the first metal layer <NUM>.

In various embodiments, this cleaning of the oxide from a top surface of the first metal layer <NUM> may be by way of wet clean or dry clean (preferred). Such dry cleaning may include, without limitation, ion milling, pre-sputter, or another appropriate technique to remove the oxide from the top of the first metal layer <NUM>. In this way, an interface without oxidation can be achieved. Accordingly, the interface between the first metal layer <NUM> and the second metal layer <NUM> is substantially free of oxide. A superconducting alloy is then formed between the two metal layers <NUM> and <NUM>, as discussed in more detail below.

<FIG> illustrates a semiconductor structure 300B after a superconducting alloy <NUM> is formed between the first metal layer <NUM> and the second metal layer <NUM>, consistent with an illustrative embodiment. In one embodiment, the superconducting alloy is formed by way of anneal. Other ways of creating the superconducting alloy <NUM> between the first metal layer <NUM> and the second metal layer <NUM> include, without limitation, a predetermined amount of pressure, and/or an increase of bias during the deposition of the second metal layer <NUM>.

According to the present invention, the first metal layer <NUM> is niobium (Nb), the second metal layer <NUM> is aluminum (Al) and the resulting alloy <NUM> between these two metals is niobium aluminide Al<NUM>Nb(<NUM>), where (<NUM>) is the lattice orientation of the superconducting alloy <NUM> with respect to the <NUM> planes of the Nb and in this case the surface of the substrate.

In various embodiments, depending on the different superconducting structure that is to be created, the second metal layer <NUM> can be kept or etched away by way of wet or dry (plasma) etching. Thus, the unreacted second metal layer <NUM> can remain or be removed, selectively leaving the metal alloy <NUM> exposed, where the metal alloy <NUM> protects the first metal layer <NUM> from reactions with the ambient environment. By virtue of creating the metal alloy <NUM>, the first metal layer <NUM> is protected from oxidation or other elements that could affect the performance of the superconductor devices of the first metal layer <NUM>, thereby improving device performance.

<FIG> illustrate a semiconductor structures 300C and 300D that include an electrode <NUM> on top of the second metal layer <NUM>, and one directly on the superconducting alloy <NUM>, respectively, consistent with illustrative embodiments. For example, the junction electrode <NUM> may belong to a JJ. The JJ could be on the capacitor (i.e. formed by a subtractive etch) or on the substrate which is connected to the capacitor by the junction electrode (i.e. Dolan shadow junction build). Trilayer junction processes can be used, for example, for the fabrication of JJ logic devices and integrated circuits. For example, the junction electrode <NUM> would have a thin layer of oxide on top of it, which would be covered by another metal layer to provide the trilayer configuration (e.g., JJ on the capacitor).

Reference now is made to <FIG>, which illustrates the formation of a superconducting alloy <NUM> having a different orientation based on the anneal temperature, consistent with an illustrative embodiment. For discussion purposes, and not by way of limitation, the original semiconductor structure 400A has a first metal layer <NUM> comprising niobium (Nb) and a second metal layer <NUM> comprising aluminum (Al) that are placed on top of a substrate <NUM>. X-Ray diffraction intensity charts 400C and 400D (with reference to structure 400B) indicate that at around a temperature of 500C, a superconducting alloy <NUM> is formed at an interface between the niobium layer <NUM> and the aluminum layer <NUM>. The superconducting alloy <NUM> (i.e., Al<NUM>Nb) has a lattice structure that may be oriented differently with the substrate based on different anneal temperatures. The desired orientation for optimal contact can be controlled by the annealing condition.

Different temperatures will form different alloy thicknesses. For example a thin layer of Al<NUM>Nb(<NUM>) forms below 400C with long anneal time, and will grow over time. When the temperature is increased (e.g., 650C) the superconducting alloy <NUM> starts to include grains exhibiting different orientations (Al<NUM>Nb(<NUM>) and (<NUM>)) as the grains in the film become more randomly oriented. In some embodiments, similar results can be achieved with different combinations of temperature and time. For example, a lower temperature but longer anneal time, sometimes referred to herein as isothermal anneal, can also be used to achieve the superconducting alloy Al<NUM>Nb(<NUM>). Applicants have determined that an anneal temperature from 350C to 500C for an Nb/Al interface creates a superconducting alloy Al<NUM>Nb having an <NUM> alignment with respect to the underlying Nb <NUM> planes.

It is noted that Nb <NUM> and Al <NUM> form a superconducting alloy <NUM> at greater than 350C when in direct contact. Alloying Nb <NUM> and Al <NUM> will form an electrical path from Nb to Al through a Nb and Al alloy <NUM>. In one embodiment, no oxygen is present at the Nb <NUM> and Nb-Al alloy <NUM> interface, and only some oxygen is present on the surface of the Al layer <NUM>. Accordingly, there is no residual Nb oxide to cause decoherence, thereby substantially increasing superconductor device performance.

