Monatomic PCMs: A New Direction

Ron Neale[The following is a guest post written by Ron Neale.]

Until now designers of PCM devices have tried to make PCM meet their expectations by experimenting with an almost infinite number of possible multi-element glass compositions, in order to tinker with or emphasise a particular composition-related device characteristic. The apparent advantage of this great variety of materials comes with the baggage of reliability and performance-compromising element separation, driven by the forces of electro-migration, electrostatic effects and phase separation.

Is it possible to cast aside the problems of the multi-element PCM compositions and look at the possibility of monatomic PCMs?  For a team at IBM, Zurich and Aachen University the answer is an unequivocal “Yes!” and recently they have published details of the remarkable progress they have made with amorphous antimony (Sb), as an initial candidate element. This research was published in a June 2018 paper in Nature Materials Letters titled: Monatomic phase change memory, by Martin Salinga et al, IBM and Aachen University).

A difficulty faces those venturing in this new direction: While it is possible to bring many elements to the amorphous state, they very quickly crystallize at room temperature and higher.  The IBM researchers used simulations to find that the keys to obtaining a stable amorphous state is to control the quenching rate and the volume of the sample. That part of the antimony research is underpinned by some very impressive simulations that use only about 200 atoms.

Here’s the issue that this approach addresses: Quenching is an essential part of PCM operation, since quenching is necessary to “freeze-in” the amorphous state.  So far most memory array designers have achieved quenching by bringing only a small volume of molten material to a high temperature and then cooling it by using any naturally-occurring low thermal resistance path to the local heat sink.

Past efforts at thermal design have focussed more on trying to avoid thermal cross-talk which itself has the tendency to come in conflict with achieving high quench rates. While lithographic scaling produces an effective heat sink it also reduces the size of the molten volume and a smaller molten volume requires a very high RESET current to reach the melting temperature.  The high RESET current exacerbates the problems of element separation for multi-element PCM compositions.

IBM’s researchers chose to design a pure antimony cell with a lateral structure that allowed them to control the volume of the antimony while also giving them control of the thickness of an underlying SiO2 thermal barrier to manage the quench rate.

The diagram above shows a side view cross section of the memory cell and the lateral structure used for the new quenching-controlled nanoscale confinement structure.  The column at the right is an enlargement of the small zone outlined in red in the cell cross-section on the left.  Starting from the bottom, the structure consists of the silicon substrate, an SiO2 heat barrier, the antimony bit layer, ZnS-SiO2 and HSQ layers (both explained below), and an SiO2 capping layer.  The red arrows indicate the experiment’s two key variables: The thickness of the antimony and the thickness of the SiO2 thermal barrier between the antimony and the silicon substrate heat sink.

The ZnS-SiO2 layer in this drawing acts as a barrier to protect the antimony during subsequent processing; in the past this same material has been used to protect the surface of PCM-based CD-RWs, so the material is well understood. The HSQ (Hydrogen Silsesquioxane) layer above that is a material that is often used in the semiconductor industry thanks to the combination its many useful photo-lithographic, dielectric, and thermal properties.

The next figure is based on this same cross-section side view as the figure above.

The large green area in this figure is a top view of the same structure’s antimony layer – the thin green layer in the side view.  Although the cell is 600nm long in this direction, the melting zone is only 50nm.

So far it has been possible to create stable amorphous antimony by managing three variables:

  • The duration of the trailing edge of the programming pulse
  • Programming power
  • Ambient temperature

The first two of these are represented in the figure below.  The programming power is indicated by the height of the pulse, and the duration of the trailing edge (red) corresponds to the slope of that line.

The figure below is my linearised version of the data from the Salinga paper cited above.  It illustrates how these three variables combine to create amorphous antimony in a cell that pairs a 40nm heat barrier with a 5nm antimony thickness.  As long as the ambient temperature and the parameters of the programming pulse remain within the purple area an amorphous state can be achieved.  The extrapolation (dashed line) indicates that there should be no sudden drop that would prevent this approach from creating an amorphous state as temperatures rise above room temperature: 295°K.

It must be stressed that this chart is for just one thermal barrier thickness (40nm) from an experimental thickness range of from 40nm to 200nm and for one antimony sample size of 5nm. It was reported that, with thermal barriers greater than 200nm, it becomes extremely difficult to produce amorphous antimony.

There are three ways to control the size of the heated volume, two are direct by either varying the thickness of the antimony film or by varying the thickness of the thermal barrier, the third is indirect by using the programming power to control the size of the melt region.  As the power is increased the width of the amorphous region expands.  This is illustrated in the figure below.

The amorphous space will have the same form and merely expand as the thermal barrier thickness is reduced or contract as the thermal barrier thickness is increased (Think Russian matrioshki dolls).  If both the thermal barrier and the heated volume are made thinner, the temperature range over which stable amorphous antimony can be produced increases. (The evidence that the antimony is amorphous is confirmed by the observation of annealing from resistance drift.)

PCM aficionados will ask two key questions: “What are the on-to-off resistance ratios and what is long term stability?”  To date on-to-off resistance ratios of greater than two orders of magnitude have been achieved for the stable amorphous state space shown in the 3D plot above. Although there is some reduction towards higher temperatures, usable on-to-off ratios and retention times are possible at temperatures well above room temperature.

Regarding stability: Despite the fact that the amorphous state is stable, it is naturally inclined to return to a crystalline state, but the time this takes is significantly longer than a DRAM’s bit decay.  With a thermal barrier thickness of 40nm and antimony thickness of 5nm, room temperature amorphous-to-crystallization or retention time is measured in hundreds of seconds. However reducing the antimony sample thickness to 3nm (with the same 40nm thermal barrier) provides longer periods of stability: room temperature values of 100,000 seconds have been reported

This is a dramatic illustration of the important role that nanoscale confinement and interfaces play in effecting very large positive changes in the stability of the amorphous state. Clearly there is much scope for improving retention times with new structures, new interface materials and even smaller volumes of material.

The authors of this new work claim they have already reached a performance level for monatomic antimony phase-change memories (Sb-PCMs) which would allow the devices to be used for in-memory computation tasks, with retention times orders of magnitude higher than DRAMs.

These first steps towards single-element PCMs have only just scratched the surface. One of the most interesting aspects of this work is the revelation that heated volume, nano-confinement, and interface surfaces all play a role as important variables. These findings have moved us into an area of technology where surface roughness at the atomic level now becomes an important design consideration.

A short video by IBM gives a 2½ minute overview of this research: https://youtu.be/89bYjLyffUE

 

 

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