Abstract:The local bonding structures of GeTe (x = 0.5, 0.6, and 0.7) films prepared through atomic layer deposition (ALD) with Ge(N(Si(CH))) and ((CH)Si)Te precursors were investigated using Ge K-edge X-ray absorption spectroscopy (XAS). The results of the X-ray absorption fine structure analyses show that for all of the compositions, the as-grown films were amorphous with a tetrahedral Ge coordination of a mixture of Ge-Te and Ge-Ge bonds but without any signature of Ge-GeTe decomposition. The compositional evolution… Show more
“…The structure of the Te(SiMe 3 ) 2 precursor is identical to that in the previous works. ,,− The established ALD process, shown in Figure b, consisted of Ge(guan)NMe 2 pulse/purge and co-injection of Te(SiMe 3 ) 2 and NH 3 and purge. The reason for such a peculiar ALD sequence setup was as follows.…”
Section: Resultsmentioning
confidence: 70%
“…While this is not a sufficiently high performance for the storage-class memory application where a switching cycle of >∼10 8 –10 10 is required, it is still promising for the mass-storage device, such as Intel’s recent Optane for solid-state drive application. More importantly, this work elucidated that fundamental chemical research for the new precursor synthesis and extensive engineering works for optimizing the ALD process can pave the way for implementing the ALD GeTe films for actual device application, which has not been the case in the previous works. ,,,,,− The GeTe ALD process described here has high potential utilities for building crystalline-as-deposited GST materials whose crystallization temperature is below 180 °C for further performance improvement as described in more detail in a separate paper …”
Atomic layer deposition
(ALD) of phase-change materials has been
suggested as the most feasible technique for the construction of high-aspect-ratio
architectures required for ultrahigh-density phase-change random access
memory (PcRAM). The recent advances in the ALD technique have established
the foundations for the formation of conformal Ge–Te or Ge–Sb–Te
films, but their electrical performance as a phase-change memory device
has been rarely reported, especially with prolonged cycles. This study
introduced Ge(II)–amido guanidinate (Ge(guan)NMe2 (guan = (
i
PrN)2CNMe2, Me = CH3)) as a new ALD Ge precursor that was compatible
with the high ALD temperature of up to 170 °C, which was necessary
for achieving the high-density and stoichiometric as-deposited GeTe
thin films. The films were deposited in an amorphous state. Coinjection
of NH3 gas with the Te precursor (Te(SiMe3)2) was essential to initiate the feasible ALD reaction with
the new Ge(II) precursor. Ab initio calculation proposed plausible
exergonic chemical reaction pathways where NH3 actively
participated in the dissociation of both −SiMe3 and
guanidinate ligands from Te and Ge precursors, respectively. The ALD
process showed self-limiting growth behavior and produced highly uniform
and conformal morphologies. Low impurity levels (<5%) and a low
crystallization temperature (180 °C) were observed for the samples
deposited at 170 °C. The prototypical memory device showed a
current–voltage curve with a voltage snapback region followed
by switching to a low resistance state. Over 104 cycling
endurance was achieved for the 170 °C grown GeTe film, whereas
inferior endurance (<103) was observed for the low-temperature-grown
GeTe.
“…The structure of the Te(SiMe 3 ) 2 precursor is identical to that in the previous works. ,,− The established ALD process, shown in Figure b, consisted of Ge(guan)NMe 2 pulse/purge and co-injection of Te(SiMe 3 ) 2 and NH 3 and purge. The reason for such a peculiar ALD sequence setup was as follows.…”
Section: Resultsmentioning
confidence: 70%
“…While this is not a sufficiently high performance for the storage-class memory application where a switching cycle of >∼10 8 –10 10 is required, it is still promising for the mass-storage device, such as Intel’s recent Optane for solid-state drive application. More importantly, this work elucidated that fundamental chemical research for the new precursor synthesis and extensive engineering works for optimizing the ALD process can pave the way for implementing the ALD GeTe films for actual device application, which has not been the case in the previous works. ,,,,,− The GeTe ALD process described here has high potential utilities for building crystalline-as-deposited GST materials whose crystallization temperature is below 180 °C for further performance improvement as described in more detail in a separate paper …”
Atomic layer deposition
(ALD) of phase-change materials has been
suggested as the most feasible technique for the construction of high-aspect-ratio
architectures required for ultrahigh-density phase-change random access
memory (PcRAM). The recent advances in the ALD technique have established
the foundations for the formation of conformal Ge–Te or Ge–Sb–Te
films, but their electrical performance as a phase-change memory device
has been rarely reported, especially with prolonged cycles. This study
introduced Ge(II)–amido guanidinate (Ge(guan)NMe2 (guan = (
i
PrN)2CNMe2, Me = CH3)) as a new ALD Ge precursor that was compatible
with the high ALD temperature of up to 170 °C, which was necessary
for achieving the high-density and stoichiometric as-deposited GeTe
thin films. The films were deposited in an amorphous state. Coinjection
of NH3 gas with the Te precursor (Te(SiMe3)2) was essential to initiate the feasible ALD reaction with
the new Ge(II) precursor. Ab initio calculation proposed plausible
exergonic chemical reaction pathways where NH3 actively
participated in the dissociation of both −SiMe3 and
guanidinate ligands from Te and Ge precursors, respectively. The ALD
process showed self-limiting growth behavior and produced highly uniform
and conformal morphologies. Low impurity levels (<5%) and a low
crystallization temperature (180 °C) were observed for the samples
deposited at 170 °C. The prototypical memory device showed a
current–voltage curve with a voltage snapback region followed
by switching to a low resistance state. Over 104 cycling
endurance was achieved for the 170 °C grown GeTe film, whereas
inferior endurance (<103) was observed for the low-temperature-grown
GeTe.
