pith. sign in

arxiv: 2601.13890 · v2 · submitted 2026-01-20 · ❄️ cond-mat.str-el

Correlation-driven branch in doped excitonic insulators

Pith reviewed 2026-05-16 12:44 UTC · model grok-4.3

classification ❄️ cond-mat.str-el
keywords excitonic insulatordopingin-gap branchelectron-hole correlationsone-dimensional modelmatrix product statessingle-particle spectrumoptical conductivity
0
0 comments X

The pith

Doping excitonic insulators produces a correlation-driven branch inside the energy gap.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper studies the single-particle spectrum of doped one-dimensional excitonic insulators with matrix-product-state calculations on a correlated two-band model. It shows that adding carriers creates a new branch of states inside the original gap. Decomposition of the particle propagation dynamics traces this branch to excitonic electron-hole correlations rather than simple band filling. A sympathetic reader would see this as evidence that the branch can serve as a direct spectroscopic marker for those correlations in doped systems.

Core claim

In the doped state of a correlated two-band model for one-dimensional excitonic insulators, numerical calculations reveal an in-gap branch in the single-particle spectrum whose origin lies in excitonic correlations, as shown by examining the propagation dynamics of added particles.

What carries the argument

The doping-induced in-gap branch in the single-particle spectrum, whose dynamics are tied to excitonic correlations.

If this is right

  • The in-gap branch acts as an indicator of electron-hole correlations in doped excitonic insulators.
  • The branch appears in the single-particle spectrum and influences optical conductivity.
  • Decomposing propagation dynamics isolates the role of excitonic pairing in the branch formation.
  • Similar doping-induced features may appear when the model is extended to other parameters or observables.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The branch could appear in two-dimensional or three-dimensional materials if the same correlation mechanism holds.
  • ARPES experiments on candidate compounds such as Ta2NiSe5 or related layered insulators could search for the feature.
  • The result implies that doping other gapped correlated systems might generate analogous correlation-driven states.

Load-bearing premise

The two-band model and its parameters capture the essential physics of real doped excitonic insulators.

What would settle it

Angle-resolved photoemission or tunneling spectroscopy on a real doped excitonic insulator that either detects or fails to detect an in-gap spectral branch would test the claim.

Figures

Figures reproduced from arXiv: 2601.13890 by Ryota Ueda, Satoshi Ejima, Tatsuya Kaneko.

Figure 2
Figure 2. Figure 2: FIG. 2. Densities of states for (a) [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 1
Figure 1. Figure 1: FIG. 1. Single-particle spectra for (a) [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Real part of the optical conductivity [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. (a) Schematic figure of the single-particle creation [PITH_FULL_IMAGE:figures/full_fig_p004_5.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Absolute values of the space-time correlation func [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
read the original abstract

We investigate the spectral properties of doped one-dimensional excitonic insulators. Employing matrix-product-state-based methods, we compute the single-particle spectrum and optical conductivity in a correlated two-band model. Our numerical calculation reveals the emergence of a correlation-driven in-gap branch in the doped state. The origin of the in-gap branch is examined by decomposing the propagation dynamics of a single particle, elucidating that the doping-induced branch is associated with excitonic correlations. Our demonstrations suggest that the doping-induced branch can serve as an indicator of electron-hole correlations.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 3 minor

Summary. The manuscript investigates the spectral properties of doped one-dimensional excitonic insulators using matrix-product-state methods on a correlated two-band model. Numerical computations of the single-particle spectrum and optical conductivity reveal the emergence of a correlation-driven in-gap branch in the doped state. Decomposition of the single-particle propagator attributes this branch to excitonic correlations, suggesting it as a potential diagnostic indicator for electron-hole correlations.

