Tailoring Phonon‐Driven Responses in α‐MoO <sub>3</sub> through Isotopic Enrichment

T Thiago S. Arnaud (Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA) R Ryan W. Spangler (Department of Materials Science and Engineering The Pennsylvania State University University Park Pennsylvania USA) J Johnathan D. Georgaras J Jonah B. Haber (Department of Materials Science and Engineering Stanford University Stanford California USA) D Daniel Hirt (Department of Mechanical and Aerospace Engineering, University of Virginia 2 , Charlottesville, Virginia 22904,) M Maximilian Obst (Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA) G Gonzalo Álvarez‐Pérez (Istituto Italiano di Tecnologia Center for Biomolecular Nanotechnologies Lecce Italy) M Mackey Long III (Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA) F Felix G. Kaps (Institute of Applied Physics TUD Dresden University of Technology Dresden Germany) J Jakob Wetzel (Institute of Applied Physics TUD Dresden University of Technology Dresden Germany) C Courtney Ragle (Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA) J John E. Buchner (Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA) Y Youngji Kim (Department of Mechanical Engineering Vanderbilt University Nashville Tennessee USA) A Aditha S. Senarath (Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA) R Richarda Niemann (Department of Mechanical Engineering Vanderbilt University Nashville Tennessee USA) M Mingze He G Giulia Carini (Department of Physcial Chemistry Fritz Haber Institute of the Max Planck Society Berlin Germany) U Unai Arregui‐Leon (Department of Physcial Chemistry Fritz Haber Institute of the Max Planck Society Berlin Germany) A Akash C. Behera (Department of Physcial Chemistry Fritz Haber Institute of the Max Planck Society Berlin Germany) R Ramachandra Bangari (Department of Physics and Astronomy University of Iowa Iowa City Iowa USA) N Nihar Sahoo (Department of Physics and Astronomy University of Iowa Iowa City Iowa USA) N Niels C. Brumby (Department of Physcial Chemistry Fritz Haber Institute of the Max Planck Society Berlin Germany) J J. Michael Klopf (Institute of Radiation Physics Helmholtz‐Zentrum Dresden‐Rossendorf Dresden Germany) M Martin Wolf (Fritz-Haber-Institut der Max-Planck-Gesellschaft, Faradayweg 4-6, Berlin 14195, Germany) L Lukas M. Eng S Susanne C. Kehr (Institute of Applied Physics TUD Dresden University of Technology Dresden Germany) T Thomas G. Folland (Department of Physics and Astronomy, The University of Iowa 1 , Iowa City, Iowa 52245,) A Alexander Paarmann (Department of Physcial Chemistry Fritz Haber Institute of the Max Planck Society Berlin Germany) P Patrick E. Hopkins F Felipe Jornada (Department of Materials Science and Engineering Stanford University Stanford California USA) J Jon‐Paul Maria (Department of Materials Science and Engineering The Pennsylvania State University University Park Pennsylvania USA) J Joshua D. Caldwell (Department of Mechanical Engineering Vanderbilt University Nashville Tennessee USA)

Abstract

ABSTRACT The implementation of polaritonic materials into nanoscale devices requires selective tuning of parameters to realize desired spectral or thermal responses. One robust material, α‐MoO 3 , an orthorhombic crystal boasting three distinct phonon dispersions, provides three polaritonic dispersions of hyperbolic phonon polaritons (HPhPs) across the mid‐infrared (MIR). Here, the tunability of both optical and thermal responses in isotopically enriched α‐MoO 3 ( 98 MoO 3, Mo 18 O 3 , and 98 Mo 18 O 3 ) is explored. A uniform ∼5% spectral redshift from 18 O enrichment is observed in both Raman‐ and IR‐active TO phonons. Both the in‐ and out‐of‐plane thermal conductivities for the isotopic variations are reported. Ab initio calculations both replicate experimental findings and analyze the select‐mode three‐phonon scattering contributions. The HPhPs from each isotopic variation are probed with s‐SNOM, and we report an HPhP Q ‐factor maxima increase in 98 Mo 18 O 3 of ∼50% along the [100] in the RB 2 and ∼100% along the [001] in the RB 3 with respect to 98 MoO 3 . Observations in both real and Fourier space of higher‐order HPhP modes propagating in slabs of isotopically enriched α‐MoO 3 without the use of a subdiffractional surface scatterer are presented here. This work establishes the dual‐element isotope enrichment of α‐MoO 3 as an intrinsic strategy to design optical, thermal, and polaritonic properties.

Article Details

Volume / Issue Vol. 38, Issue 39
Published July 01, 2026
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (32)

T

Thiago S. Arnaud

Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA

R

Ryan W. Spangler

Department of Materials Science and Engineering The Pennsylvania State University University Park Pennsylvania USA

J

Johnathan D. Georgaras

J

Jonah B. Haber

Department of Materials Science and Engineering Stanford University Stanford California USA

D

Daniel Hirt

Department of Mechanical and Aerospace Engineering, University of Virginia 2 , Charlottesville, Virginia 22904,

M

Maximilian Obst

Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA

G

Gonzalo Álvarez‐Pérez

Istituto Italiano di Tecnologia Center for Biomolecular Nanotechnologies Lecce Italy

M

Mackey Long III

Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA

F

Felix G. Kaps

Institute of Applied Physics TUD Dresden University of Technology Dresden Germany

J

Jakob Wetzel

Institute of Applied Physics TUD Dresden University of Technology Dresden Germany

C

Courtney Ragle

Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA

J

John E. Buchner

Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA

Y

Youngji Kim

Department of Mechanical Engineering Vanderbilt University Nashville Tennessee USA

A

Aditha S. Senarath

Interdisciplinary Material Science Vanderbilt University Nashville Tennessee USA

R

Richarda Niemann

Department of Mechanical Engineering Vanderbilt University Nashville Tennessee USA

M

Mingze He

G

Giulia Carini

Department of Physcial Chemistry Fritz Haber Institute of the Max Planck Society Berlin Germany

U

Unai Arregui‐Leon

Department of Physcial Chemistry Fritz Haber Institute of the Max Planck Society Berlin Germany

A

Akash C. Behera

Department of Physcial Chemistry Fritz Haber Institute of the Max Planck Society Berlin Germany

R

Ramachandra Bangari

Department of Physics and Astronomy University of Iowa Iowa City Iowa USA

N

Nihar Sahoo

Department of Physics and Astronomy University of Iowa Iowa City Iowa USA

N

Niels C. Brumby

Department of Physcial Chemistry Fritz Haber Institute of the Max Planck Society Berlin Germany

J

J. Michael Klopf

Institute of Radiation Physics Helmholtz‐Zentrum Dresden‐Rossendorf Dresden Germany

M

Martin Wolf

Fritz-Haber-Institut der Max-Planck-Gesellschaft, Faradayweg 4-6, Berlin 14195, Germany

L

Lukas M. Eng

S

Susanne C. Kehr

Institute of Applied Physics TUD Dresden University of Technology Dresden Germany

T

Thomas G. Folland

Department of Physics and Astronomy, The University of Iowa 1 , Iowa City, Iowa 52245,

A

Alexander Paarmann

Department of Physcial Chemistry Fritz Haber Institute of the Max Planck Society Berlin Germany

P

Patrick E. Hopkins

F

Felipe Jornada

Department of Materials Science and Engineering Stanford University Stanford California USA

J

Jon‐Paul Maria

Department of Materials Science and Engineering The Pennsylvania State University University Park Pennsylvania USA

J

Joshua D. Caldwell

Department of Mechanical Engineering Vanderbilt University Nashville Tennessee USA