Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films

Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Mohri, Maryam [verfasserIn] Chellali, Mohammed Renda Wang, Di Ivanisenko, Julia

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2021

Schlagwörter:	Ti–Zr–Pd–Cu–Bi thin film High entropy alloy thin film Nanoglass Thermal stability Microstructure

Anmerkung:	© The Korean Institute of Metals and Materials 2021

Übergeordnetes Werk:	Enthalten in: Metals and materials international - Sŏul : Inst., 1995, 28(2021), 7 vom: 20. Sept., Seite 1650-1661
Übergeordnetes Werk:	volume:28 ; year:2021 ; number:7 ; day:20 ; month:09 ; pages:1650-1661

Links:	Volltext

DOI / URN:	10.1007/s12540-021-01051-1

Katalog-ID:	SPR050805045

Internformat


LEADER	01000caa a22002652 4500
001	SPR050805045
003	DE-627
005	20230509103126.0
007	cr uuu---uuuuu
008	230507s2021 xx \|\|\|\|\|o 00\| \|\|eng c
024	7		\|a 10.1007/s12540-021-01051-1 \|2 doi
035			\|a (DE-627)SPR050805045
035			\|a (SPR)s12540-021-01051-1-e
040			\|a DE-627 \|b ger \|c DE-627 \|e rakwb
041			\|a eng
100	1		\|a Mohri, Maryam \|e verfasserin \|4 aut
245	1	0	\|a Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films
264		1	\|c 2021
336			\|a Text \|b txt \|2 rdacontent
337			\|a Computermedien \|b c \|2 rdamedia
338			\|a Online-Ressource \|b cr \|2 rdacarrier
500			\|a © The Korean Institute of Metals and Materials 2021
520			\|a Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract
650		4	\|a Ti–Zr–Pd–Cu–Bi thin film \|7 (dpeaa)DE-He213
650		4	\|a High entropy alloy thin film \|7 (dpeaa)DE-He213
650		4	\|a Nanoglass \|7 (dpeaa)DE-He213
650		4	\|a Thermal stability \|7 (dpeaa)DE-He213
650		4	\|a Microstructure \|7 (dpeaa)DE-He213
700	1		\|a Chellali, Mohammed Renda \|4 aut
700	1		\|a Wang, Di \|4 aut
700	1		\|a Ivanisenko, Julia \|4 aut
773	0	8	\|i Enthalten in \|t Metals and materials international \|d Sŏul : Inst., 1995 \|g 28(2021), 7 vom: 20. Sept., Seite 1650-1661 \|w (DE-627)60059405X \|w (DE-600)2496162-0 \|x 2005-4149 \|7 nnns
773	1	8	\|g volume:28 \|g year:2021 \|g number:7 \|g day:20 \|g month:09 \|g pages:1650-1661
856	4	0	\|u https://dx.doi.org/10.1007/s12540-021-01051-1 \|z lizenzpflichtig \|3 Volltext
912			\|a GBV_USEFLAG_A
912			\|a SYSFLAG_A
912			\|a GBV_SPRINGER
912			\|a GBV_ILN_11
912			\|a GBV_ILN_20
912			\|a GBV_ILN_22
912			\|a GBV_ILN_23
912			\|a GBV_ILN_24
912			\|a GBV_ILN_31
912			\|a GBV_ILN_32
912			\|a GBV_ILN_39
912			\|a GBV_ILN_40
912			\|a GBV_ILN_60
912			\|a GBV_ILN_62
912			\|a GBV_ILN_63
912			\|a GBV_ILN_65
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_74
912			\|a GBV_ILN_90
912			\|a GBV_ILN_95
912			\|a GBV_ILN_100
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_250
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_636
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2001
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2031
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2056
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
912			\|a GBV_ILN_2110
912			\|a GBV_ILN_2111
912			\|a GBV_ILN_2112
912			\|a GBV_ILN_2113
912			\|a GBV_ILN_2118
912			\|a GBV_ILN_2122
912			\|a GBV_ILN_2129
912			\|a GBV_ILN_2143
912			\|a GBV_ILN_2144
912			\|a GBV_ILN_2147
912			\|a GBV_ILN_2148
912			\|a GBV_ILN_2152
912			\|a GBV_ILN_2153
912			\|a GBV_ILN_2188
912			\|a GBV_ILN_2190
912			\|a GBV_ILN_2232
912			\|a GBV_ILN_2336
912			\|a GBV_ILN_2446
912			\|a GBV_ILN_2470
912			\|a GBV_ILN_2472
912			\|a GBV_ILN_2507
912			\|a GBV_ILN_2522
912			\|a GBV_ILN_2548
912			\|a GBV_ILN_4035
912			\|a GBV_ILN_4037
912			\|a GBV_ILN_4046
912			\|a GBV_ILN_4112
912			\|a GBV_ILN_4125
912			\|a GBV_ILN_4126
912			\|a GBV_ILN_4242
912			\|a GBV_ILN_4246
912			\|a GBV_ILN_4249
912			\|a GBV_ILN_4251
912			\|a GBV_ILN_4305
912			\|a GBV_ILN_4306
912			\|a GBV_ILN_4307
912			\|a GBV_ILN_4313
912			\|a GBV_ILN_4322
912			\|a GBV_ILN_4323
912			\|a GBV_ILN_4324
912			\|a GBV_ILN_4325
912			\|a GBV_ILN_4326
912			\|a GBV_ILN_4328
912			\|a GBV_ILN_4333
912			\|a GBV_ILN_4334
912			\|a GBV_ILN_4335
912			\|a GBV_ILN_4336
912			\|a GBV_ILN_4338
912			\|a GBV_ILN_4393
912			\|a GBV_ILN_4700
951			\|a AR
952			\|d 28 \|j 2021 \|e 7 \|b 20 \|c 09 \|h 1650-1661