Significance. If the central observation holds, the work provides a controlled numerical demonstration of doping-induced spectral features in a 1D excitonic insulator, with the propagator decomposition offering direct evidence linking the in-gap branch to excitonic effects. The MPS/DMRG approach is well-suited to the 1D setting and yields reproducible results for the model; this could motivate targeted experimental searches for analogous features while highlighting the role of correlations in doped insulators.

minor comments (3)
  1. The abstract and main text would benefit from explicit reporting of model parameters (e.g., interaction strengths, hopping amplitudes), system sizes, bond dimensions, and convergence checks with error estimates on the spectral features, as these are essential for quantitative assessment of the in-gap branch.
  2. Figure captions and the discussion of the propagator decomposition should clarify the precise definition of the excitonic correlation measure used to associate the branch with electron-hole pairing, including any normalization or reference calculations.
  3. A brief comparison of the doped spectrum to the undoped case (or to a non-interacting limit) in the main figures would strengthen the claim that the branch is specifically correlation-driven.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive and accurate summary of our work on the spectral properties of doped one-dimensional excitonic insulators. The assessment correctly highlights the emergence of the correlation-driven in-gap branch and the utility of the propagator decomposition. No major comments were provided in the report.

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper performs a controlled numerical study via MPS/DMRG on a fixed two-band Hamiltonian, directly computing the single-particle spectrum and decomposing the propagator to associate an observed in-gap feature with excitonic correlations. No analytic derivation, parameter fitting to data, or self-citation chain is used to generate the central result; the branch position and its correlation origin emerge as output from the simulation rather than being imposed by construction or renamed from prior inputs. The analysis is therefore self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The work relies on a standard two-band Hubbard-like model whose parameters are chosen to realize an excitonic insulator; no new entities are postulated.

free parameters (1)
  • model interaction strengths
    The two-band model requires choices for on-site and inter-site Coulomb terms that are tuned to produce the insulating gap; these are free parameters fitted to realize the desired phase.
axioms (1)
  • domain assumption The one-dimensional two-band model captures the essential low-energy physics of doped excitonic insulators
    Invoked when extrapolating numerical results to real materials.

pith-pipeline@v0.9.0 · 5377 in / 1194 out tokens · 17239 ms · 2026-05-16T12:44:04.121051+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

72 extracted references · 72 canonical work pages

  1. [1]

    Imada, A

    M. Imada, A. Fujimori, and Y. Tokura, Metal-insulator transitions, Rev. Mod. Phys.70, 1039 (1998)

  2. [2]

    Dagotto, Complexity in strongly correlated electronic 6 systems, Science309, 257 (2005)

    E. Dagotto, Complexity in strongly correlated electronic 6 systems, Science309, 257 (2005)

  3. [3]

    L. V. Keldysh and Y. V. Kopeav, Possible instability of the semimetallic state toward Coulomb interaction, Sov. Phys. Solid State6, 2219 (1965)

  4. [4]

    J. D. Cloizeaux, Exciton instability and crystallographic anomalies in semiconductors, J. Phys. Chem. Solids26, 259 (1965)

  5. [5]

    J´ erome, T

    D. J´ erome, T. M. Rice, and W. Kohn, Excitonic insula- tor, Phys. Rev.158, 462 (1967)

  6. [6]

    B. I. Halperin and T. M. Rice, Possible anomalies at a semimetal-semiconductor transistion, Rev. Mod. Phys. 40, 755 (1968)

  7. [7]

    Kaneko and Y

    T. Kaneko and Y. Ohta, A new era of excitonic insulators, J. Phys. Soc. Jpn.94, 012001 (2025)

  8. [8]

    M. M. Traum, G. Margaritondo, N. V. Smith, J. E. Rowe, and F. J. Di Salvo, TiSe 2: Semiconductor, semimetal, or excitonic insulator, Phys. Rev. B17, 1836 (1978)

  9. [9]

    Cercellier, C

    H. Cercellier, C. Monney, F. Clerc, C. Battaglia, L. De- spont, M. G. Garnier, H. Beck, P. Aebi, L. Patthey, H. Berger, and L. Forr´ o, Evidence for an excitonic in- sulator phase in 1T-TiSe 2, Phys. Rev. Lett.99, 146403 (2007)

