This application claims the benefit of U.S. Provisional Application No. 62/052,328, filed Sep. 18, 2014, the entire contents of which are incorporated herein by reference.
Embodiments described herein relate generally to a magnetic memory and a method of manufacturing the same.
In recent years, various kinds of devices comprising magnetic elements have been developed. A magnetic memory, which is one of these, for example a spin-transfer-torque (STT)-magnetic random access memory (MRAM), stores data in a magnetic element.
In these devices, the patterning of a magnetic element is performed by physical etching such as ion beam etching (IBE) with a metal layer as a hard mask used as a mask. However, the physical etching has a problem that it is hard to sufficiently increase an etching selection ratio between the magnetic element and the hard mask.
In general, according to one embodiment, a magnetic memory comprises: a magnetic element; and a metal layer stacked on the magnetic element, wherein H/D>1.47 is satisfied, where H denotes a sum of thicknesses of the magnetic element and the metal layer in a first direction in which the magnetic element and the metal layer are stacked, and D denotes a width of the magnetic element in a second direction perpendicular to the first direction.
In the embodiment, first, a magnetic layer 12 is formed on a substrate 11, and a metal layer 13 is formed on the magnetic layer 12. In addition, the metal layer 13 is patterned by a photo-engraving process (PEP) and reactive ion etching (RIE). The metal layer 13 may be patterned by ion beam etching (IBE) instead of by RIE.
Then, with the metal layer 13 used as a mask, the magnetic layer 12 is patterned by IBE. This IBE is executed by using an ion beam accelerated by an acceleration voltage higher than 200 V. The ion beam includes one of Ne, Ar, Kr, Xe, N2 and O2.
According to the embodiment, the acceleration voltage of the ion beam is set at a value higher than 200 V. In this case, the etching rate of the magnetic layer 12 increases more with respect to the etching rate of the metal layer 13 than in the case where the acceleration voltage of the ion beam is 200 V. That is, an etching selection ratio between the magnetic layer 12 and the metal layer 13 can be improved.
This is caused for the following reasons:
The irradiation of an ion beam exhibits an etching effect or an ion implantation effect on an object to which the ion beam is irradiated. In the case of the embodiment, as the acceleration voltage of an ion beam becomes larger, the etching effect becomes larger in the magnetic layer 12, while the ion implantation effect becomes larger in the metal layer 13. Thus, it is conceivable that such an advantage of an improvement in an etching selection ratio as described above can be obtained.
It should be noted that the above-described advantage can be obtained from a magnetic material including Co, Fe, Tb, etc., with respect to the magnetic layer 12, and from a metal material including W, Ta, Ru, Ti, TaN, TiN, etc., with respect to the metal layer 13. In addition, the magnetic layer 12 may have a single-layer structure or may have a multilayer structure.
Moreover, if the magnetic layer 12 is thick, for example, if the magnetic layer 12 has a multilayer structure, it is preferable to pattern the magnetic layer 12 by first etching and second etching after the first etching in order to prevent a bad influence of an etched material generated incidentally by IBE.
The first etching is executed at a beam angle selected to be in the range of, for example, 30° to 89°, and more preferably in the range of 30° to 60°, and the second etching is executed at a beam angle selected to be in the range of, for example, 0° to 30°. However, the beam angles are angles between a direction in which the magnetic layer 12 and the metal layer 13 are stacked and a direction in which an ion beam is irradiated.
Also in this case, the first and second etchings are executed by using an ion beam accelerated by an acceleration voltage higher than 200 V.
The comparative example (
In the comparative example, first, the magnetic layer 12 is formed on the substrate 11, and the metal layer 13 is formed on the magnetic layer 12. In addition, the metal layer 13 is patterned by PEP and RIE. The metal layer 13 may be patterned by IBE instead of by RIE.
Then, with the metal layer 13 used as a mask, the magnetic layer 12 is patterned by IBE. This IBE is executed by using an ion beam accelerated by an acceleration voltage of 200 V or a value lower than 200 V. The ion beam includes one of Ne, Ar, Kr, Xe, N2 and O2.
