Preparation, electronic structure and piezooptical properties of solid solutions Tl3PbBr5–xIx

Phase diagram of the Tl3PbBr5–Tl3PbI5 section of the reciprocal system 2TlI + PbBr2⇔2TlBr + PbI2 was investigated by differential thermal and X-ray phase analysis methods on 18 alloys. The section is quasi-binary, of eutectic type, with the invariant point coordinates 76 mol% Tl3PbI5 and 355 °C. The...

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Veröffentlicht in:Materials chemistry and physics 2019-04, Vol.227, p.255-264
Hauptverfasser: Khyzhun, O.Y., Fochuk, P.M., Fedorchuk, A.O., Piasecki, M., Kityk, I.V., Myronchuk, G.L., Levkovets, S.I., Piskach, L.V., Parasyuk, O.V.
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container_title Materials chemistry and physics
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creator Khyzhun, O.Y.
Fochuk, P.M.
Fedorchuk, A.O.
Piasecki, M.
Kityk, I.V.
Myronchuk, G.L.
Levkovets, S.I.
Piskach, L.V.
Parasyuk, O.V.
description Phase diagram of the Tl3PbBr5–Tl3PbI5 section of the reciprocal system 2TlI + PbBr2⇔2TlBr + PbI2 was investigated by differential thermal and X-ray phase analysis methods on 18 alloys. The section is quasi-binary, of eutectic type, with the invariant point coordinates 76 mol% Tl3PbI5 and 355 °C. The addition of Tl3PbI5 results in stabilization of the high-temperature (HT) modification of Tl3PbBr5 forming a substitution solid solution, which at room temperature occupies the concentration range of ∼9–71 mol% Tl3PbI5. The solid solution range of low-temperature (LT) Tl3PbBr5 is minor (0–∼6 mol% Tl3PbI5), and that of Tl3PbI5 is in the range of ∼71–100 mol% Tl3PbI5. Tl3PbBr2.5I2.5 crystals were grown by Bridgman-Stockbarger method; they belong to wide-gap semiconductors with Eg decreasing from 2.45 eV at 100 K to 2.36 eV at 300 K. Based on X-ray photoelectron (XP) core-level spectra, one can conclude that the Tl3PbBr2.5I2.5 crystal reveals the XP fine-structure peculiarities well ascribed to thallium, lead, bromine and iodine, constituent atoms of the quaternary halide under consideration. Treatment of the Tl3PbBr2.5I2.5 crystal with 3 keV Ar+ ions reveals that the Pb–I bonds are somewhat weaker in this compound, as compared to the Pb–Br, Tl–Br and Tl–I bonds. Comparison with the similar XP measurements of the related ternary bromide and iodide (Tl3PbBr5 and Tl3PbI5) indicates that the positive effective charge of lead atoms gradually decreases when going from Tl3PbBr5 to Tl3PbBr2.5I2.5 and, further, to Tl3PbI5, while the charge state of thallium atoms does not change in the above sequence of compounds. In the sequence Tl3PbBr5 → Tl3PbBr2.5I2.5 → Tl3PbI5 the relative peak intensity of the XP valence-band spectrum monotonously decreases. The laser stimulated piezooptics at 1150 nm excited by 1540 nm Er:glass nanosecond laser and its second harmonic generation are reported. [Display omitted] •Phase diagram of Tl3PbBr5–Tl3PbI5 section of 2TlI + PbBr2⇔2TlBr + PbI2 system is studied.•Tl3PbBr2.5I2.5 single crystals have been grown by Bridgman-Stockbarger method.•Electronic structure of the Tl3PbBr2.5I2.5 crystal is studied by XPS and XES methods.•Tl3PbBr2.5I2.5 is a semiconductor: Eg decreases from 2.45 eV at 100 K to 2.36 eV at 300 K.•Effects of laser stimulated piezooptics are explored for Tl3PbBr2.5I2.5
doi_str_mv 10.1016/j.matchemphys.2019.02.018
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The section is quasi-binary, of eutectic type, with the invariant point coordinates 76 mol% Tl3PbI5 and 355 °C. The addition of Tl3PbI5 results in stabilization of the high-temperature (HT) modification of Tl3PbBr5 forming a substitution solid solution, which at room temperature occupies the concentration range of ∼9–71 mol% Tl3PbI5. The solid solution range of low-temperature (LT) Tl3PbBr5 is minor (0–∼6 mol% Tl3PbI5), and that of Tl3PbI5 is in the range of ∼71–100 mol% Tl3PbI5. Tl3PbBr2.5I2.5 crystals were grown by Bridgman-Stockbarger method; they belong to wide-gap semiconductors with Eg decreasing from 2.45 eV at 100 K to 2.36 eV at 300 