US9136457B2 - Double-masking technique for increasing fabrication yield in superconducting electronics - Google Patents
Double-masking technique for increasing fabrication yield in superconducting electronics Download PDFInfo
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- US9136457B2 US9136457B2 US13/771,330 US201313771330A US9136457B2 US 9136457 B2 US9136457 B2 US 9136457B2 US 201313771330 A US201313771330 A US 201313771330A US 9136457 B2 US9136457 B2 US 9136457B2
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- 238000004519 manufacturing process Methods 0.000 title abstract description 21
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims abstract description 66
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- 239000002887 superconductor Substances 0.000 claims abstract description 39
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- 230000007547 defect Effects 0.000 claims abstract description 10
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N69/00—Integrated devices, or assemblies of multiple devices, comprising at least one superconducting element covered by group H10N60/00
-
- H01L39/025—
-
- H01L39/2493—
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/01—Manufacture or treatment
- H10N60/0156—Manufacture or treatment of devices comprising Nb or an alloy of Nb with one or more of the elements of group IVB, e.g. titanium, zirconium or hafnium
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/01—Manufacture or treatment
- H10N60/0884—Treatment of superconductor layers by irradiation, e.g. ion-beam, electron-beam, laser beam or X-rays
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/01—Manufacture or treatment
- H10N60/0912—Manufacture or treatment of Josephson-effect devices
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/10—Junction-based devices
- H10N60/12—Josephson-effect devices
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/80—Constructional details
- H10N60/805—Constructional details for Josephson-effect devices
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/80—Constructional details
- H10N60/85—Superconducting active materials
Definitions
- the invention is directed to fabrication of electronic devices and more particularly to the fabrication of superconducting electronic devices such as Josephson junctions.
- Superconducting integrated circuits (ICs) based on Josephson junctions offer the possibility of operation at clock frequencies of 100 GHz or above. In order to achieve this on an industrial scale, it is necessary to decrease junction size toward submicron dimensions, and increase junction density, so that chips with many thousands of Josephson junctions can be reliably manufactured.
- the key parameter is the critical current I c of a junction, which must be defined to within about 1% of design specifications, without defects.
- junction fabrication technology is based on the superconductor niobium (Nb), and in particular on a trilayer structure based on an ultrathin insulating “tunnel barrier” layer of aluminum oxide (AlO x ), 1-2 nm thick, sandwiched between two layers of Nb.
- Nb superconductor niobium
- AlO x aluminum oxide
- Applications of standard microlithography techniques may produce junctions with edge damage that can reduce junction quality and yield.
- Nb IC technology also incorporates multiple layers of superconducting Nb wiring to bias and connect the Josephson junctions. This requires high-quality insulating layers between Nb layers, which are typically provided by silicon dioxide (SiO 2 ). SiO 2 is of course a standard material in semiconductor technology, and standard procedures for fabricating high-quality films are available.
- An established technique in the prior art to improve junction yield is the use of selective anodization (Meng 2003, Kerber 2006).
- Anodization is an electrolytic process of surface oxidation that passivates all exposed Nb and Al surfaces, preventing damage in subsequent lithographic steps.
- This has not completely eliminated defects and related yield problems. It is essential to solve these problems to advance to the next stage of circuit integration.
- the techniques of the prior art have resulted in a number of problems. Specifically, the techniques of the prior art have resulted in low yield, that is, a large number of junctions fabricated on a silicon based wafer fail for a variety of reasons. This results in a substantial percentage of defective junctions on each wafer.
- SiO 2 adheres well to Nb (since it has also been optimized for an insulation layer), and also adheres very well to the top resist layer. Furthermore, SiO 2 is inert with respect to both aqueous and organic solvents used in anodization processing and resist processing (for both positive and negative resists), but can also be removed where necessary by standard etching techniques.
- the invention recognizes that failure of interlayer adhesion between photoresist and Nb is a major cause of defects in the fabrication technology of the prior art. By substantially improving such adhesion, the present invention offers the possibility of improved reliability and IC yield.
- the present invention does increase the number of steps in the full process, since the SiO 2 layer in the mask must first be deposited, and subsequently etched away. (However, this etch-away step can be done simultaneously with the counter-electrode etching.) Nevertheless, this extra effort is easily worthwhile, since it enables the manufacturing (with reasonable yield) of higher-density superconducting ICs with greatly enhanced device speed and performance.