In the case of the comparative example, as shown in
For the above reason, it is preferable to make the metal layer 13 as thick as possible. According to the embodiment, because the etching selection ratio between the magnetic layer 12 and the metal layer 13 can be improved, the metal layer 13, which is sufficiently thick, can be secured even after a magnetic element is patterned.
A magnetic memory as an application example will be described.
In the example, the memory cell of the magnetic memory comprises a selection transistor (for example, an FET) ST and a magnetoresistive effect element MTJ.
The selection transistor ST is disposed in an active area AA in a semiconductor substrate 21. The active area AA is surrounded by an element isolation insulating layer 22 in the semiconductor substrate 21. In the example, the element isolation insulating layer 22 has a shallow trench isolation (STI) structure.
The selection transistor ST comprises source/drain diffusion layers 23a and 23b in the semiconductor substrate 21, and a gate insulating layer 24 and a gate electrode (word line) 25 formed therebetween in the semiconductor substrate 21. The selection transistor ST of the example has a so-called embedded gate structure in which the gate electrode 25 is embedded in the semiconductor substrate 21.
An interlayer insulating layer (for example, a silicon oxide layer) 26 covers the selection transistor ST. Contact plugs BEC and SC are disposed in the interlayer insulating layer 26. The contact plug BEC is connected to the source/drain diffusion layer 23a, and the contact plug SC is connected to the source/drain diffusion layer 23b. The contact plugs BEC and SC include, for example, one of W, Ta, Ru and Ti.
The magnetoresistive effect element MTJ is disposed on the contact plug BEC. In addition, a contact plug TEC is disposed on the magnetoresistive effect element MTJ.
A bit line BL1 is connected to the magnetoresistive effect element MTJ through the contact plug TEC. A bit line BL2 is connected to the source/drain diffusion layer 23b through the contact plug SC. The bit line BL2 also functions as, for example, a source line SL to which ground potential is applied at the time of reading.
In the figure, the same elements as those shown in
The magnetoresistive effect element MTJ comprises a first ferromagnetic layer 31 on the contact plug BEC, a nonmagnetic insulating layer (tunnel barrier layer) 32 on the first ferromagnetic layer 31, a second ferromagnetic layer 33 on the nonmagnetic insulating layer 32, and the hard mask layer 13 on the second ferromagnetic layer 33.
The hard mask layer 13 functions as, for example, a mask layer at the time of processing the magnetoresistive effect element MTJ. The hard mask layer 13 includes, for example, W, Ta, Ru, Ti, TaN or TiN. It is preferable that the hard mask layer 13 comprise a material which has a low electrical resistance and good diffusion, etching and milling tolerances, for example, a lamination of Ta/Ru.
One of the first and second ferromagnetic layers 31 and 33 is a reference layer having invariable magnetization, and the other is a storage layer having variable magnetization.
Here, the invariable magnetization means that a magnetization direction does not vary before or after writing, and the variable magnetization means that the magnetization direction can vary in reverse before or after writing.
Further, the writing means spin transfer writing in which a spin implantation current (spin-polarized electron) is passed to the magnetoresistive element MTJ, thereby imparting a spin torque to the magnetization of a storage layer.
If the first ferromagnetic layer 31 is a storage layer and the second ferromagnetic layer 33 is a reference layer, the magnetoresistive effect element MTJ is referred to as a top-pin type. In addition, if the first ferromagnetic layer 31 is a reference layer and the second ferromagnetic layer 33 is a storage layer, the magnetoresistive effect element MTJ is referred to as a bottom-pin type.
It is preferable that each of the first and second ferromagnetic layers 31 and 33 have vertical magnetization, that is, residual magnetization in a vertical direction in which the first and second ferromagnetic layers 31 and 33 are stacked. However, each of the first and second ferromagnetic layers 31 and 33 may have in-plane magnetization, that is, residual magnetization in an in-plane direction perpendicular to a direction in which the first and second ferromagnetic layers 31 and 33 are stacked.