“…The FT was processed on k 2 -weighted ( k : electron momentum) EXAFS in a range of 2–10 Å –1 using a Hanning window. 41 The FT EXAFS magnitudes show the bonding distributions of Er ions in both samples. The overall FT spectra are very different from each other, suggesting that the local environment of Er in the x = 0.2 sample is fundamentally different from that of Er 2 O 3 .…”
We synthesized a series of slightly erbium-substituted
yttrium
iron garnets (Er:YIG), Y
3–
x
Er
x
Fe
5
O
12
at different Er
concentrations (
x
= 0, 0.01, 0.05, 0.10, and 0.20)
using a solid-state reaction and investigated their structural, magnetic,
and optical properties as a function of Er concentration. The volume
of the unit cell slightly increased with Er concentration and Er atoms
predominately replaced Y atoms in the dodecahedrons of YIG. The optical
properties exhibited certain decreases in reflectance in the 1500–1600
nm wavelength range due to the presence of Er
3+
. Despite
the many unpaired 4f electrons in Er
3+
, the total magnetic
moments of Er:YIG showed similar trends with temperatures and magnetic
fields above 30 K. An X-ray magnetic circular dichroism study confirmed
the robust Fe 3d magnetic moments. However, the magnetic moments suddenly
decreased to below 30 K with Er substitution, and the residual magnetism
(
M
R
) and coercive field (
H
C
) in the magnetic hysteresis loops decreased to below
30 K with Er substitution. This implies that Er substitution in YIG
has a negligible effect on magnetic properties over a wide temperature
range except below 30 K where the Er 4f spins are coupled antiparallel
to the majority Fe 3d spins. Our studies demonstrated that above 30
K the magnetic properties of YIG are retained even with Er substitution,
which is evidence that the Er doping scheme is applicable for YIG-based
magneto-optical devices in the mid-infrared regime.
“…The composition of the GeTe film was close to that of Ge 0.6 Te 0.4 , which was confirmed by X-ray fluorescence spectroscopy and TEM-EDS. It was revealed that the as-grown GeTe films were amorphous with a tetrahedral Ge coordination of a uniform mixture of (major) Ge–Te and (minor) Ge–Ge bonds, according to the X-ray absorption fine structure analysis [20].…”
Section: Methodsmentioning
confidence: 99%
“…In this study, an atomic-layer-deposited GeTe-based PCRAM device was fabricated on TiN and W as BE, and the effect of electrode material on the crystallization of the GeTe phase-changing material was investigated. GeTe or Ge–Sb–Te phase-changing material, fabricated via atomic layer deposition (ALD), shows excellent step coverage even in a very-high-aspect-ratio (20:1) trench structure [17,18,19,20]. In addition, the conformal deposition will guarantee uniformity in electrical properties, including the crystallization process, because the void and adhesion issue can be avoided.…”
The electrical switching behavior of the GeTe phase-changing material grown by atomic layer deposition is characterized for the phase change random access memory (PCRAM) application. Planar-type PCRAM devices are fabricated with a TiN or W bottom electrode (BE). The crystallization behavior is characterized by applying an electrical pulse train and analyzed by applying the Johnson–Mehl–Avrami kinetics model. The device with TiN BE shows a high Avrami coefficient (>4), meaning that continuous and multiple nucleations occur during crystallization (set switching). Meanwhile, the device with W BE shows a smaller Avrami coefficient (~3), representing retarded nucleation during the crystallization. In addition, larger voltage and power are necessary for crystallization in case of the device with W BE. It is believed that the thermal conductivity of the BE material affects the temperature distribution in the device, resulting in different crystallization kinetics and set switching behavior.
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