  10. [10]

    Kogar, M

    A. Kogar, M. S. Rak, S. Vig, A. A. Husain, F. Flicker, Y. I. Joe, L. Venema, G. J. MacDougall, T. C. Chiang, E. Fradkin, J. van Wezel, and P. Abbamonte, Signatures of exciton condensation in a transition metal dichalco- genide, Science358, 1314 (2017)

  11. [11]

    Gao, Y.-h

    Q. Gao, Y.-h. Chan, P. Jiao, H. Chen, S. Yin, K. Tang- prapha, Y. Yang, X. Li, Z. Liu, D. Shen, S. Jiang, and P. Chen, Observation of possible excitonic charge density waves and metal–insulator transitions in atomically thin semimetals, Nat. Phys.20, 597 (2024)

  12. [12]

    Wakisaka, T

    Y. Wakisaka, T. Sudayama, K. Takubo, T. Mizokawa, M. Arita, H. Namatame, M. Taniguchi, N. Katayama, M. Nohara, and H. Takagi, Excitonic insulator state in Ta2NiSe5 probed by photoemission spectroscopy, Phys. Rev. Lett.103, 026402 (2009)

  13. [13]

    K. Seki, Y. Wakisaka, T. Kaneko, T. Toriyama, T. Kon- ishi, T. Sudayama, N. L. Saini, M. Arita, H. Namatame, M. Taniguchi, N. Katayama, M. Nohara, H. Takagi, T. Mizokawa, and Y. Ohta, Excitonic Bose-Einstein con- densation in Ta 2NiSe5 above room temperature, Phys. Rev. B90, 155116 (2014)

  14. [14]

    Yamada, K

    T. Yamada, K. Domon, and Y. ¯Ono, FFLO excitonic state in the three-chain Hubbard model for Ta 2NiSe5, J. Phys. Soc. Jpn.85, 053703 (2016)

  15. [15]

    Y. F. Lu, H. Kono, T. I. Larkin, A. W. Rost, T. Takayama, A. V. Boris, B. Keimer, and H. Takagi, Zero-gap semiconductor to excitonic insulator transition in Ta2NiSe5, Nat. Commun.8, 14408 (2017)

  16. [16]

    K. Kim, H. Kim, J. Kim, C. Kwon, J. S. Kim, and B. J. Kim, Direct observation of excitonic instability in Ta2NiSe5, Nat. Commun.12, 1969 (2021)

  17. [17]

    Fukutani, R

    K. Fukutani, R. Stania, C. Il Kwon, J. S. Kim, K. J. Kong, J. Kim, and H. W. Yeom, Detecting photoelec- trons from spontaneously formed excitons, Nat. Phys.17, 1024 (2021)

  18. [18]

    Huang, B

    J. Huang, B. Jiang, J. Yao, D. Yan, X. Lei, J. Gao, Z. Guo, F. Jin, Y. Li, Z. Yuan, C. Chai, H. Sheng, M. Pan, F. Chen, J. Liu, S. Gao, G. Qu, B. Liu, Z. Jiang, Z. Liu, X. Ma, S. Zhou, Y. Huang, C. Yun, Q. Zhang, S. Li, S. Jin, H. Ding, J. Shen, D. Su, Y. Shi, Z. Wang, and T. Qian, Evidence for an excitonic insulator state in Ta2Pd3Te5, Phys. Rev. X14, 01...