K. Based on X-ray photoelectron (XP) core-level spectra, one can conclude that the Tl3PbBr2.5I2.5 crystal reveals the XP fine-structure peculiarities well ascribed to thallium, lead, bromine and iodine, constituent atoms of the quaternary halide under consideration. Treatment of the Tl3PbBr2.5I2.5 crystal with 3 keV Ar+ ions reveals that the Pb–I bonds are somewhat weaker in this compound, as compared to the Pb–Br, Tl–Br and Tl–I bonds. Comparison with the similar XP measurements of the related ternary bromide and iodide (Tl3PbBr5 and Tl3PbI5) indicates that the positive effective charge of lead atoms gradually decreases when going from Tl3PbBr5 to Tl3PbBr2.5I2.5 and, further, to Tl3PbI5, while the charge state of thallium atoms does not change in the above sequence of compounds. In the sequence Tl3PbBr5 → Tl3PbBr2.5I2.5 → Tl3PbI5 the relative peak intensity of the XP valence-band spectrum monotonously decreases. The laser stimulated piezooptics at 1150 nm excited by 1540 nm Er:glass nanosecond laser and its second harmonic generation are reported. [Display omitted] •Phase diagram of Tl3PbBr5–Tl3PbI5 section of 2TlI + PbBr2⇔2TlBr + PbI2 system is studied.•Tl3PbBr2.5I2.5 single crystals have been grown by Bridgman-Stockbarger method.•Electronic structure of the Tl3PbBr2.5I2.5 crystal is studied by XPS and XES methods.•Tl3PbBr2.5I2.5 is a semiconductor: Eg decreases from 2.45 eV at 100 K to 2.36 eV at 300 K.•Effects of laser stimulated piezooptics are explored for Tl3PbBr2.5I2.5</description><identifier>ISSN: 0254-0584</identifier><identifier>EISSN: 1879-3312</identifier><identifier>DOI: 10.1016/j.matchemphys.2019.02.018</identifier><language>eng</language><publisher>Lausanne: Elsevier B.V</publisher><subject>Argon ions ; Bonding strength ; Bridgman method ; Bromine ; Chemical bonds ; Crystal growth ; Crystal structure ; Differential thermal analysis ; Electronic structure ; High temperature ; Iodine ; Optical spectra ; Phase diagram ; Phase diagrams ; Photoelectrons ; Second harmonic generation ; Single crystal growth ; Solid solutions ; Thallium ; XPS</subject><ispartof>Materials chemistry and physics, 2019-04, Vol.227, p.255-264</ispartof><rights>2019 Elsevier B.V.</rights><rights>Copyright Elsevier BV Apr 1, 2019</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0254058419301130$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27901,27902,65306</link.rule.ids></links><search><creatorcontrib>Khyzhun, O.Y.</creatorcontrib><creatorcontrib>Fochuk, P.M.</creatorcontrib><creatorcontrib>Fedorchuk, A.O.</creatorcontrib><creatorcontrib>Piasecki, M.</creatorcontrib><creatorcontrib>Kityk, I.V.</creatorcontrib><creatorcontrib>Myronchuk, G.L.</creatorcontrib><creatorcontrib>Levkovets, S.I.</creatorcontrib><creatorcontrib>Piskach, L.V.</creatorcontrib><creatorcontrib>Parasyuk, O.V.</creatorcontrib><title>Preparation, electronic structure and piezooptical properties of solid solutions Tl3PbBr5–xIx</title><title>Materials chemistry and physics</title><description>Phase diagram of the Tl3PbBr5–Tl3PbI5 section of the reciprocal system 2TlI + PbBr2⇔2TlBr + PbI2 was investigated by differential thermal and X-ray phase analysis methods on 18 alloys. The section is quasi-binary, of eutectic type, with the invariant point coordinates 76 mol% Tl3PbI5 and 355 °C. The addition of Tl3PbI5 results in stabilization of the high-temperature (HT) modification of Tl3PbBr5 forming a substitution solid solution, which at room temperature occupies the concentration range of ∼9–71 mol% Tl3PbI5. The solid solution range of low-temperature (LT) Tl3PbBr5 is minor (0–∼6 mol% Tl3PbI5), and that of Tl3PbI5 is in the range of ∼71–100 mol% Tl3PbI5. Tl3PbBr2.5I2.5 crystals were grown by Bridgman-Stockbarger method; they belong to wide-gap semiconductors with Eg decreasing from 2.45 eV at 100 K to 2.36 eV at 300 K. Based on X-ray photoelectron (XP) core-level spectra, one can conclude that the Tl3PbBr2.5I2.5 crystal reveals the XP fine-structure peculiarities well ascribed to thallium, lead, bromine and iodine, constituent atoms of