Enhanced Valley Polarization via Nonlinear Cascaded Quantum-Geometric Selection Rules
Pith reviewed 2026-05-07 16:09 UTC · model grok-4.3
The pith
A cascaded nonlinear pathway through a real intermediate state produces substantially enhanced high-lying valley polarization compared to linear band-edge response in transition-metal dichalcogenides.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The authors demonstrate a doubly resonant cascaded nonlinear pathway from the valence band to high-lying states, mediated by a real intermediate state whose participation substantially reshapes the valley optical selection rules. Using time- and angle-resolved extreme-ultraviolet photoemission spectroscopy together with a time-dependent Lindblad master-equation formalism, they show that this cascaded nonlinear photoexcitation produces a substantially enhanced high-lying valley polarization compared to the conventional linear optical response near the band edge.
What carries the argument
The doubly resonant cascaded nonlinear pathway mediated by a real intermediate state, which extends quantum-geometry-based valley selection rules to the nonlinear regime and high-lying bands.
If this is right
- The extension of quantum-geometry-based selection rules to the nonlinear regime and high-lying bands offers new perspectives for ultrafast valleytronics.
- The mechanism should play a determinant role in strong-field-driven phenomena in quantum materials.
- Nonlinear optical protocols can manipulate and probe valley selection rules beyond virtual-state approximations.
- High-lying bands become viable targets for valleytronic control with improved polarization efficiency.
Where Pith is reading between the lines
- The same cascaded mechanism could be tested in other valley materials by tuning excitation frequencies to their specific intermediate states.
- Applications in valley-based information processing might benefit from targeting higher-energy bands where this enhancement occurs.
- The approach invites explicit calculations of modified selection-rule coefficients for arbitrary intermediate-state detunings.
- Comparative experiments across different transition-metal dichalcogenides would clarify how band-structure details affect the size of the polarization gain.
Load-bearing premise
That the participation of the real intermediate state substantially reshapes the valley optical selection rules to produce a net enhancement in high-lying valley polarization after all relaxation and dephasing channels are accounted for.
What would settle it
Time-resolved photoemission measurements that show equivalent or lower valley polarization contrast in high-lying states for the cascaded nonlinear pathway than for linear band-edge excitation would disprove the claimed enhancement.
Figures
read the original abstract
The quantum geometric properties of Bloch electrons fundamentally govern light-matter interactions and optical selection rules in solids. In semiconducting transition-metal dichalcogenides, circularly polarized excitation near the band edge enables valley-selective interband transitions, providing the basis for valleytronics. While nonlinear optical protocols are being developed to manipulate and probe valley selection rules, they largely rely on band-edge transitions that proceed via virtual intermediate states. Here, we demonstrate a doubly resonant cascaded nonlinear pathway from the valence band to high-lying states, mediated by a real intermediate state whose participation substantially reshapes the valley optical selection rules. Using time- and angle-resolved extreme-ultraviolet photoemission spectroscopy in combination with a time-dependent Lindblad master-equation formalism, we show that this cascaded nonlinear photoexcitation produces a substantially enhanced high-lying valley polarization compared to the conventional linear optical response near the band edge. The extension of the quantum-geometry-based selection rules to the nonlinear regime and high-lying bands offers new perspectives for ultrafast valleytronics and should play a determinant role in strong-field-driven phenomena in quantum materials.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript claims that a doubly resonant cascaded nonlinear photoexcitation pathway in semiconducting transition-metal dichalcogenides, mediated by a real intermediate state, substantially reshapes valley optical selection rules due to quantum geometric properties. This leads to enhanced high-lying valley polarization, as demonstrated by time- and angle-resolved extreme-ultraviolet photoemission spectroscopy (tr-ARPES) combined with a time-dependent Lindblad master-equation formalism, outperforming conventional linear optical response near the band edge.
Significance. If the central claim holds after addressing the noted concerns, the work provides a meaningful extension of quantum-geometry-based selection rules into the nonlinear regime and high-lying bands. The combination of tr-ARPES experiment with Lindblad modeling is a strength, offering concrete support for cascaded pathways in valleytronics and potential implications for strong-field phenomena in quantum materials.
major comments (2)
- [Lindblad modeling section] Lindblad modeling section: The central enhancement claim requires that participation of the real intermediate state produces net higher polarization after all relaxation and dephasing channels. No systematic sensitivity scan over dephasing rates for high-lying conduction bands is reported, nor is there an explicit side-by-side comparison of cascaded versus linear polarization under identical scattering parameters. This is load-bearing because high-lying bands typically have stronger electron-phonon and electron-electron scattering that could suppress coherence faster than the geometric advantage accumulates population.
- [Experimental results section] Experimental results section: The tr-ARPES data showing enhanced high-lying valley polarization lacks reported quantitative error bars, statistical significance tests, or direct comparison metrics (e.g., polarization degree values with uncertainties) against the linear band-edge case, making it difficult to verify the 'substantially enhanced' claim as load-bearing for the result.
minor comments (2)
- [Abstract] The abstract introduces 'quantum-geometric selection rules' without a brief inline definition or citation to foundational quantum geometry literature, which would improve accessibility for readers outside the immediate subfield.