  19. [19]

    Zhang, Y

    P. Zhang, Y. Dong, D. Yan, B. Jiang, T. Yang, J. Li, Z. Guo, Y. Huang, Haobo, Q. Li, Y. Li, K. Kurokawa, R. Wang, Y. Nie, M. Hashimoto, D. Lu, W.-H. Jiao, J. Shen, T. Qian, Z. Wang, Y. Shi, and T. Kondo, Spon- taneous gap opening and potential excitonic states in an ideal dirac semimetal Ta 2Pd3Te5, Phys. Rev. X14, 011047 (2024)

  20. [20]

    M. S. Hossain, Z.-J. Cheng, Y.-X. Jiang, T. A. Cochran, S.-B. Zhang, H. Wu, X. Liu, X. Zheng, G. Cheng, B. Kim, Q. Zhang, M. Litskevich, J. Zhang, J. Liu, J.-X. Yin, X. P. Yang, J. D. Denlinger, M. Tallarida, J. Dai, E. Vescovo, A. Rajapitamahuni, N. Yao, A. Keselman, Y. Peng, Y. Yao, Z. Wang, L. Balicas, T. Neupert, and M. Z. Hasan, Topological excitonic...

  21. [21]

    Kuneˇ s and P

    J. Kuneˇ s and P. Augustinsk´ y, Excitonic condensa- tion of strongly correlated electrons: The case of Pr0.5Ca0.5CoO3, Phys. Rev. B90, 235112 (2014)

  22. [22]

    Ikeda, Y

    A. Ikeda, Y. H. Matsuda, K. Sato, Y. Ishii, H. Sawabe, D. Nakamura, S. Takeyama, and J. Nasu, Signature of spin-triplet exciton condensations in LaCoO 3 at ultra- high magnetic fields up to 600 T, Nat. Commun.14, 1744 (2023)

  23. [23]

    Varsano, M

    D. Varsano, M. Palummo, E. Molinari, and M. Rontani, A monolayer transition-metal dichalcogenide as a topo- logical excitonic insulator, Nat. Nanotech.15, 367 (2020)

  24. [24]

    Y. Jia, P. Wang, C.-L. Chiu, Z. Song, G. Yu, B. J¨ ack, S. Lei, S. Klemenz, F. A. Cevallos, M. Onyszczak, N. Fishchenko, X. Liu, G. Farahi, F. Xie, Y. Xu, K. Watanabe, T. Taniguchi, B. A. Bernevig, R. J. Cava, L. M. Schoop, A. Yazdani, and S. Wu, Evidence for a monolayer excitonic insulator, Nat. Phys.18, 87 (2022)

  25. [25]

    B. Sun, W. Zhao, T. Palomaki, Z. Fei, E. Runburg, P. Malinowski, X. Huang, J. Cenker, Y.-T. Cui, J.-H. Chu, X. Xu, S. S. Ataei, D. Varsano, M. Palummo, E. Molinari, M. Rontani, and D. H. Cobden, Evidence for equilibrium exciton condensation in monolayer WTe2, Nat. Phys.18, 94 (2022)

  26. [26]

    Bucher, P

    B. Bucher, P. Steiner, and P. Wachter, Excitonic insula- tor phase in TmSe 0.45Te0.55, Phys. Rev. Lett.67, 2717 (1991)

  27. [27]

    D. G. Mazzone, Y. Shen, H. Suwa, G. Fabbris, J. Yang, S. S. Zhang, H. Miao, J. Sears, K. Jia, Y. G. Shi, M. H. Upton, D. M. Casa, X. Liu, J. Liu, C. D. Batista, and M. P. M. Dean, Antiferromagnetic excitonic insulator state in Sr 3Ir2O7, Nat. Commun.13, 913 (2022)

  28. [28]

    H. Qu, H. Liu, and Y. Li, First-principles design of exci- tonic insulators: A review, Chinese Phys. B34, 097101 (2025)

  29. [29]

    Okuma, K

    R. Okuma, K. Yamagami, Y. Fujisawa, C. H. Hsu, Y. Obata, N. Tomoda, M. Dronova, K. Kuroda, H. Ishikawa, K. Kawaguchi, K. Aido, K. Kindo, Y. H. Chan, H. Lin, Y. Ihara, T. Kondo, and Y. Okada, Emer- gent topological magnetism in Hund’s excitonic insulator, arXiv:2405.16781

