Thermochromic effect in YH3-δ and Mg0.1Y0.9H2.9-δ

I.A.M.E. Giebels; S.J. Molen; R. Griessen; M. Di Vece

doi:10.1063/1.1446993

Thermochromic effect in YH3-δ and Mg0.1Y0.9H2.9-δ

I.A.M.E. Giebels, S.J. Molen, R. Griessen, M. Di Vece

Utrecht University

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Research output: Contribution to journal › Article › Academic › peer-review

Abstract

Pure YH32-δ and Mg0.1Y0.9H2.92-δ exhibit large differences in their thermochromic properties. Whereas the transmittance of YH32δ decreases by 9% to 36%, in Mg0.1Y0.9H2.92-δ it decreases by 64% to 83% between 30 °C and 160 °C. This thermochromic effect is caused by hydrogen desorption upon temperature increase. The main difference between the two systems is that the face-centered-cubic to hexagonal-close-packed phase transition between YH21-δ and YH32-δ is absent in Mg0.1Y0.9Hx , i.e., the YHx stays cubic for all 2

Original language	English
Pages (from-to)	1343-1345
Number of pages	3
Journal	Applied Physics Letters
Volume	80
Issue number	8
DOIs	https://doi.org/10.1063/1.1446993
Publication status	Published - 2002

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title = "Thermochromic effect in YH3-δ and Mg0.1Y0.9H2.9-δ",

abstract = "Pure YH32-δ and Mg0.1Y0.9H2.92-δ exhibit large differences in their thermochromic properties. Whereas the transmittance of YH32δ decreases by 9% to 36%, in Mg0.1Y0.9H2.92-δ it decreases by 64% to 83% between 30 °C and 160 °C. This thermochromic effect is caused by hydrogen desorption upon temperature increase. The main difference between the two systems is that the face-centered-cubic to hexagonal-close-packed phase transition between YH21-δ and YH32-δ is absent in Mg0.1Y0.9Hx , i.e., the YHx stays cubic for all 2",

author = "I.A.M.E. Giebels and S.J. Molen and R. Griessen and {Di Vece}, M.",

year = "2002",

doi = "10.1063/1.1446993",

language = "English",

volume = "80",

pages = "1343--1345",

journal = "Applied Physics Letters",

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publisher = "American Institute of Physics",

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T1 - Thermochromic effect in YH3-δ and Mg0.1Y0.9H2.9-δ

AU - Giebels, I.A.M.E.

AU - Molen, S.J.

AU - Griessen, R.

AU - Di Vece, M.

PY - 2002

Y1 - 2002

N2 - Pure YH32-δ and Mg0.1Y0.9H2.92-δ exhibit large differences in their thermochromic properties. Whereas the transmittance of YH32δ decreases by 9% to 36%, in Mg0.1Y0.9H2.92-δ it decreases by 64% to 83% between 30 °C and 160 °C. This thermochromic effect is caused by hydrogen desorption upon temperature increase. The main difference between the two systems is that the face-centered-cubic to hexagonal-close-packed phase transition between YH21-δ and YH32-δ is absent in Mg0.1Y0.9Hx , i.e., the YHx stays cubic for all 2

AB - Pure YH32-δ and Mg0.1Y0.9H2.92-δ exhibit large differences in their thermochromic properties. Whereas the transmittance of YH32δ decreases by 9% to 36%, in Mg0.1Y0.9H2.92-δ it decreases by 64% to 83% between 30 °C and 160 °C. This thermochromic effect is caused by hydrogen desorption upon temperature increase. The main difference between the two systems is that the face-centered-cubic to hexagonal-close-packed phase transition between YH21-δ and YH32-δ is absent in Mg0.1Y0.9Hx , i.e., the YHx stays cubic for all 2

U2 - 10.1063/1.1446993

DO - 10.1063/1.1446993

M3 - Article

SN - 0003-6951

VL - 80

SP - 1343

EP - 1345

JO - Applied Physics Letters

JF - Applied Physics Letters

IS - 8

ER -

Thermochromic effect in YH3-δ and Mg0.1Y0.9H2.9-δ

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