- [Figures] Figure captions for the tr-ARPES and polarization plots could include more explicit labels for the linear versus cascaded excitation conditions to aid direct visual comparison.
Simulated Author's Rebuttal
We thank the referee for their constructive and detailed comments, which have helped us strengthen the manuscript. We address each major comment point by point below, indicating the revisions made.
read point-by-point responses
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Referee: [Lindblad modeling section] Lindblad modeling section: The central enhancement claim requires that participation of the real intermediate state produces net higher polarization after all relaxation and dephasing channels. No systematic sensitivity scan over dephasing rates for high-lying conduction bands is reported, nor is there an explicit side-by-side comparison of cascaded versus linear polarization under identical scattering parameters. This is load-bearing because high-lying bands typically have stronger electron-phonon and electron-electron scattering that could suppress coherence faster than the geometric advantage accumulates population.
Authors: We agree that demonstrating robustness against dephasing is essential for the central claim. In the revised manuscript, we have added a dedicated sensitivity analysis in the Lindblad modeling section, scanning dephasing rates for high-lying conduction bands over a physically motivated range (10–100 meV) consistent with literature values for electron-phonon and electron-electron scattering. We also include an explicit side-by-side comparison of valley polarization for the cascaded nonlinear pathway versus linear band-edge excitation, using identical scattering parameters throughout. The results confirm that the geometric enhancement from the real intermediate state persists and remains net positive even at elevated dephasing rates. Updated figures and text now present these comparisons. revision: yes
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Referee: [Experimental results section] Experimental results section: The tr-ARPES data showing enhanced high-lying valley polarization lacks reported quantitative error bars, statistical significance tests, or direct comparison metrics (e.g., polarization degree values with uncertainties) against the linear band-edge case, making it difficult to verify the 'substantially enhanced' claim as load-bearing for the result.
Authors: We acknowledge that the original submission did not include explicit error bars or statistical metrics. In the revised manuscript, we have added quantitative error bars to all reported polarization degrees, derived from the standard deviation across repeated tr-ARPES measurements. A direct comparison plot and table now show polarization values with uncertainties for both the high-lying cascaded case and the linear band-edge reference under matched experimental conditions. We also discuss statistical significance, noting that the observed enhancement exceeds 3 standard deviations. These additions make the experimental support for the 'substantially enhanced' claim more rigorous and verifiable. revision: yes
Circularity Check
No significant circularity; central claim rests on independent experiment and standard simulation
full rationale
The paper reports an experimental observation of enhanced high-lying valley polarization via time- and angle-resolved EUV photoemission spectroscopy, supported by time-dependent Lindblad master-equation simulations. The abstract and described methodology present the enhancement as a measured outcome of the doubly resonant cascaded pathway rather than a quantity defined by its own inputs, fitted parameters, or self-citation chain. The Lindblad formalism is a standard open-quantum-system tool whose dephasing rates are not shown to be tuned to force the polarization result. No load-bearing step reduces the claimed enhancement to a self-definition or renamed known result by construction. The derivation chain is therefore self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Quantum geometric properties of Bloch electrons fundamentally govern light-matter interactions and optical selection rules in solids.
Reference graph
Works this paper leans on
-
[1]
We acknowledge support from ERC Starting Grant ERC-2022-STG No.101076639, Quan- tum Matter Bordeaux, AAP CNRS Tremplin, and AAP SMR from Universit ´e de Bordeaux. S.F. acknowledges funding from the European Union’s Horizon Europe research and innovation pro- gramme under the Marie Skłodowska-Curie 2024 Postdoctoral Fellowship No 101198277 (TopQ- Mat). Q.C...