the quaternary halide under consideration. Treatment of the Tl3PbBr2.5I2.5 crystal with 3 keV Ar+ ions reveals that the Pb–I bonds are somewhat weaker in this compound, as compared to the Pb–Br, Tl–Br and Tl–I bonds. Comparison with the similar XP measurements of the related ternary bromide and iodide (Tl3PbBr5 and Tl3PbI5) indicates that the positive effective charge of lead atoms gradually decreases when going from Tl3PbBr5 to Tl3PbBr2.5I2.5 and, further, to Tl3PbI5, while the charge state of thallium atoms does not change in the above sequence of compounds. In the sequence Tl3PbBr5 → Tl3PbBr2.5I2.5 → Tl3PbI5 the relative peak intensity of the XP valence-band spectrum monotonously decreases. The laser stimulated piezooptics at 1150 nm excited by 1540 nm Er:glass nanosecond laser and its second harmonic generation are reported. [Display omitted] •Phase diagram of Tl3PbBr5–Tl3PbI5 section of 2TlI + PbBr2⇔2TlBr + PbI2 system is studied.•Tl3PbBr2.5I2.5 single crystals have been grown by Bridgman-Stockbarger method.•Electronic structure of the Tl3PbBr2.5I2.5 crystal is studied by XPS and XES methods.•Tl3PbBr2.5I2.5 is a semiconductor: Eg decreases from 2.45 eV at 100 K to 2.36 eV at 300 K.•Effects of laser stimulated piezooptics are explored for Tl3PbBr2.5I2.5</description><subject>Argon ions</subject><subject>Bonding strength</subject><subject>Bridgman method</subject><subject>Bromine</subject><subject>Chemical bonds</subject><subject>Crystal growth</subject><subject>Crystal structure</subject><subject>Differential thermal analysis</subject><subject>Electronic structure</subject><subject>High temperature</subject><subject>Iodine</subject><subject>Optical spectra</subject><subject>Phase diagram</subject><subject>Phase diagrams</subject><subject>Photoelectrons</subject><subject>Second harmonic generation</subject><subject>Single crystal growth</subject><subject>Solid solutions</subject><subject>Thallium</subject><subject>XPS</subject><issn>0254-0584</issn><issn>1879-3312</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNpNkL1OxDAQhC0EEsfPOwTRkrBrx3FSwok_CQmKo7YSZ6PzKcTBdhBQ8Q68IU9CTlDQzDaj2ZmPsROEDAGL8032XEezpudx_R4yDlhlwDPAcoctsFRVKgTyXbYALvMUZJnvs4MQNgCoEMWC6UdPY-3raN1wllBPJno3WJOE6CcTJ09JPbTJaOnDuTFaU_fJ6N1IPloKieuS4HrbbnXaZoRk1YvH5tLL78-vt7u3I7bX1X2g4797yJ6ur1bL2_T-4eZueXGfEioR07pspMqhAeBFKyvJkRMooaDieVNQ15WKoymNUSZvQcimqDGXUnUddIgFiEN2-ps7l3uZKES9cZMf5peac14VOVSFml3LXxfNVV4teR2MpcFQa_28XLfOagS9Jas3-h9ZvSWrgeuZrPgBh2ly5w</recordid><startdate>20190401</startdate><enddate>20190401</enddate><creator>Khyzhun, O.Y.</creator><creator>Fochuk, P.M.</creator><creator>Fedorchuk, A.O.</creator><creator>Piasecki, M.</creator><creator>Kityk, I.V.</creator><creator>Myronchuk, G.L.</creator><creator>Levkovets, S.I.</creator><creator>Piskach, L.V.</creator><creator>Parasyuk, O.V.</creator><general>Elsevier B.V</general><general>Elsevier BV</general><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20190401</creationdate><title>Preparation, electronic structure and piezooptical properties of solid solutions Tl3PbBr5–xIx</title><author>Khyzhun, O.Y. ; Fochuk, P.M. ; Fedorchuk, A.O. ; Piasecki, M. ; Kityk, I.V. ; Myronchuk, G.L. ; Levkovets, S.I. ; Piskach, L.V. ; Parasyuk, O.V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-e173t-a8b5740b0026d595212e07370924b6eff8721c8cc7c4d035b6a14557ff0f11603</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Argon ions</topic><topic>Bonding strength</topic><topic>Bridgman method</topic><topic>Bromine</topic><topic>Chemical bonds</topic><topic>Crystal growth</topic><topic>Crystal structure</topic><topic>Differential thermal analysis</topic><topic>Electronic structure</topic><topic>High temperature</topic><topic>Iodine</topic><topic>Optical spectra</topic><topic>Phase diagram</topic><topic>Phase diagrams</topic><topic>Photoelectrons</topic><topic>Second harmonic generation</topic><topic>Single crystal growth</topic><topic>Solid solutions</topic><topic>Thallium</topic><topic>XPS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Khyzhun, O.Y.</creatorcontrib><creatorcontrib>Fochuk, P.M.