Pub Date : 2025-01-02DOI: 10.1103/physrevb.111.045102
Steven H. Simon, Ajit C. Balram
We use several techniques to probe the wave functions proposed to describe the A phases by Das, Das, and Mandal [; ; ]. As opposed to representing fractional quantum Hall liquids, we find these wave functions to describe states that clearly display strong phase separation. In the process of exploring these wave functions, we have also constructed several methods for diagnosing phase separation and generating such wave functions numerically. Finally, we uncover a property of entanglement spectra that can be used as a check for the accuracy of numerics. Published by the American Physical Society2025
{"title":"Phase separation in the putative fractional quantum Hall A phases","authors":"Steven H. Simon, Ajit C. Balram","doi":"10.1103/physrevb.111.045102","DOIUrl":"https://doi.org/10.1103/physrevb.111.045102","url":null,"abstract":"We use several techniques to probe the wave functions proposed to describe the A</a:mi></a:math> phases by Das, Das, and Mandal [; ; ]. As opposed to representing fractional quantum Hall liquids, we find these wave functions to describe states that clearly display strong phase separation. In the process of exploring these wave functions, we have also constructed several methods for diagnosing phase separation and generating such wave functions numerically. Finally, we uncover a property of entanglement spectra that can be used as a check for the accuracy of numerics. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20082,"journal":{"name":"Physical Review B","volume":"66 1","pages":""},"PeriodicalIF":3.7,"publicationDate":"2025-01-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142917013","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-30DOI: 10.1103/physrevb.110.214115
Cherrie S. J. Lee, Carlota Canalias, Robin Buschbeck, Boris Koppitz, Franz Hempel, Zeeshan Amber, Lukas M. Eng, Michael Rüsing
Recently, ion exchange (IE) has been used to periodically modify the coercive field (E</a:mi>c</a:mi></a:msub></a:math>) of the crystal prior to periodic poling, to fabricate fine-pitch domain structures in Rb-doped <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:mrow><c:mi>KTiOP</c:mi><c:msub><c:mi mathvariant="normal">O</c:mi><c:mn>4</c:mn></c:msub></c:mrow></c:math> (RKTP). Here, we use micro-Raman spectroscopy to understand the impact of IE on the vibrational modes related to the Rb/K lattice sites, <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:mrow><e:mi>Ti</e:mi><e:msub><e:mi mathvariant="normal">O</e:mi><e:mn>6</e:mn></e:msub></e:mrow></e:math> octahedra, and <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:mrow><g:mi mathvariant="normal">P</g:mi><g:msub><g:mi mathvariant="normal">O</g:mi><g:mn>4</g:mn></g:msub></g:mrow></g:math> tetrahedra, which all form the basis of the RKTP crystal structure. We analyze the Raman spectra of three different RKTP samples: (1) a RKTP sample that shows a poled domain grating only, (2) a RKTP sample that has an <j:math xmlns:j="http://www.w3.org/1998/Math/MathML"><j:msub><j:mi>E</j:mi><j:mi mathvariant="normal">c</j:mi></j:msub></j:math> grating only, and (3) a RKTP sample that has both an <l:math xmlns:l="http://www.w3.org/1998/Math/MathML"><l:msub><l:mi>E</l:mi><l:mi mathvariant="normal">c</l:mi></l:msub></l:math> and a domain grating of the nominally same spacing. This allows us to determine the impact of IE on the vibrational modes of RKTP. We characterize the changes in the lower Raman peaks related to the alkali-metal ions, as well as observe lattice modifications induced by the incorporation of <n:math xmlns:n="http://www.w3.org/1998/Math/MathML"><n:mrow><n:mi mathvariant="normal">R</n:mi><n:msup><n:mrow><n:mi mathvariant="normal">b</n:mi></n:mrow><n:mo>+</n:mo></n:msup></n:mrow></n:math> that extend further into the crystal bulk than the expected IE depth. Moreover, the influence of IE on the domain walls is also manifested in their Raman peak shift. We discuss our results in terms of the deformation of the <q:math xmlns:q="http://www.w3.org/1998/Math/MathML"><q:mrow><q:mi