Indexfelder

author_variant	m m mm m r c mr mrc d w dw j i ji
matchkey_str	article:20054149:2021----::vlainfirsrcueehnclntemlrprisfirduntz
hierarchy_sort_str	2021
publishDate	2021
allfields	10.1007/s12540-021-01051-1 doi (DE-627)SPR050805045 (SPR)s12540-021-01051-1-e DE-627 ger DE-627 rakwb eng Mohri, Maryam verfasserin aut Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Korean Institute of Metals and Materials 2021 Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract Ti–Zr–Pd–Cu–Bi thin film (dpeaa)DE-He213 High entropy alloy thin film (dpeaa)DE-He213 Nanoglass (dpeaa)DE-He213 Thermal stability (dpeaa)DE-He213 Microstructure (dpeaa)DE-He213 Chellali, Mohammed Renda aut Wang, Di aut Ivanisenko, Julia aut Enthalten in Metals and materials international Sŏul : Inst., 1995 28(2021), 7 vom: 20. Sept., Seite 1650-1661 (DE-627)60059405X (DE-600)2496162-0 2005-4149 nnns volume:28 year:2021 number:7 day:20 month:09 pages:1650-1661 https://dx.doi.org/10.1007/s12540-021-01051-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 28 2021 7 20 09 1650-1661
spelling	10.1007/s12540-021-01051-1 doi (DE-627)SPR050805045 (SPR)s12540-021-01051-1-e DE-627 ger DE-627 rakwb eng Mohri, Maryam verfasserin aut Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Korean Institute of Metals and Materials 2021 Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract Ti–Zr–Pd–Cu–Bi thin film (dpeaa)DE-He213 High entropy alloy thin film (dpeaa)DE-He213 Nanoglass (dpeaa)DE-He213 Thermal stability (dpeaa)DE-He213 Microstructure (dpeaa)DE-He213 Chellali, Mohammed Renda aut Wang, Di aut Ivanisenko, Julia aut Enthalten in Metals and materials international Sŏul : Inst., 1995 28(2021), 7 vom: 20. Sept., Seite 1650-1661 (DE-627)60059405X (DE-600)2496162-0 2005-4149 nnns volume:28 year:2021 number:7 day:20 month:09 pages:1650-1661 https://dx.doi.org/10.1007/s12540-021-01051-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 28 2021 7 20 09 1650-1661
allfields_unstemmed	10.1007/s12540-021-01051-1 doi (DE-627)SPR050805045 (SPR)s12540-021-01051-1-e DE-627 ger DE-627 rakwb eng Mohri, Maryam verfasserin aut Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Korean Institute of Metals and Materials 2021 Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract Ti–Zr–Pd–Cu–Bi thin film (dpeaa)DE-He213 High entropy alloy thin film (dpeaa)DE-He213 Nanoglass (dpeaa)DE-He213 Thermal stability (dpeaa)DE-He213 Microstructure (dpeaa)DE-He213 Chellali, Mohammed Renda aut Wang, Di aut Ivanisenko, Julia aut Enthalten in Metals and materials international Sŏul : Inst., 1995 28(2021), 7 vom: 20. Sept., Seite 1650-1661 (DE-627)60059405X (DE-600)2496162-0 2005-4149 nnns volume:28 year:2021 number:7 day:20 month:09 pages:1650-1661 https://dx.doi.org/10.1007/s12540-021-01051-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 28 2021 7 20 09 1650-1661
allfieldsGer	10.1007/s12540-021-01051-1 doi (DE-627)SPR050805045 (SPR)s12540-021-01051-1-e DE-627 ger DE-627 rakwb eng Mohri, Maryam verfasserin aut Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Korean Institute of Metals and Materials 2021 Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract Ti–Zr–Pd–Cu–Bi thin film (dpeaa)DE-He213 High entropy alloy thin film (dpeaa)DE-He213 Nanoglass (dpeaa)DE-He213 Thermal stability (dpeaa)DE-He213 Microstructure (dpeaa)DE-He213 Chellali, Mohammed Renda aut Wang, Di aut Ivanisenko, Julia aut Enthalten in Metals and materials international Sŏul : Inst., 1995 28(2021), 7 vom: 20. Sept., Seite 1650-1661 (DE-627)60059405X (DE-600)2496162-0 2005-4149 nnns volume:28 year:2021 number:7 day:20 month:09 pages:1650-1661 https://dx.doi.org/10.1007/s12540-021-01051-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 28 2021 7 20 09 1650-1661
allfieldsSound	10.1007/s12540-021-01051-1 doi (DE-627)SPR050805045 (SPR)s12540-021-01051-1-e DE-627 ger DE-627 rakwb eng Mohri, Maryam verfasserin aut Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Korean Institute of Metals and Materials 2021 Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract Ti–Zr–Pd–Cu–Bi thin film (dpeaa)DE-He213 High entropy alloy thin film (dpeaa)DE-He213 Nanoglass (dpeaa)DE-He213 Thermal stability (dpeaa)DE-He213 Microstructure (dpeaa)DE-He213 Chellali, Mohammed Renda aut Wang, Di aut Ivanisenko, Julia aut Enthalten in Metals and materials international Sŏul : Inst., 1995 28(2021), 7 vom: 20. Sept., Seite 1650-1661 (DE-627)60059405X (DE-600)2496162-0 2005-4149 nnns volume:28 year:2021 number:7 day:20 month:09 pages:1650-1661 https://dx.doi.org/10.1007/s12540-021-01051-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 28 2021 7 20 09 1650-1661
language	English
source	Enthalten in Metals and materials international 28(2021), 7 vom: 20. Sept., Seite 1650-1661 volume:28 year:2021 number:7 day:20 month:09 pages:1650-1661
sourceStr	Enthalten in Metals and materials international 28(2021), 7 vom: 20. Sept., Seite 1650-1661 volume:28 year:2021 number:7 day:20 month:09 pages:1650-1661
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Ti–Zr–Pd–Cu–Bi thin film High entropy alloy thin film Nanoglass Thermal stability Microstructure
isfreeaccess_bool	false
container_title	Metals and materials international
authorswithroles_txt_mv	Mohri, Maryam @@aut@@ Chellali, Mohammed Renda @@aut@@ Wang, Di @@aut@@ Ivanisenko, Julia @@aut@@
publishDateDaySort_date	2021-09-20T00:00:00Z
hierarchy_top_id	60059405X
id	SPR050805045
language_de	englisch