- a second process improvement of the present invention replaces a wet-etch process for AlO x removal in the prior art with an optimized dry-etch (or argon ion mill) process, in order to enhance junction uniformity and yield for small junctions.
- FIG. 1 shows a cross section of a wafer having Nb/Al/AlO x /Nb layers as used in the fabrication of superconducting devices such as a Josephson junction.
- FIG. 2 shows a modification of the prior art process whereby dielectric layer of SiO 2 is deposited to act as an adhesion layer between the Nb and the photoresist layer deposited during the next process step.
- FIG. 3 shows application of a photoresist layer on top of the silicon dioxide layer in accordance with one aspect of the invention.
- FIG. 4 shows the photoresist area that defines the junction area after exposure and development of the photoresist.
- FIG. 5 shows the etching of the SiO 2 adhesion layer and Nb counter-electrode down to the AlO x /Al barrier layer.
- FIG. 6A shows the results of a selective anodization step whereby all the exposed Al and part of the underlying Nb are converted to insulating oxides.
- FIG. 6B shows a magnified view of the region inside the small dashed box in FIG. 6A .
- FIG. 7 shows the removal of the photoresist layer.
- FIG. 8 shows the result of coating and patterning of another photoresist layer designed to produce a protective anodization ring around the junction area.
- FIG. 9 shows the etching (by Ar ion milling or dry reactive ion etching) of the anodized oxide (both AlO x and NbO x layers) except in the anodization ring (under the photoresist mask)
- FIG. 10 shows the removal of the photoresist defining the anodization ring.
- FIG. 11 shows the deposition of an SiO 2 insulating layer, designed to isolate the junction from subsequent wiring layers.
- FIG. 12 shows the coating and patterning of a third photoresist layer, designed to produce a contact via to the Nb junction from a Nb wiring layer.
- FIG. 13 shows the selective etching of the SiO 2 up to the Nb counter-electrode.
- FIG. 14 shows the removal of the photoresist. Now the structure is ready for deposition of a Nb wiring layer
- a new fabrication method is proposed for increasing the yield and quality of superconducting junctions and more particularly Josephson junctions and Josephson-based digital and analog circuits in superconducting electronics.
- the method is based on using a double-layer mask for partial anodization of the junction side-walls and base-electrode around the junction.
- the top layer of this mask is a photoresist or electron-beam resist, and the bottom layer is a dielectric (e.g., SiO 2 ) that is insoluble in either aqueous or organic solvents.
- the existing fabrication scheme for making Nb-based Josephson tunnel junctions for superconducting electronics is comprised of the following fabrication steps:
- a Nb/Al/AlO x /Nb trilayer is deposited in-situ on a wafer that includes or will include several other patterned layers of metal and dielectric.
- a tunnel barrier is formed by in-situ thermal oxidation of the Al layer in oxygen or an oxygen/argon mixture at a defined pressure, to form a thin ( ⁇ 1-2 nm) layer of AlO x . Both the oxidation time and the pressure determine the properties of the tunnel barrier such as the Josephson critical current density J c .
- the bottom Nb layer is called the base electrode, and the top Nb layer is called the counter-electrode of the tunnel Josephson junctions.
- FIG. 2 shows a step that differs from prior art fabrication techniques and will be discussed in more detail hereinafter.
- the wafer is coated with either positive or negative resist ( FIG. 3 ), and the resist etch mask is formed by optical or e-beam lithography ( FIG. 4 ).
- the counter-electrode area is then defined by etching ( FIG. 5 ), using e.g. plasma etching, reactive-ion etching, or high-density plasma etching.
- the AlO x /Al layer acts as an etch stop. (Note—the prior art method does not include the thin SiO 2 layer shown in FIGS. 3 , 4 and 5 .)
- the wafer is immersed in an anodization solution, and all the surfaces that are not protected by the resist mask formed in step 5 are anodized. That is, the same resist etch mask is also used as an anodization mask.
- Anodization creates a bilayer of anodized Al (AlO x ) and anodized Nb (NbO x ) on the surface of the base electrode ( FIG. 6 ). A layer of anodized Nb is also formed on all sidewalls of the junction's counter-electrode.