The resistance of the magnetoresistive effect element MTJ varies depending on the relative magnetization directions of a storage layer and a reference layer because of a magnetoresistive effect. For example, the resistance of the magnetoresistive effect element MTJ is low at the time of a parallel state in which the magnetization directions of the storage layer and the reference layer are the same, and is high at the time of an antiparallel state in which the magnetization directions of the storage layer and the reference layer are opposite to each other.
The first and second ferromagnetic layers 31 and 33 comprise, for example, CoFeB, MgFeO or a lamination of these. In the case of a magnetoresistive effect element having vertical magnetization, it is preferable that the first and second ferromagnetic layers 31 and 33 comprise TbCoFe having vertical magnetic anisotropy, an artificial lattice in which Co and Pt are stacked together, Llo-ordered FePt, etc. In this case, CoFeB as an interface layer may be provided between the first ferromagnetic layer 31 and the nonmagnetic insulating layer 32, or between the nonmagnetic insulating layer 32 and the second ferromagnetic layer 33.
The nonmagnetic insulating layer 32 comprises, for example, MgO or AlO. The nonmagnetic insulating layer 32 may be nitride of Al, Si, Be, Mg, Ca, Sr, Ba, Sc, Y, La, Zr, Hf, etc.
The first and second ferromagnetic layers 31 and 33 may each comprise a shift cancelling layer. The shift cancelling layer has a magnetization direction opposite to the magnetization direction of a reference layer. The shift cancelling layer thereby cancels a shift of a magnetization reversal characteristic (hysteresis curve) of a storage layer which occurs due to a stray magnetic field from the reference layer. It is preferable that the shift cancelling layer have, for example, a structure [Co/Pt]n in which n Co layers and Pt layers are stacked.
The above-described magnetoresistive effect element MTJ is pattered by IBE, for example, with the metal layer 13 used as a mask. This IBE is executed with the acceleration voltage of 200 V in the comparative example, and with the acceleration voltage higher than 200 V in the embodiment. An ion beam includes one of Ne, Ar, Kr, Xe, N2 and O2.
In this case, the magnetoresistive effect element MTJ formed by IBE of the comparative example has, for example, an aspect ratio H/D of 1.47. On the other hand, the magnetoresistive effect element MTJ formed by IBE of the embodiment has, for example, an aspect ration H/D higher than 1.47. This is mainly because a thickness t1 of the metal layer 13 after IBE is small in the comparative example, while a thickness t2 of the metal layer 13 after IBE is sufficiently large in the embodiment.
However, as shown in
It should be noted that the width of the nonmagnetic insulating layer 32 has been defined as D because the width of the nonmagnetic insulating layer 32 has an influence on the MR ratio of the magnetoresistive effect element 12 (MTJ).
Moreover, according to the embodiment, it is proved that as an acceleration voltage VIBE becomes larger, an aspect ratio H/D becomes larger as shown in
More specifically, the figure shows the aspect ratio H/D with the acceleration voltage VIBE higher than 200 V in the case where the aspect ratio H/D with the acceleration voltage VIBE of 200 V is 1.0.
As is clear from the figure, the aspect ratio H/D with the acceleration voltage VIBE higher than 200 V is always higher than 1.0. That is, by making the acceleration voltage VIBE of IBE higher than 200 V as in the embodiment, an aspect ratio H/D higher than in the conventional art (where the acceleration voltage VIBE is 200 V) can be achieved.
In addition, as shown in
Also in this case, the first and second etchings are executed by using an ion beam accelerated by an acceleration voltage higher than 200 V.
However, the beam angle θhigh/θlow is an angle between a direction NL in which the first and second ferromagnetic layers 31 and 33 in the magnetoresistive effect element MTJ are stacked (or a direction perpendicular to a top surface of the substrate 21) and a direction in which the ion beam is irradiated.