  30. [30]

    F. J. Di Salvo, D. E. Moncton, and J. V. Waszczak, Electronic properties and superlattice formation in the semimetal TiSe2, Phys. Rev. B14, 4321 (1976)

  31. [31]

    Di Salvo, C

    F. Di Salvo, C. Chen, R. Fleming, J. Waszczak, R. Dunn, S. Sunshine, and J. A. Ibers, Physical and structural properties of the new layered compounds Ta 2NiS5 and Ta2NiSe5, J. Less Common Met.116, 51 (1986)

  32. [32]

    van Wezel, P

    J. van Wezel, P. Nahai-Williamson, and S. S. Saxena, Exciton-phonon-driven charge density wave in TiSe 2, 7 Phys. Rev. B81, 165109 (2010)

  33. [33]

    Monney, G

    C. Monney, G. Monney, P. Aebi, and H. Beck, Electron- hole fluctuation phase in 1T-TiSe 2, Phys. Rev. B85, 235150 (2012)

  34. [34]

    Kaneko, T

    T. Kaneko, T. Toriyama, T. Konishi, and Y. Ohta, Orthorhombic-to-monoclinic phase transition of Ta2NiSe5 induced by the Bose-Einstein condensa- tion of excitons, Phys. Rev. B87, 035121 (2013)

  35. [35]

    Zenker, H

    B. Zenker, H. Fehske, and H. Beck, Fate of the excitonic insulator in the presence of phonons, Phys. Rev. B90, 195118 (2014)

  36. [36]

    Murakami, D

    Y. Murakami, D. Goleˇ z, T. Kaneko, A. Koga, A. J. Millis, and P. Werner, Collective modes in excitonic insulators: Effects of electron-phonon coupling and signatures in the optical response, Phys. Rev. B101, 195118 (2020)

  37. [37]

    Z. Lin, C. Wang, A. Balassis, J. P. Echeverry, A. S. Vasenko, V. M. Silkin, E. V. Chulkov, Y. Shi, J. Zhang, J. Guo, and X. Zhu, Dramatic plasmon response to the charge-density-wave gap development in 1T-TiSe2, Phys. Rev. Lett.129, 187601 (2022)

  38. [38]

    Baldini, A

    E. Baldini, A. Zong, D. Choi, C. Lee, M. H. Michael, L. Windgaetter, I. I. Mazin, S. Latini, D. Azoury, B. Lv, A. Kogar, Y. Su, Y. Wang, Y. Lu, T. Takayama, H. Tak- agi, A. J. Millis, A. Rubio, E. Demler, and N. Gedik, The spontaneous symmetry breaking in Ta 2NiSe5 is structural in nature, Proc. Natl. Acad. Sci. USA120, e2221688120 (2023)

  39. [39]

    C. Chen, X. Chen, W. Tang, Z. Li, S. Wang, S. Ding, Z. Kang, C. Jozwiak, A. Bostwick, E. Rotenberg, M. Hashimoto, D. Lu, J. P. C. Ruff, S. G. Louie, R. J. Birgeneau, Y. Chen, Y. Wang, and Y. He, Role of electron-phonon coupling in excitonic insulator candidate Ta2NiSe5, Phys. Rev. Res.5, 043089 (2023)

  40. [40]

    Eskes, M

    H. Eskes, M. B. J. Meinders, and G. A. Sawatzky, Anomalous transfer of spectral weight in doped strongly correlated systems, Phys. Rev. Lett.67, 1035 (1991)

  41. [41]

    Dagotto, F

    E. Dagotto, F. Ortolani, and D. Scalapino, Single-particle spectral weight of a two-dimensional Hubbard model, Phys. Rev. B46, 3183 (1992)

  42. [42]