- This anodization step is very important because it encapsulates the junction's tunnel barrier with an anodized NbO x layer, and this, protects it from reacting with water, oxygen, and other processing chemicals during all further wafer processing steps. This step also allows for opening a contact hole to the counter-electrode that is larger in size than the junction itself.
- the thickness of the anodized layer is controlled by the anodization voltage, usually in the range of 15-50 V.
- the initial anodization current density is in the range from 0.5-5 mA/cm 2 .
- the resist is stripped ( FIG. 7 ), and the wafer proceeds to the next fabrication steps that are intended to pattern the base electrode of the junction by lithography and etching. This may also require removing the anodization layer in some parts of the circuit. It remains around the junction (the anodization ring of FIGS. 8-10 ).
- the Josephson junction is completely formed. All other fabrication steps are necessary in order to interconnect junctions in the circuits (such as the SiO 2 insulating layer in FIGS. 11-14 ), and to create resistors for biasing and shunting the junctions. These steps may vary depending on the details the fabrication process.
- One improvement of the invention is to use a double-layer anodization mask with the lower layer being an inorganic dielectric layer (such as SiO 2 ) that is insoluble in water, solvents, and components of the anodization solution, and the upper layer is the photoresist (or e-beam resist) layer.
- SiO 2 is especially suitable since it has already been optimized as an insulating layer in the prior-art Nb integrated circuit process, and is also fully compatible with standard Si-based resist processing.
- This double-layer mask is formed in the following simple way:
- a pinhole-free layer of SiO 2 is deposited by any appropriate method (e.g., rf magnetron sputtering, or plasma-enhanced chemical vapor deposition—PECVD) on top of the trilayer (see FIG. 2 ).
- the layer thickness may be anywhere from 5 to 300 nm, and is not critical, as long as it is free from pinholes. Thicker layers require long etch times, making them impractical.
- a resist mask is formed in the same way as in step 4 above.
- etching is done, using reactive ion etching (ME) or inductively coupled plasma (ICP) with fluorine-based chemistry (e.g., SF 6 , NF 3 , or CF 4 +O 2 ) such that both the SiO 2 overlayer and the Nb counter-electrode are etched in the same process.
- fluorine-based chemistry e.g., SF 6 , NF 3 , or CF 4 +O 2
- This may be a one-step process when the same etch parameters are used for both layers, or a two-step process when different etch recipes are used for etching first the SiO 2 and then the Nb counter-electrode.
- the top of the Josephson junction will have a double-layer structure (SiO 2 +resist) that serves as the double-layer anodization mask.
- the advantages of the proposed method are as follows.
- the SiO 2 layer improves the adhesion of the resist, and does not allow the anodization solution to leach underneath. Since the adhesion of sputtered or PECVD-deposited SiO 2 to Nb has already been optimized, and is stronger than the adhesion of the resist to Nb, the double-layer also protects the junction counter-electrode from being anodized even in the unlikely event that a part of the resist mask pops off, or if the anodization solution does leach under the resist. In the rare case that the SiO 2 layer has a pinhole or other defect, the presence of the resist on top still provides protection during the anodization. The probability that both layers of the double-layer anodization mask fail in the same location is much smaller than the probability of a failure of a single-layer resist mask. As a result, a dramatic increase in the yield and junction quality is achieved.
- approach A ion-milling with a neutral beam of argon (Ar) atoms is used to remove both the AlO x and the NbO x layers.
- Approach B plasma etching (ME or ICP) is used in a two-step process. First, a chlorine-based plasma is used to remove AlO x , and then a fluorine-based plasma is used to remove the NbO x . Either approach provides for increased yield and uniformity.
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US15/456,010 US10109673B2 (en) | 2006-09-20 | 2017-03-10 | Double-masking technique for increasing fabrication yield in superconducting electronics |
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Also Published As
Publication number | Publication date |
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US20090315021A1 (en) | 2009-12-24 |
US20140054552A1 (en) | 2014-02-27 |
US20170179193A1 (en) | 2017-06-22 |
US20150380632A1 (en) | 2015-12-31 |
US10109673B2 (en) | 2018-10-23 |
US9595656B2 (en) | 2017-03-14 |
US20080070325A1 (en) | 2008-03-20 |
US7615385B2 (en) | 2009-11-10 |
US8383426B1 (en) | 2013-02-26 |
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