</creatorcontrib><creatorcontrib>Fedorchuk, A.O.</creatorcontrib><creatorcontrib>Piasecki, M.</creatorcontrib><creatorcontrib>Kityk, I.V.</creatorcontrib><creatorcontrib>Myronchuk, G.L.</creatorcontrib><creatorcontrib>Levkovets, S.I.</creatorcontrib><creatorcontrib>Piskach, L.V.</creatorcontrib><creatorcontrib>Parasyuk, O.V.</creatorcontrib><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Materials chemistry and physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Khyzhun, O.Y.</au><au>Fochuk, P.M.</au><au>Fedorchuk, A.O.</au><au>Piasecki, M.</au><au>Kityk, I.V.</au><au>Myronchuk, G.L.</au><au>Levkovets, S.I.</au><au>Piskach, L.V.</au><au>Parasyuk, O.V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Preparation, electronic structure and piezooptical properties of solid solutions Tl3PbBr5–xIx</atitle><jtitle>Materials chemistry and physics</jtitle><date>2019-04-01</date><risdate>2019</risdate><volume>227</volume><spage>255</spage><epage>264</epage><pages>255-264</pages><issn>0254-0584</issn><eissn>1879-3312</eissn><abstract>Phase diagram of the Tl3PbBr5–Tl3PbI5 section of the reciprocal system 2TlI + PbBr2⇔2TlBr + PbI2 was investigated by differential thermal and X-ray phase analysis methods on 18 alloys. The section is quasi-binary, of eutectic type, with the invariant point coordinates 76 mol% Tl3PbI5 and 355 °C. The addition of Tl3PbI5 results in stabilization of the high-temperature (HT) modification of Tl3PbBr5 forming a substitution solid solution, which at room temperature occupies the concentration range of ∼9–71 mol% Tl3PbI5. The solid solution range of low-temperature (LT) Tl3PbBr5 is minor (0–∼6 mol% Tl3PbI5), and that of Tl3PbI5 is in the range of ∼71–100 mol% Tl3PbI5. Tl3PbBr2.5I2.5 crystals were grown by Bridgman-Stockbarger method; they belong to wide-gap semiconductors with Eg decreasing from 2.45 eV at 100 K to 2.36 eV at 300 K. Based on X-ray photoelectron (XP) core-level spectra, one can conclude that the Tl3PbBr2.5I2.5 crystal reveals the XP fine-structure peculiarities well ascribed to thallium, lead, bromine and iodine, constituent atoms of the quaternary halide under consideration. Treatment of the Tl3PbBr2.5I2.5 crystal with 3 keV Ar+ ions reveals that the Pb–I bonds are somewhat weaker in this compound, as compared to the Pb–Br, Tl–Br and Tl–I bonds. Comparison with the similar XP measurements of the related ternary bromide and iodide (Tl3PbBr5 and Tl3PbI5) indicates that the positive effective charge of lead atoms gradually decreases when going from Tl3PbBr5 to Tl3PbBr2.5I2.5 and, further, to Tl3PbI5, while the charge state of thallium atoms does not change in the above sequence of compounds. In the sequence Tl3PbBr5 → Tl3PbBr2.5I2.5 → Tl3PbI5 the relative peak intensity of the XP valence-band spectrum monotonously decreases. The laser stimulated piezooptics at 1150 nm excited by 1540 nm Er:glass nanosecond laser and its second harmonic generation are reported. [Display omitted] •Phase diagram of Tl3PbBr5–Tl3PbI5 section of 2TlI + PbBr2⇔2TlBr + PbI2 system is studied.•Tl3PbBr2.5I2.5 single crystals have been grown by Bridgman-Stockbarger method.•Electronic structure of the Tl3PbBr2.5I2.5 crystal is studied by XPS and XES methods.•Tl3PbBr2.5I2.5 is a semiconductor: Eg decreases from 2.45 eV at 100 K to 2.36 eV at 300 K.•Effects of laser stimulated piezooptics are explored for Tl3PbBr2.5I2.5</abstract><cop>Lausanne</cop><pub>Elsevier B.V</pub><doi>10.1016/j.matchemphys.2019.02.018</doi><tpages>10</tpages></addata></record>
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subjects Argon ions
Bonding strength
Bridgman method
Bromine
Chemical bonds
Crystal growth
Crystal structure
Differential thermal analysis
Electronic structure
High temperature
Iodine
Optical spectra
Phase diagram
Phase diagrams
Photoelectrons
Second harmonic generation
Single crystal growth
Solid solutions
Thallium
XPS
title Preparation, electronic structure and piezooptical properties of solid solutions Tl3PbBr5–xIx
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