mathvariant="normal">P</q:mi><q:msub><q:mi mathvariant="normal">O</q:mi><q:mn>4</q:mn></q:msub></q:mrow></q:math> and <t:math xmlns:t="http://www.w3.org/1998/Math/MathML"><t:mrow><t:mi>Ti</t:mi><t:msub><t:mi mathvariant="normal">O</t:mi><t:mn>6</t:mn></t:msub></t:mrow></t:math> groups. Our results highlight the intricate impact of IE on the crystal structure and how it facilitates periodic poling, paving the way for further development of the <v:math xmlns:v="http://www.w3.org/1998/Math/MathML"><v:msub><v:mi>E</v:mi><v:mi mathvariant="normal">c</v:mi></v:msub></v:math>-engineering technique. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2024</jats:copyright-year> </jats:permissions> </jats:supplementary-mat
{"title":"Impact of ion exchange on vibrational modes in Rb-doped KTiOPO4 : A Raman spectroscopy study on the interplay between ion exchange and polarization switching","authors":"Cherrie S. J. Lee, Carlota Canalias, Robin Buschbeck, Boris Koppitz, Franz Hempel, Zeeshan Amber, Lukas M. Eng, Michael Rüsing","doi":"10.1103/physrevb.110.214115","DOIUrl":"https://doi.org/10.1103/physrevb.110.214115","url":null,"abstract":"Recently, ion exchange (IE) has been used to periodically modify the coercive field (E</a:mi>c</a:mi></a:msub></a:math>) of the crystal prior to periodic poling, to fabricate fine-pitch domain structures in Rb-doped <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\"><c:mrow><c:mi>KTiOP</c:mi><c:msub><c:mi mathvariant=\"normal\">O</c:mi><c:mn>4</c:mn></c:msub></c:mrow></c:math> (RKTP). Here, we use micro-Raman spectroscopy to understand the impact of IE on the vibrational modes related to the Rb/K lattice sites, <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\"><e:mrow><e:mi>Ti</e:mi><e:msub><e:mi mathvariant=\"normal\">O</e:mi><e:mn>6</e:mn></e:msub></e:mrow></e:math> octahedra, and <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\"><g:mrow><g:mi mathvariant=\"normal\">P</g:mi><g:msub><g:mi mathvariant=\"normal\">O</g:mi><g:mn>4</g:mn></g:msub></g:mrow></g:math> tetrahedra, which all form the basis of the RKTP crystal structure. We analyze the Raman spectra of three different RKTP samples: (1) a RKTP sample that shows a poled domain grating only, (2) a RKTP sample that has an <j:math xmlns:j=\"http://www.w3.org/1998/Math/MathML\"><j:msub><j:mi>E</j:mi><j:mi mathvariant=\"normal\">c</j:mi></j:msub></j:math> grating only, and (3) a RKTP sample that has both an <l:math xmlns:l=\"http://www.w3.org/1998/Math/MathML\"><l:msub><l:mi>E</l:mi><l:mi mathvariant=\"normal\">c</l:mi></l:msub></l:math> and a domain grating of the nominally same spacing. This allows us to determine the impact of IE on the vibrational modes of RKTP. We characterize the changes in the lower Raman peaks related to the alkali-metal ions, as well as observe lattice modifications induced by the incorporation of <n:math xmlns:n=\"http://www.w3.org/1998/Math/MathML\"><n:mrow><n:mi mathvariant=\"normal\">R</n:mi><n:msup><n:mrow><n:mi mathvariant=\"normal\">b</n:mi></n:mrow><n:mo>+</n:mo></n:msup></n:mrow></n:math> that extend further into the crystal bulk than the expected IE depth. Moreover, the influence of IE on the domain walls is also manifested in their Raman peak shift. We discuss our results in terms of the deformation of the <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\"><q:mrow><q:mi mathvariant=\"normal\">P</q:mi><q:msub><q:mi mathvariant=\"normal\">O</q:mi><q:mn>4</q:mn></q:msub></q:mrow></q:math> and <t:math xmlns:t=\"http://www.w3.org/1998/Math/MathML\"><t:mrow><t:mi>Ti</t:mi><t:msub><t:mi mathvariant=\"normal\">O</t:mi><t:mn>6</t:mn></t:msub></t:mrow></t:math> groups. Our results highlight the intricate impact of IE on the crystal structure and how it facilitates periodic poling, paving the way for further development of the <v:math xmlns:v=\"http://www.w3.org/1998/Math/MathML\"><v:msub><v:mi>E</v:mi><v:mi mathvariant=\"normal\">c</v:mi></v:msub></v:math>-engineering technique. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2024</jats:copyright-year> </jats:permissions> </jats:supplementary-mat","PeriodicalId":20082,"journal":{"name":"Physical Review B","volume":"4 1","pages":""},"PeriodicalIF":3.7,"publicationDate":"2024-12-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142902024","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-30DOI: 10.1103/physrevb.110.245145
