Phase transitions in Ge-Sb phase change materials

Thin films of the phase change material Ge-Sb with Ge concentrations between 7.3 and 81.1   at . % were deposited by cosputtering from elemental targets. Their crystallization behavior was studied using time-resolved x-ray diffraction, Auger electron spectroscopy, differential scanning calorimetry,...

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Veröffentlicht in:Journal of applied physics 2009-03, Vol.105 (6), p.064918-064918-8
Hauptverfasser: Raoux, Simone, Cabral, Cyril, Krusin-Elbaum, Lia, Jordan-Sweet, Jean L., Virwani, Kumar, Hitzbleck, Martina, Salinga, Martin, Madan, Anita, Pinto, Teresa L.
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container_end_page 064918-8
container_issue 6
container_start_page 064918
container_title Journal of applied physics
container_volume 105
creator Raoux, Simone
Cabral, Cyril
Krusin-Elbaum, Lia
Jordan-Sweet, Jean L.
Virwani, Kumar
Hitzbleck, Martina
Salinga, Martin
Madan, Anita
Pinto, Teresa L.
description Thin films of the phase change material Ge-Sb with Ge concentrations between 7.3 and 81.1   at . % were deposited by cosputtering from elemental targets. Their crystallization behavior was studied using time-resolved x-ray diffraction, Auger electron spectroscopy, differential scanning calorimetry, x-ray reflectivity, profilometry, optical reflectivity, and resistivity versus temperature measurements. It was found that the crystallization temperature increases with Ge content. Calculations of the glass transition temperature (which is a lower limit for the crystallization temperature T x ) also show an increase with Ge concentration closely tracking the measured values of T x . For low Ge content samples, Sb x-ray diffraction peaks occurred during a heating ramp at lower temperature than Ge diffraction peaks. The appearance of Ge peaks is related to Ge precipitation and agglomeration. For Ge concentrations of 59.3   at . % and higher, Sb and Ge peaks occurred at the same temperature. Upon crystallization, film mass density and optical reflectivity increase as well as electrical contrast (ratio of resistivity in amorphous phase to crystalline phase) all showed a maximum for the eutectic alloy ( 14.5   at . % Ge). For the alloy with 59.3   at . % Ge there was very little change in any of these parameters, while the alloy with 81.1   at . % Ge behaved opposite to a typical phase change alloy and showed reduced mass density and reflectivity and increased resistivity.
doi_str_mv 10.1063/1.3091271
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Their crystallization behavior was studied using time-resolved x-ray diffraction, Auger electron spectroscopy, differential scanning calorimetry, x-ray reflectivity, profilometry, optical reflectivity, and resistivity versus temperature measurements. It was found that the crystallization temperature increases with Ge content. Calculations of the glass transition temperature (which is a lower limit for the crystallization temperature T x ) also show an increase with Ge concentration closely tracking the measured values of T x . For low Ge content samples, Sb x-ray diffraction peaks occurred during a heating ramp at lower temperature than Ge diffraction peaks. The appearance of Ge peaks is related to Ge precipitation and agglomeration. For Ge concentrations of 59.3   at . % and higher, Sb and Ge peaks occurred at the same temperature. Upon crystallization, film mass density and optical reflectivity increase as well as electrical contrast (ratio of resistivity in amorphous phase to crystalline phase) all showed a maximum for the eutectic alloy ( 14.5   at . % Ge). 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Their crystallization behavior was studied using time-resolved x-ray diffraction, Auger electron spectroscopy, differential scanning calorimetry, x-ray reflectivity, profilometry, optical reflectivity, and resistivity versus temperature measurements. It was found that the crystallization temperature increases with Ge content. Calculations of the glass transition temperature (which is a lower limit for the crystallization temperature T x ) also show an increase with Ge concentration closely tracking the measured values of T x . For low Ge content samples, Sb x-ray diffraction peaks occurred during a heating ramp at lower temperature than Ge diffraction peaks. The appearance of Ge peaks is related to Ge precipitation and agglomeration. For Ge concentrations of 59.3   at . % and higher, Sb and Ge peaks occurred at the same temperature. Upon crystallization, film mass density and optical reflectivity increase as well as electrical contrast (ratio of resistivity in amorphous phase to crystalline phase) all showed a maximum for the eutectic alloy ( 14.5   at . % Ge). For the alloy with 59.3   at . % Ge there was very little change in any of these parameters, while the alloy with 81.1   at . % Ge behaved opposite to a typical phase change alloy and showed reduced mass density and reflectivity and increased resistivity.</abstract><cop>United States</cop><pub>American Institute of Physics</pub><doi>10.1063/1.3091271</doi></addata></record>
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subjects AGGLOMERATION
AMORPHOUS STATE
ANTIMONY ALLOYS
AUGER ELECTRON SPECTROSCOPY
CALORIMETRY
CRYSTALLIZATION
DEPOSITION
EUTECTICS
GERMANIUM ALLOYS
GLASS
HEATING
MATERIALS SCIENCE
PHASE CHANGE MATERIALS
PRECIPITATION
REFLECTIVITY
SPUTTERING
TEMPERATURE MEASUREMENT
THIN FILMS
TIME RESOLUTION
TRANSITION TEMPERATURE
X-RAY DIFFRACTION
title Phase transitions in Ge-Sb phase change materials
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