Persistence of Charge Ordering Instability to Coulomb Engineering in the Excitonic Insulator Candidate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi>TiSe</mml:mi> </mml:mrow> <mml:

<a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msub> <a:mi>TiSe</a:mi> <a:mn>2</a:mn> </a:msub> </a:math> has long been considered one of the best candidate materials to host the elusive excitonic insulator (EI) phase. However, a finite coupling to the lattice can generically be expected, while a lack of “smoking-gun” signatures for the importance of the electron-hole interaction in driving the phase transition has rendered it challenging to distinguish the EI from the conventional charge-density wave (CDW) phase. Here, we demonstrate a new approach, exploiting the susceptibility of excitons to dielectric screening. We combine mechanical exfoliation with molecular-beam epitaxy to fabricate ultraclean van der Waals heterostructures of monolayer (ML) <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mrow> <c:msub> <c:mrow> <c:mi>TiSe</c:mi> </c:mrow> <c:mrow> <c:mn>2</c:mn> </c:mrow> </c:msub> </c:mrow> </c:math> /graphite and ML <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:mrow> <e:msub> <e:mrow> <e:mi>TiSe</e:mi> </e:mrow> <e:mrow> <e:mn>2</e:mn> </e:mrow> </e:msub> </e:mrow> <e:mo>/</e:mo> <e:mi>h</e:mi> </e:math> -BN. We observe how the modified substrate screening environment drives a renormalization of the quasiparticle band gap of the <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:mrow> <g:msub> <g:mrow> <g:mi>TiSe</g:mi> </g:mrow> <g:mrow> <g:mn>2</g:mn> </g:mrow> </g:msub> </g:mrow> </g:math> layer, signifying its susceptibility to Coulomb engineering. The temperature-dependent evolution of its electronic structure, however, remains unaffected, indicating that excitons are not required to drive the CDW transition in <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"> <i:mrow> <i:msub> <i:mrow> <i:mi>TiSe</i:mi> </i:mrow> <i:mrow> <i:mn>2</i:mn> </i:mrow> </i:msub> </i:mrow> </i:math> .

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Publication Details

Journal
Physical Review X
Published
2025-11-12
DOI
https://doi.org/10.1103/9trc-9865
Citations
3
Primary Topic
2D Materials and Applications
Type
article
Field-Weighted Citation Impact
1.55
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article

Persistence of Charge Ordering Instability to Coulomb Engineering in the Excitonic Insulator Candidate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi>TiSe</mml:mi> </mml:mrow> <mml:

Dina Carbone, Philip A. E. Murgatroyd, Tim O. Wehling, Jacek Osiecki et al.
3 citations
Physical Review X
2D Materials and Applications
1.55
article

Persistence of Charge Ordering Instability to Coulomb Engineering in the Excitonic Insulator Candidate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi>TiSe</mml:mi> </mml:mrow> <mml:

Dina Carbone, Philip A. E. Murgatroyd, Tim O. Wehling, Jacek Osiecki, P. D. C. King, Sebastian Buchberger, Craig Polley, Jan Berges, Akhil Rajan, Yann in ’t Veld, Bruno Kenichi Saika, Brendan Edwards, Naina Kushwaha, Maria H. Visscher
article en
3 citations

Abstract

<a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msub> <a:mi>TiSe</a:mi> <a:mn>2</a:mn> </a:msub> </a:math> has long been considered one of the best candidate materials to host the elusive excitonic insulator (EI) phase. However, a finite coupling to the lattice can generically be expected, while a lack of “smoking-gun” signatures for the importance of the electron-hole interaction in driving the phase transition has rendered it challenging to distinguish the EI from the conventional charge-density wave (CDW) phase. Here, we demonstrate a new approach, exploiting the susceptibility of excitons to dielectric screening. We combine mechanical exfoliation with molecular-beam epitaxy to fabricate ultraclean van der Waals heterostructures of monolayer (ML) <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mrow> <c:msub> <c:mrow> <c:mi>TiSe</c:mi> </c:mrow> <c:mrow> <c:mn>2</c:mn> </c:mrow> </c:msub> </c:mrow> </c:math> /graphite and ML <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:mrow> <e:msub> <e:mrow> <e:mi>TiSe</e:mi> </e:mrow> <e:mrow> <e:mn>2</e:mn> </e:mrow> </e:msub> </e:mrow> <e:mo>/</e:mo> <e:mi>h</e:mi> </e:math> -BN. We observe how the modified substrate screening environment drives a renormalization of the quasiparticle band gap of the <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:mrow> <g:msub> <g:mrow> <g:mi>TiSe</g:mi> </g:mrow> <g:mrow> <g:mn>2</g:mn> </g:mrow> </g:msub> </g:mrow> </g:math> layer, signifying its susceptibility to Coulomb engineering. The temperature-dependent evolution of its electronic structure, however, remains unaffected, indicating that excitons are not required to drive the CDW transition in <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"> <i:mrow> <i:msub> <i:mrow> <i:mi>TiSe</i:mi> </i:mrow> <i:mrow> <i:mn>2</i:mn> </i:mrow> </i:msub> </i:mrow> </i:math> .

Physical Review XVol. 15(4)
Universität Hamburg (DE), University of St Andrews (GB), University of Bremen (DE), Lund University (SE), Research Complex at Harwell (GB), Max Planck Institute for Chemical Physics of Solids (DE), Centro Laser (IT), MAX IV Laboratory (SE), Max Planck Institute for the Structure and Dynamics of Matter (DE), Hamburg Centre for Ultrafast Imaging
Openalex Percentile: Top 16%
2D Materials and Applications
1.55
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