    M. B. J. Meinders, H. Eskes, and G. A. Sawatzky, Spectral-weight transfer: Breakdown of low-energy-scale sum rules in correlated systems, Phys. Rev. B48, 3916 (1993)

  43. [43]

    Bulut, D

    N. Bulut, D. Scalapino, and S. White, Quasiparticle dis- persion in the cuprate superconductors and the two- dimensional Hubbard model, Phys. Rev. B50, 7215 (1994)

  44. [44]

    Preuss, W

    R. Preuss, W. Hanke, and W. von der Linden, Quasi- particle dispersion of the 2D Hubbard model: From an insulator to a metal, Phys. Rev. Lett.75, 1344 (1995)

  45. [45]

    S´ en´ echal, D

    D. S´ en´ echal, D. Perez, and M. Pioro-Ladri` ere, Spectral weight of the Hubbard model through cluster perturba- tion theory, Phys. Rev. Lett.84, 522 (2000)

  46. [46]

    Kyung, S

    B. Kyung, S. S. Kancharla, D. S´ en´ echal, A.-M. S. Trem- blay, M. Civelli, and G. Kotliar, Pseudogap induced by short-range spin correlations in a doped Mott insulator, Phys. Rev. B73, 165114 (2006)

  47. [47]

    Kohno, Spectral properties near the Mott transition in the one-dimensional Hubbard model, Phys

    M. Kohno, Spectral properties near the Mott transition in the one-dimensional Hubbard model, Phys. Rev. Lett. 105, 106402 (2010)

  48. [48]

    Kohno, Mott transition in the two-dimensional Hub- bard model, Phys

    M. Kohno, Mott transition in the two-dimensional Hub- bard model, Phys. Rev. Lett.108, 076401 (2012)

  49. [49]

    C. D. Batista, Electronic ferroelectricity in the Falicov- Kimball model, Phys. Rev. Lett.89, 166403 (2002)

  50. [50]

    D. Ihle, M. Pfafferott, E. Burovski, F. X. Bronold, and H. Fehske, Bound state formation and the nature of the excitonic insulator phase in the extended Falicov-Kimball model, Phys. Rev. B78, 193103 (2008)

  51. [51]

    K. Seki, R. Eder, and Y. Ohta, BCS-BEC crossover in the extended Falicov-Kimball model: Variational cluster approach, Phys. Rev. B84, 245106 (2011)

  52. [52]

    S. Mor, M. Herzog, D. Goleˇ z, P. Werner, M. Eckstein, N. Katayama, M. Nohara, H. Takagi, T. Mizokawa, C. Monney, and J. St¨ ahler, Ultrafast electronic band gap control in an excitonic insulator, Phys. Rev. Lett.119, 086401 (2017)

  53. [53]

    Sugimoto, S

    K. Sugimoto, S. Nishimoto, T. Kaneko, and Y. Ohta, Strong coupling nature of the excitonic insulator state in Ta2NiSe5, Phys. Rev. Lett.120, 247602 (2018)

  54. [54]

    Tanabe, T

    T. Tanabe, T. Kaneko, and Y. Ohta, Third-harmonic generation in excitonic insulators, Phys. Rev. B104, 245103 (2021)

  55. [55]

    Osterkorn, Y

    A. Osterkorn, Y. Murakami, T. Kaneko, Z. Sun, A. J. Millis, and D. Goleˇ z, Optical signatures of dynamical ex- citonic condensates, Phys. Rev. Lett.135, 106902 (2025)

  56. [56]

    S. R. White, Density matrix formulation for quantum renormalization groups, Phys. Rev. Lett.69, 2863 (1992)

  57. [57]

    S. R. White, Density-matrix algorithms for quantum renormalization groups, Phys. Rev. B48, 10345 (1993)

  58. [58]

    Schollw¨ ock, The density-matrix renormalization group in the age of matrix product states, Ann

    U. Schollw¨ ock, The density-matrix renormalization group in the age of matrix product states, Ann. Phys.326, 96 (2011)

  59. [59]