The first etching is executed under such a condition as prevents an etched material from being reattached to a sidewall of the magnetoresistive effect element MTJ. However, in the first etching, because of a so-called shadow effect, it is hard to carry out etching at a bottom portion of the magnetoresistive effect element MTJ, and the magnetoresistive effect element MTJ assumes a shape with its foot trailed. Thus, the bottom portion of the magnetoresistive effect element MTJ is etched by the second etching.
A changing point between the first etching and the second etching may be in the second ferromagnetic layer 33 (point A), or may be in the vicinity of the nonmagnetic insulating layer 32 (point B), and moreover, may be in the first ferromagnetic layer 31 (point C).
3. Method of Manufacturing Magnetic Memory
A method of manufacturing a magnetic memory comprising the magnetoresistive effect element of
First, as shown in
Then, a first etching process is executed.
The first etching process is executed by, for example, ion beam etching (IBE) using an ion beam at a high angle θhigh. In this example, the first etching process is stopped in a middle of the second ferromagnetic layer 33.
Next, as shown in
The second etching process is executed by, for example, IBE using an ion beam at a low angle θlow. The second etching process is executed until the interlayer insulating layer 26 to be the ground of the magnetoresistive effect element 12 (MTJ) is exposed.
This is because the magnetic memory comprises an array of magnetoresistive effect elements MTJ. That is, the magnetoresistive effect elements MTJ in the magnetic memory can be electrically separated from each other by etching the first ferromagnetic layer 31 to the end.
Then, a protective layer, an interlayer insulating layer, etc., are formed by a well-known method.
By the above-described manufacturing method, the magnetic memory comprising the magnetoresistive effect element MTJ of
A direction perpendicular to a top surface of the stage 3a (or a top surface of the wafer 2) can be inclined at e in a direction in which an ion beam is irradiated. That is, an angle θ between the direction perpendicular to the top surface of the stage 3a and the direction in which an ion beam is irradiated can be changed. This angle θ corresponds to a beam angle, and can be changed within a predetermined range of angles.
The example shows examples of the stage (solid line) 3a with a beam angle θ of 0° and the stage (broken line) 3a with a beam angle θ of 45°.
Moreover, the support portion 3b comprises an axis of rotation AS having its center at a point O. The axis of rotation AS is parallel to a direction in which an ion beam is irradiated, if the angle θ is 0°. The support portion 3b rotates, for example, with the stage 3a inclined at the angle θ. The stage 3a and the support portion 3b perform the function of causing the wafer 2 to rotate while an ion beam is irradiated. This rotation enables the wafer in-plane uniformity (σ) of an etching rate of the wafer 2 to be improved.
A plasma generating portion 4 is disposed in the etching chamber 1. The plasma generating portion 4 faces the stage 3a and generates ions from which an ion beam is generated. The plasma generating portion 4 is separated from the stage 3a by a grid 5.
The grid 5 comprises first, second and third electrodes 5a, 5b and 5c as shown in
A plasma power supply window 8 is, for example, an element for generating plasma by transmitting an electromagnetic wave (energy) from an antenna 9 to the plasma generating portion 4. The antenna 9 has a ring shape and surrounds the etching chamber 1.
A first drive portion 6a is a drive portion for adjusting the beam angle θ by rotating the stage 3a on the point O and changing the direction of the stage 3a. Also, a second drive portion 6b is a drive portion for rotating the stage 3a on the axis of rotation AS.
A potential generating portion 7 determines an acceleration voltage of ions used for IBE. For example, the potential generating portion 7 applies predetermined potentials to the first, second and third electrodes 5a, 5b and 5c of
Further, a control portion 10 controls the first drive portion 6a, the second drive portion 6b and the potential generating portion 7.
As described above, according to the embodiment, an aspect ratio of a magnetic element can be increased by etching the magnetic element by IBE with the acceleration voltage of ions higher than 200 V. As a result, because the magnetic element can be prevented from being damaged at the time of etching for forming a contact hole for the magnetic element, the characteristics of the magnetic element can be improved.
While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the inventions. Indeed, the novel embodiments described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the embodiments described herein may be made without departing from the spirit of the inventions. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the inventions.
Number | Date | Country | |
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62052328 | Sep 2014 | US |