fullrecord	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR050805045</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230509103126.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230507s2021 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s12540-021-01051-1</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR050805045</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s12540-021-01051-1-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Mohri, Maryam</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2021</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Korean Institute of Metals and Materials 2021</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Ti–Zr–Pd–Cu–Bi thin film</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">High entropy alloy thin film</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Nanoglass</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Thermal stability</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Microstructure</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Chellali, Mohammed Renda</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Wang, Di</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ivanisenko, Julia</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Metals and materials international</subfield><subfield code="d">Sŏul : Inst., 1995</subfield><subfield code="g">28(2021), 7 vom: 20. Sept., Seite 1650-1661</subfield><subfield code="w">(DE-627)60059405X</subfield><subfield code="w">(DE-600)2496162-0</subfield><subfield code="x">2005-4149</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:28</subfield><subfield code="g">year:2021</subfield><subfield code="g">number:7</subfield><subfield code="g">day:20</subfield><subfield code="g">month:09</subfield><subfield code="g">pages:1650-1661</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/s12540-021-01051-1</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_SPRINGER</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_32</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_74</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_90</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_100</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_120</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_138</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_150</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_152</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_171</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_187</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_224</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_250</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_281</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_636</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_702</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2001</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2003</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2004</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2005</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2006</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2007</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2008</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2009</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2010</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2011</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2015</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2020</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2021</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2025</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2026</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2027</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2031</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2034</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2038</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2039</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2044</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2048</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2049</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2050</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2055</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2056</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2057</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2059</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2061</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2064</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2065</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2068</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2088</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2093</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2106</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2107</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2108</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2111</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2113</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2118</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2122</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2129</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2143</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2144</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2147</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2148</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2152</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2153</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2188</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2190</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2232</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2336</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2446</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2470</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2472</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2507</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2522</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2548</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4035</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4046</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4242</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4246</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4251</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4326</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4328</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4333</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4334</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4336</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4393</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">28</subfield><subfield code="j">2021</subfield><subfield code="e">7</subfield><subfield code="b">20</subfield><subfield code="c">09</subfield><subfield code="h">1650-1661</subfield></datafield></record></collection>