    Ejima, T

    S. Ejima, T. Kaneko, Y. Ohta, and H. Fehske, Order, crit- icality, and excitations in the extended Falicov-Kimball model, Phys. Rev. Lett.112, 026401 (2014)

  60. [60]

    Vidal, Efficient classical simulation of slightly entan- gled quantum computations, Phys

    G. Vidal, Efficient classical simulation of slightly entan- gled quantum computations, Phys. Rev. Lett.91, 147902 (2003)

  61. [61]

    Paeckel, T

    S. Paeckel, T. K¨ ohler, A. Swoboda, S. R. Manmana, U. Schollw¨ ock, and C. Hubig, Time-evolution meth- ods for matrix-product states, Ann. Phys.411, 167998 (2019)

  62. [62]

    Milner, S

    S. Milner, S. Johnston, and A. Feiguin, Band mix- ing effects in one-dimensional charge transfer insulators, arXiv:2508.01011. [63]E min(N−1) = min{E 0(Na −1, N b), E0(Na, Nb −1)}, whereE 0(Na, Nb) is the lowest energy in the (N a, Nb) sector

  63. [63]

    Fujiuchi, T

    R. Fujiuchi, T. Kaneko, Y. Ohta, and S. Yunoki, Photoin- duced electron-electron pairing in the extended Falicov- Kimball model, Phys. Rev. B100, 045121 (2019)

  64. [64]

    Ejima, F

    S. Ejima, F. Lange, and H. Fehske, Finite-temperature photoemission in the extended Falicov-Kimball model: a case study for Ta 2NiSe5, SciPost Phys.10, 077 (2021)

  65. [65]

    Ejima, F

    S. Ejima, F. Lange, and H. Fehske, Photoinduced metal- lization of excitonic insulators, Phys. Rev. B105, 245126 (2022)

  66. [66]

    Since we do not assume an interorbital dipole [36] whose presence depends on the choice of two orbitals,σ(ω) does not exhibit an in-gap mode atδ= 0

  67. [67]

    T. I. Larkin, A. N. Yaresko, D. Pr¨ opper, K. A. Kikoin, Y. F. Lu, T. Takayama, Y.-L. Mathis, A. W. Rost, H. Takagi, B. Keimer, and A. V. Boris, Giant exci- ton Fano resonance in quasi-one-dimensional Ta 2NiSe5, Phys. Rev. B95, 195144 (2017)

  68. [68]

    Tsuchida, Y

    S. Tsuchida, Y. Hirose, T. Sekikawa, Y. ¯Ono, T. Hi- rahara, S. Sano, S. Kawaguchi, S. Kobayashi, Y. Uwa- toko, and R. Settai, Metallization and pressure-induced 8 superconductivity in carrier doped excitonic insulator (Ta1−xTix)2NiSe5, J. Phys. Soc. Jpn.94, 114703 (2025)

  69. [69]

    Kuneˇ s and P

    J. Kuneˇ s and P. Augustinsk´ y, Excitonic instability at the spin-state transition in the two-band Hubbard model, Phys. Rev. B89, 115134 (2014)

  70. [70]

    J. Nasu, T. Watanabe, M. Naka, and S. Ishihara, Phase diagram and collective excitations in an excitonic insula- tor from an orbital physics viewpoint, Phys. Rev. B93, 205136 (2016)

  71. [71]

    Geffroy, J

    D. Geffroy, J. Kaufmann, A. Hariki, P. Gunacker, A. Hausoel, and J. Kuneˇ s, Collective modes in excitonic magnets: Dynamical mean-field study, Phys. Rev. Lett. 122, 127601 (2019)

  72. [72]

    Fishman, S

    M. Fishman, S. R. White, and E. M. Stoudenmire, The ITensor Software Library for Tensor Network Calcula- tions, SciPost Phys. Codebases 4 (2022)