Thermal conductivity of chemical vapor deposition diamond enriched with 13C isotope

被引:0
作者
Inyushkin, A. V. [1 ]
Ralchenko, V. G. [2 ,3 ]
Bolshakov, A. P. [2 ]
Khomich, A. A. [4 ]
Chernodubov, D. A. [1 ]
Taldenkov, A. N. [1 ]
Saraykin, V. V. [1 ]
Kilin, S. Ya. [5 ]
机构
[1] Natl Res Ctr Kurchatov Inst, Moscow 123182, Russia
[2] Russian Acad Sci, Prokhorov Inst Gen Phys, Moscow 119991, Russia
[3] Harbin Inst Technol, Harbin 150080, Peoples R China
[4] Russian Acad Sci, Kotelnikov Inst Radio Engn & Elect, Fryazino 141120, Russia
[5] Natl Res Nucl Univ MEPhI, Moscow 115409, Russia
关键词
RAMAN-SCATTERING; PHONON-SCATTERING; LATTICE-DYNAMICS; HIGH-RESOLUTION; CRYSTALS; TRANSPORT; NITROGEN; SPECTRA; MODEL;
D O I
10.1063/5.0255049
中图分类号
O59 [应用物理学];
学科分类号
摘要
Thermal conductivity kappa(T) of single-crystal CVD diamond enriched with C-13 isotope to 98.16% was measured by the method of steady-state longitudinal heat flow in the temperature range from 6 to 410 K. This crystal with low nitrogen impurity content ( <50 ppb) showed thermal conductivity 2010 +/- 50 W m(-1) K-1 at 300 K (with a maximum of 12 100 W m(-1) K-1 at 83 K), which is significantly lower than that of diamond with natural isotopic composition: kappa(300K) = 2360 +/- 50 W m(-1) K-1. The measured data were analyzed using first-principles theory and the Callaway model, taking into account phonon scattering in three-phonon processes, scattering at sample boundaries and at isotopes. The first-principles calculations overestimate the thermal conductivity compared to the measured one near and to the right of the kappa(T) peak, indicating the presence of significant additional phonon scattering by lattice defects in the studied chemically pure diamond samples. The results of both theoretical approaches for thermal conductivity at 300 K are in good agreement with our measured data and other published experimental data for isotopically modified diamonds. First-principles calculations yield a thermal conductivity ratio of kappa(12)(T)/kappa(13)(T)=1.072 for monoisotopic defect-free C-12 and C-13 crystals at 300 K. This ratio decreases at high temperatures to a value of 1.041 according to the Leibfried-Schlomann theory and to a value of 0.921 at very low temperatures. (c) 2025 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution-NonCommercial 4.0International (CC BY-NC) license (https://creativecommons.org/licenses/by-nc/4.0/).
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页数:11
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