author	Mohri, Maryam
spellingShingle	Mohri, Maryam misc Ti–Zr–Pd–Cu–Bi thin film misc High entropy alloy thin film misc Nanoglass misc Thermal stability misc Microstructure Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films
authorStr	Mohri, Maryam
ppnlink_with_tag_str_mv	@@773@@(DE-627)60059405X
format	electronic Article
delete_txt_mv	keep
author_role	aut aut aut aut
collection	springer
remote_str	true
illustrated	Not Illustrated
issn	2005-4149
topic_title	Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films Ti–Zr–Pd–Cu–Bi thin film (dpeaa)DE-He213 High entropy alloy thin film (dpeaa)DE-He213 Nanoglass (dpeaa)DE-He213 Thermal stability (dpeaa)DE-He213 Microstructure (dpeaa)DE-He213
topic	misc Ti–Zr–Pd–Cu–Bi thin film misc High entropy alloy thin film misc Nanoglass misc Thermal stability misc Microstructure
topic_unstemmed	misc Ti–Zr–Pd–Cu–Bi thin film misc High entropy alloy thin film misc Nanoglass misc Thermal stability misc Microstructure
topic_browse	misc Ti–Zr–Pd–Cu–Bi thin film misc High entropy alloy thin film misc Nanoglass misc Thermal stability misc Microstructure
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
format_main_str_mv	Text Zeitschrift/Artikel
carriertype_str_mv	cr
hierarchy_parent_title	Metals and materials international
hierarchy_parent_id	60059405X
hierarchy_top_title	Metals and materials international
isfreeaccess_txt	false
familylinks_str_mv	(DE-627)60059405X (DE-600)2496162-0
title	Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films
ctrlnum	(DE-627)SPR050805045 (SPR)s12540-021-01051-1-e
title_full	Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films
author_sort	Mohri, Maryam
journal	Metals and materials international
journalStr	Metals and materials international
lang_code	eng
isOA_bool	false
recordtype	marc
publishDateSort	2021
contenttype_str_mv	txt
container_start_page	1650
author_browse	Mohri, Maryam Chellali, Mohammed Renda Wang, Di Ivanisenko, Julia
container_volume	28
format_se	Elektronische Aufsätze
author-letter	Mohri, Maryam
doi_str_mv	10.1007/s12540-021-01051-1
title_sort	evaluation of microstructure, mechanical and thermal properties of ti–zr–pd–cu and ti–zr–pd–cu–bi nanoglass thin films
title_auth	Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films
abstract	Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract © The Korean Institute of Metals and Materials 2021
abstractGer	Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract © The Korean Institute of Metals and Materials 2021
abstract_unstemmed	Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract © The Korean Institute of Metals and Materials 2021
collection_details	GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700
container_issue	7
title_short	Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films
url	https://dx.doi.org/10.1007/s12540-021-01051-1
remote_bool	true
author2	Chellali, Mohammed Renda Wang, Di Ivanisenko, Julia
author2Str	Chellali, Mohammed Renda Wang, Di Ivanisenko, Julia
ppnlink	60059405X
mediatype_str_mv	c
isOA_txt	false
hochschulschrift_bool	false
doi_str	10.1007/s12540-021-01051-1
up_date	2024-07-03T17:53:28.318Z
_version_	1803581347143352320
fullrecord_marcxml	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR050805045</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230509103126.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230507s2021 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s12540-021-01051-1</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR050805045</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s12540-021-01051-1-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Mohri, Maryam</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2021</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Korean Institute of Metals and Materials 2021</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract High entropy alloy thin films have been gained attention recently due to their exceptional properties like high corrosion resistance, unique mechanical and physical properties. In this research, DC magnetron sputtering was used to fabricate two kinds of high entropy alloys thin films of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi at two working pressure 2 and 5 mTorr. Structural, thermal, and mechanical properties of the Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi thin films deposited at room temperature using DC magnetron sputtering have been considered in this research. The microstructural analyses using X-ray diffractometer, scanning, and transmission electron microscopies show that the size of glassy clusters and the chemical composition of thin films can be controlled by adjusting the sputtering pressure. The high entropy alloy thin films deposited at high pressure displayed nano-clusters with an amorphous structure. The elemental distribution obtained using atom probe tomography illustrated that Bi atoms were segregated along with the columnar interfaces. Furthermore, Bi addition to the Ti–Zr–Pd–Cu thin film led to increase in thermal stability and decrease in the characteristic enthalpy of the nanoglass thin films. The thin films’ mechanical properties were evaluated by nano-indentation. The results indicated that the Ti–Zr–Pd–Cu–Bi nanoglass thin film had higher strength, hardness, and elastic modulus than the Ti–Zr–Cu–Pd thin film. It was suggested that lattice distortion and nano columnar structure caused to increase in the mechanical properties of Ti–Zr–Pd–Cu–Bi thin film. Graphic abstract</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Ti–Zr–Pd–Cu–Bi thin film</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">High entropy alloy thin film</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Nanoglass</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Thermal stability</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Microstructure</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Chellali, Mohammed Renda</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Wang, Di</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ivanisenko, Julia</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Metals