Sam Azadi, N. D. Drummond, Sam M. Vinko
We present a study of spin-unpolarized and spin-polarized two-dimensional uniform electron liquids using variational and diffusion quantum Monte Carlo (VMC and DMC) methods with Slater-Jastrow-backflow trial wave functions. Ground-state VMC and DMC energies are obtained in the density range 1≤rs≤40. Single-particle and many-body finite-size errors are corrected using canonical-ensemble twist-averaged boundary conditions and extrapolation of twist-averaged energies to the thermodynamic limit of infinite system size. System-size-dependent errors in Slater-Jastrow-backflow DMC energies caused by partially converged VMC energy minimization calculations are discussed. We find that, for 1≤rs≤5, optimizing the backflow function at each twist lowers the twist-averaged DMC energy at finite system size. However, nonsystematic system-size-dependent effects remain in the DMC energies, which can be partially removed by extrapolation from multiple finite system sizes to infinite system size. The DMC energies in the thermodynamic limit are used to parametrize a local spin density approximation correlation functional for inhomogeneous electron systems. Our zero-temperature phase diagram shows a single transition from a paramagnetic fluid to a hexagonal Wigner crystal at rs=35(1), with no region of stability for a ferromagnetic fluid. Published by the American Physical Society2024
{"title":"Quantum Monte Carlo study of the phase diagram of the two-dimensional uniform electron liquid","authors":"Sam Azadi, N. D. Drummond, Sam M. Vinko","doi":"10.1103/physrevb.110.245145","DOIUrl":"https://doi.org/10.1103/physrevb.110.245145","url":null,"abstract":"We present a study of spin-unpolarized and spin-polarized two-dimensional uniform electron liquids using variational and diffusion quantum Monte Carlo (VMC and DMC) methods with Slater-Jastrow-backflow trial wave functions. Ground-state VMC and DMC energies are obtained in the density range 1</a:mn>≤</a:mo>r</a:mi>s</a:mtext></a:msub>≤</a:mo>40</a:mn></a:mrow></a:math>. Single-particle and many-body finite-size errors are corrected using canonical-ensemble twist-averaged boundary conditions and extrapolation of twist-averaged energies to the thermodynamic limit of infinite system size. System-size-dependent errors in Slater-Jastrow-backflow DMC energies caused by partially converged VMC energy minimization calculations are discussed. We find that, for <b:math xmlns:b=\"http://www.w3.org/1998/Math/MathML\"><b:mrow><b:mn>1</b:mn><b:mo>≤</b:mo><b:msub><b:mi>r</b:mi><b:mtext>s</b:mtext></b:msub><b:mo>≤</b:mo><b:mn>5</b:mn></b:mrow></b:math>, optimizing the backflow function at each twist lowers the twist-averaged DMC energy at finite system size. However, nonsystematic system-size-dependent effects remain in the DMC energies, which can be partially removed by extrapolation from multiple finite system sizes to infinite system size. The DMC energies in the thermodynamic limit are used to parametrize a local spin density approximation correlation functional for inhomogeneous electron systems. Our zero-temperature phase diagram shows a single transition from a paramagnetic fluid to a hexagonal Wigner crystal at <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\"><c:mrow><c:msub><c:mi>r</c:mi><c:mtext>s</c:mtext></c:msub><c:mo>=</c:mo><c:mn>35</c:mn><c:mrow><c:mo>(</c:mo><c:mn>1</c:mn><c:mo>)</c:mo></c:mrow></c:mrow></c:math>, with no region of stability for a ferromagnetic fluid. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2024</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20082,"journal":{"name":"Physical Review B","volume":"3 1","pages":""},"PeriodicalIF":3.7,"publicationDate":"2024-12-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142902094","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-30DOI: 10.1103/physrevb.110.l241411