The foregoing discussion is generally related to avoiding an oxygen layer between the first metal layer (e.g., Nb) and the second metal layer (e.g., Al). It should be noted that when native niobium oxide is present between the two metal layers, a superconducting alloy can still form under certain conditions, but not as rapidly. In this regard, reference is made to <FIG> that provide different processing steps of creating a superconductor structure that includes an initial oxide layer between first and second metal layers <NUM> and <NUM>, consistent with an illustrative embodiment. As illustrated in <FIG>, there is a first metal layer <NUM> (e.g., Nb) on top of a substrate <NUM>. There is a second metal layer (e.g., Al) <NUM> on top of the first metal layer <NUM>. There is a native oxide layer (e.g., niobium oxide) <NUM> between the metal layers <NUM> and <NUM>.

<FIG> illustrates that during alloy formation (e.g., by anneal), the native oxide <NUM> moves away from the niobium surface to the superconducting alloy <NUM> surface, represented by oxide layer <NUM>.

<FIG> illustrates that a selective etch and can remove the second metal layer <NUM> and the oxide layer <NUM>. In various embodiments, both the second metal layer <NUM> and the oxide layer <NUM> can be removed concurrently or separately by different etch steps. An electrode (e.g., Josephson) <NUM> can then be deposited on top of the superconducting alloy <NUM>. For example, the selective etch and aluminum JJ fabrication result in an electrical path from Nb to Al through Nb and Al alloy without niobium oxide defects.

Accordingly, Applicants have determined that while a superconducting alloy between the metal layers having no oxide (e.g., niobium oxide) layer between the metal layers can be achieved without an aggressive prevention and/or removal of the oxide layer between the first and second metal layers <NUM> and <NUM>, such processing takes a substantial amount of more fabrication time and/or temperature to create the protective alloy <NUM>. While the discussion herein may refer to the idealized term "having no oxide," it will be understood that it includes the meaning that it is substantially free of oxygen such that it would be very difficult to detect with known tools.

The descriptions of the various embodiments of the present teachings have been presented for purposes of illustration, but are not intended to be exhaustive or limited to the embodiments disclosed. The terminology used herein was chosen to best explain the principles of the embodiments, the practical application or technical improvement over technologies found in the marketplace, or to enable others of ordinary skill in the art to understand the embodiments disclosed herein.

While the foregoing has described what are considered to be the best state and/or other examples, it is understood that various modifications may be made therein and that the subject matter disclosed herein may be implemented in various forms and examples, and that the teachings may be applied in numerous applications, only some of which have been described herein. The scope of the present invention is defined, however, by the following claims.

The components, steps, features, objects, benefits and advantages that have been discussed herein are merely illustrative. None of them, nor the discussions relating to them, are intended to limit the scope of protection. While various advantages have been discussed herein, it will be understood that not all embodiments necessarily include all advantages.

Numerous other embodiments are also contemplated. These include embodiments that have fewer, additional, and/or different components, steps, features, objects, benefits and advantages. These also include embodiments in which the components and/or steps are arranged and/or ordered differently.

While the foregoing has been described in conjunction with exemplary embodiments, it is understood that the term "exemplary" is merely meant as an example, rather than the best or optimal.

It will be understood that the terms and expressions used herein have the ordinary meaning as is accorded to such terms and expressions with respect to their corresponding respective areas of inquiry and study except where specific meanings have otherwise been set forth herein. Relational terms such as first and second and the like may be used solely to distinguish one entity or action from another without necessarily requiring or implying any actual such relationship or order between such entities or actions. The terms "comprises," "comprising," or any other variation thereof, are intended to cover a non-exclusive inclusion, such that a process, method, article, or apparatus that comprises a list of elements does not include only those elements but may include other elements not expressly listed or inherent to such process, method, article, or apparatus. An element proceeded by "a" or "an" does not, without further constraints, preclude the existence of additional identical elements in the process, method, article, or apparatus that comprises the element.

Claim 1:
A superconductor device, comprising:
a substrate (<NUM>, <NUM>, <NUM>, <NUM>);
a first metal layer (<NUM>, <NUM>, <NUM>, <NUM>) on top of the substrate (<NUM>, <NUM>, <NUM>, <NUM>);
a second metal layer (<NUM>, <NUM>, <NUM>, <NUM>) on top of the first metal layer (<NUM>, <NUM>, <NUM>, <NUM>);
a superconducting alloy (<NUM>, <NUM>, <NUM>, <NUM>) of the first metal layer (<NUM>, <NUM>, <NUM>, <NUM>) and the second metal layer (<NUM>, <NUM>, <NUM>, <NUM>) between the first metal layer (<NUM>, <NUM>, <NUM>, <NUM>) and the second metal layer (<NUM>, <NUM>, <NUM>, <NUM>),
wherein there is no oxide layer between the superconducting alloy (<NUM>, <NUM>, <NUM>, <NUM>) and the first metal layer (<NUM>, <NUM>, <NUM>, <NUM>),
wherein:
the first metal layer (<NUM>, <NUM>, <NUM>, <NUM>) is Niobium, Nb;
the second metal layer (<NUM>, <NUM>, <NUM>, <NUM>) is Aluminum, Al; and
the superconducting alloy (<NUM>, <NUM>, <NUM>, <NUM>) is Al<NUM>Nb.