and materials international</subfield><subfield code="d">Sŏul : Inst., 1995</subfield><subfield code="g">28(2021), 7 vom: 20. Sept., Seite 1650-1661</subfield><subfield code="w">(DE-627)60059405X</subfield><subfield code="w">(DE-600)2496162-0</subfield><subfield code="x">2005-4149</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:28</subfield><subfield code="g">year:2021</subfield><subfield code="g">number:7</subfield><subfield code="g">day:20</subfield><subfield code="g">month:09</subfield><subfield code="g">pages:1650-1661</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/s12540-021-01051-1</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_SPRINGER</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_32</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_74</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_90</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_100</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_120</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_138</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_150</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_152</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_171</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_187</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_224</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_250</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_281</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_636</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_702</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2001</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2003</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2004</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2005</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2006</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2007</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2008</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2009</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2010</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2011</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2015</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2020</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2021</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2025</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2026</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2027</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2031</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2034</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2038</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2039</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2044</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2048</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2049</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2050</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2055</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2056</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2057</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2059</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2061</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2064</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2065</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2068</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2088</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2093</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2106</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2107</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2108</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2111</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2113</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2118</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2122</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2129</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2143</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2144</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2147</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2148</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2152</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2153</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2188</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2190</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2232</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2336</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2446</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2470</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2472</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2507</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2522</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2548</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4035</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4046</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4242</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4246</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4251</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4326</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4328</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4333</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4334</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4336</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4393</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">28</subfield><subfield code="j">2021</subfield><subfield code="e">7</subfield><subfield code="b">20</subfield><subfield code="c">09</subfield><subfield code="h">1650-1661</subfield></datafield></record></collection>
score	7.3977413

Nicht das Richtige dabei?

Schreiben Sie uns!

Evaluation of Microstructure, Mechanical and Thermal Properties of Ti–Zr–Pd–Cu and Ti–Zr–Pd–Cu–Bi Nanoglass Thin Films

Nicht das Richtige dabei?

Zugang & Verfügbarkeit

Vorhandene Bände

Nicht das Richtige dabei?