Egor I. Kiselev, Yiming Pan, Netanel H. Lindner
This Letter establishes a Floquet engineering framework in which coherent high frequency light with a time dependent amplitude can be used to parametrically excite and amplify THz plasmons, mirror plasmonic wave packets in time, and generate momentum-gapped plasmonic band structures, entangled plasmon pairs, and THz radiation in two dimensional Dirac systems. Our results show how low frequency plasmons can be coherently excited and manipulated without the need for THz light. Published by the American Physical Society2024
{"title":"Light-controlled terahertz plasmonic time-varying media: Momentum gaps, entangled plasmon pairs, and pulse-induced time reversal","authors":"Egor I. Kiselev, Yiming Pan, Netanel H. Lindner","doi":"10.1103/physrevb.110.l241411","DOIUrl":"https://doi.org/10.1103/physrevb.110.l241411","url":null,"abstract":"This Letter establishes a Floquet engineering framework in which coherent high frequency light with a time dependent amplitude can be used to parametrically excite and amplify THz plasmons, mirror plasmonic wave packets in time, and generate momentum-gapped plasmonic band structures, entangled plasmon pairs, and THz radiation in two dimensional Dirac systems. Our results show how low frequency plasmons can be coherently excited and manipulated without the need for THz light. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2024</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20082,"journal":{"name":"Physical Review B","volume":"10 1","pages":""},"PeriodicalIF":3.7,"publicationDate":"2024-12-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142901978","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-30DOI: 10.1103/physrevb.110.245146
Joachim Schwardt, Benjamin Michen, Carl Lehmann, Jan Carl Budich
We demonstrate how exceptional points (EPs) naturally occur in the Luttinger liquid (LL) theory describing the low-energy excitations of a microscopic lattice model with sublattice-dependent electron-electron interaction. Upon bosonization, this sublattice dependence directly translates to a nonstandard sine-Gordon-type term responsible for the non-Hermitian matrix structure of the single-particle Green function (GF). As the structure in the lifetime of excitations does not commute with the underlying free Bloch Hamiltonian, non-Hermitian topological properties of the single-particle GF emerge—despite our Hermitian model Hamiltonian. Both finite temperature and a nontrivial Luttinger parameter K≠1 are required for the formation of EPs, and their topological stability in one spatial dimension is guaranteed by the chiral symmetry of our model. In the presence of the aforementioned sine-Gordon term, we resort to leading-order perturbation theory (PT) to compute the single-particle GF. All qualitative findings derived within LL theory are corroborated by comparison to both numerical simulations within the conserving second Born approximation and, for weak interactions and high temperatures, by fermionic plain PT. In certain parameter regimes, quantitative agreement can be reached by a suitable parameter choice in the effective bosonized model. Published by the American Physical Society2024
{"title":"Exceptional Luttinger liquids from sublattice-dependent interaction","authors":"Joachim Schwardt, Benjamin Michen, Carl Lehmann, Jan Carl Budich","doi":"10.1103/physrevb.110.245146","DOIUrl":"https://doi.org/10.1103/physrevb.110.245146","url":null,"abstract":"We demonstrate how exceptional points (EPs) naturally occur in the Luttinger liquid (LL) theory describing the low-energy excitations of a microscopic lattice model with sublattice-dependent electron-electron interaction. Upon bosonization, this sublattice dependence directly translates to a nonstandard sine-Gordon-type term responsible for the non-Hermitian matrix structure of the single-particle Green function (GF). As the structure in the lifetime of excitations does not commute with the underlying free Bloch Hamiltonian, non-Hermitian topological properties of the single-particle GF emerge—despite our Hermitian model Hamiltonian. Both finite temperature and a nontrivial Luttinger parameter K</a:mi>≠</a:mo>1</a:mn></a:mrow></a:math> are required for the formation of EPs, and their topological stability in one spatial dimension is guaranteed by the chiral symmetry of our model. In the presence of the aforementioned sine-Gordon term, we resort to leading-order perturbation theory (PT) to compute the single-particle GF. All qualitative findings derived within LL theory are corroborated by comparison to both numerical simulations within the conserving second Born approximation and, for weak interactions and high temperatures, by fermionic plain PT. In certain parameter regimes, quantitative agreement can be reached by a suitable parameter choice in the effective bosonized model. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2024</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20082,"journal":{"name":"Physical Review B","volume":"5 1","pages":""},"PeriodicalIF":3.7,"publicationDate":"2024-12-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142902022","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-27DOI: 10.1103/physrevb.110.235158
Jaskirat Brar, Sharshad K., B. H. Reddy, Asif Ali, Sakshi Bansal, R. S. Singh, R. Bindu
{"title":"Electronic structure studies of Ni1−xVx across the critical concentration for ferromagnetic to paramagnetic transition","authors":"Jaskirat Brar, Sharshad K., B. H. Reddy, Asif Ali, Sakshi Bansal, R. S. Singh, R. Bindu","doi":"10.1103/physrevb.110.235158","DOIUrl":"https://doi.org/10.1103/physrevb.110.235158","url":null,"abstract":"","PeriodicalId":20082,"journal":{"name":"Physical Review B","volume":"65 1","pages":""},"PeriodicalIF":3.7,"publicationDate":"2024-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142889129","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-27DOI: 10.1103/physrevb.110.214112
Jiyuan Yang, Shi Liu
{"title":"Topological phase transitions in perovskite superlattices driven by temperature, electric field, and doping","authors":"Jiyuan Yang, Shi Liu","doi":"10.1103/physrevb.110.214112","DOIUrl":"https://doi.org/10.1103/physrevb.110.214112","url":null,"abstract":"","PeriodicalId":20082,"journal":{"name":"Physical Review B","volume":"50 1","pages":""},"PeriodicalIF":3.7,"publicationDate":"2024-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142889101","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-27DOI: 10.1103/physrevb.110.214519
Zachary W. Anderson, Marin Spaić, Nikolaos Biniskos, Liam Thompson, Biqiong Yu, Jack Zwettler, Yaohua Liu, Feng Ye, Garrett E. Granroth, Matthew Krogstad, Raymond Osborn, Damjan Pelc, Martin Greven
{"title":"Nanoscale structural correlations in a model cuprate superconductor","authors":"Zachary W. Anderson, Marin Spaić, Nikolaos Biniskos, Liam Thompson, Biqiong Yu, Jack Zwettler, Yaohua Liu, Feng Ye, Garrett E. Granroth, Matthew Krogstad, Raymond Osborn, Damjan Pelc, Martin Greven","doi":"10.1103/physrevb.110.214519","DOIUrl":"https://doi.org/10.1103/physrevb.110.214519","url":null,"abstract":"","PeriodicalId":20082,"journal":{"name":"Physical Review B","volume":"26 1","pages":""},"PeriodicalIF":3.7,"publicationDate":"2024-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142889123","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-27DOI: 10.1103/physrevb.110.245425
Deepankur Thureja, F. Emre Yazıcı, Tomasz Smoleński, Martin Kroner, David J. Norris, Atac İmamoǧlu
{"title":"Electrically defined quantum dots for bosonic excitons","authors":"Deepankur Thureja, F. Emre Yazıcı, Tomasz Smoleński, Martin Kroner, David J. Norris, Atac İmamoǧlu","doi":"10.1103/physrevb.110.245425","DOIUrl":"https://doi.org/10.1103/physrevb.110.245425","url":null,"abstract":"","PeriodicalId":20082,"journal":{"name":"Physical Review B","volume":"66 1","pages":""},"PeriodicalIF":3.7,"publicationDate":"2024-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142889122","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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