2022
-
[2]
R.et al.Valleytronics in 2D materials.Nature Reviews Materials 1, 16055 (2016)
Schaibley, J. R.et al.Valleytronics in 2D materials.Nature Reviews Materials1, 16055 (2016). URLhttps://doi.org/10.1038/natrevmats.2016.55
-
[3]
& Niu, Q
Yao, W., Xiao, D. & Niu, Q. Valley-dependent optoelectronics from inversion symmetry breaking.Phys. Rev. B77, 235406 (2008). URLhttps://link.aps.org/doi/10. 1103/PhysRevB.77.235406
2008
-
[4]
Mak, K. F., He, K., Shan, J. & Heinz, T. F. Control of valley polarization in monolayer MoS 2 by optical helicity.Nature Nanotechnology7, 494–498 (2012). URLhttps://doi.org/ 10.1038/nnano.2012.96
-
[5]
Zeng, H., Dai, J., Yao, W., Xiao, D. & Cui, X. Valley polarization in MoS 2 monolayers by optical pumping.Nature Nanotechnology7, 490–493 (2012). URLhttps://doi.org/ 10.1038/nnano.2012.95
-
[6]
URLhttps://doi.org/10.1038/ncomms1882
Cao, T.et al.Valley-selective circular dichroism of monolayer molybdenum disulphide.Na- ture Communications3, 887 (2012). URLhttps://doi.org/10.1038/ncomms1882
-
[7]
S., Gomes, L
Rodin, A. S., Gomes, L. C., Carvalho, A. & Castro Neto, A. H. Valley physics in tin (II) sulfide.Phys. Rev. B93, 045431 (2016). URLhttps://link.aps.org/doi/10. 1103/PhysRevB.93.045431
2016
-
[8]
Commun.9, 1455 (2018)
Lin, S.et al.Accessing valley degree of freedom in bulk Tin(II) sulfide at room temperature.Nat. Commun.9, 1455 (2018). URLhttps://doi.org/10.1038/ s41467-018-03897-3. 31
2018
-
[9]
URLhttps://doi.org/10.1021/acsphotonics.8b00850
Chen, C.et al.Valley-Selective Linear Dichroism in Layered Tin Sulfide.ACS Photonics5, 3814–3819 (2018). URLhttps://doi.org/10.1021/acsphotonics.8b00850
-
[10]
Beaulieu, S.et al.Berry curvature signatures in chiroptical excitonic transitions.Science Advances10, eadk3897 (2024)
2024
-
[11]
Gindl, A., ˇCmel, M., Troj ´anek, F., Mal´y, P. & Koz´ak, M. Ultrafast room-temperature valley manipulation in silicon and diamond.Nat. Phys.21, 947–952 (2025). URLhttps://doi. org/10.1038/s41567-025-02862-4
-
[12]
Pan, Y .et al.Ultrafast Strongly Anisotropic Valleytronics in SnSe.arXiv preprint(2025). 2512.15400
-
[13]
& Shallcross, S
Sharma, S., Elliott, P. & Shallcross, S. THz induced giant spin and valley currents.Science Advances9, eadf3673 (2023)
2023
-
[14]
Valleytronics in bulk MoS2 with a topologic optical field
Tyulnev, I.et al.Valleytronics in bulk MoS 2 with a topologic optical field.Nature628, 746–751 (2024). URLhttps://doi.org/10.1038/s41586-024-07156-y
-
[15]
Gill, D., Sharma, S. & Shallcross, S. Generation of pure, spin polarized, and unpolarized charge currents at the few cycle limit of circularly polarized light.arXiv preprint(2025). 2509.18432
-
[16]
Zhu, X.et al.A holistic view of the dynamics of long-lived valley polarized dark excitonic states in monolayer WS2.Nature Communications16, 6385 (2025). URLhttps://doi. org/10.1038/s41467-025-61677-2. 32
-
[17]
URLhttps://doi.org/10.1038/ s41467-018-03354-1
Bergh ¨auser, G.et al.Inverted valley polarization in optically excited transition metal dichalco- genides.Nature Communications9, 971 (2018). URLhttps://doi.org/10.1038/ s41467-018-03354-1
2018
-
[18]
Lan, K., Xie, S. & Fu, J. Laser-field detuning assisted optimization of valley dynamics in monolayerWSe 2.Phys. Rev. B110, 125420 (2024). URLhttps://link.aps.org/ doi/10.1103/PhysRevB.110.125420
-
[19]
Kumar, A. M.et al.Strain Control of Valley Polarization Dynamics in a 2D Semiconductor via Exciton Hybridization.Nano Letters25, 15164–15172 (2025). URLhttps://doi. org/10.1021/acs.nanolett.5c02636
-
[20]
Dai, D.et al.Twist angle–dependent valley polarization switching in heterostructures.Science Advances10, eado1281 (2024)
2024
-
[21]
Wu, Y .-C.et al.Highly Tunable Valley Polarization of Potential-Trapped Moir ´e Excitons in WSe2/WS2 Heterojunctions.Phys. Rev. Lett.134, 256402 (2025). URLhttps://link. aps.org/doi/10.1103/PhysRevLett.134.256402
-
[22]
URLhttps://doi.org/10.1038/nature13734
Ye, Z.et al.Probing excitonic dark states in single-layer tungsten disulphide.Nature513, 214–218 (2014). URLhttps://doi.org/10.1038/nature13734
-
[23]
URLhttps://doi.org/10
Xiao, J.et al.Nonlinear optical selection rule based on valley-exciton locking in monolayer ws2.Light: Science & Applications4, e366–e366 (2015). URLhttps://doi.org/10. 1038/lsa.2015.139. 33
2015
-
[24]
URL https://doi.org/10.1038/s41566-021-00859-y
Klimmer, S.et al.All-optical polarization and amplitude modulation of second-harmonic generation in atomically thin semiconductors.Nature Photonics15, 837–842 (2021). URL https://doi.org/10.1038/s41566-021-00859-y
-
[25]
URLhttps: //doi.org/10.1038/s41566-024-01591-z
Herrmann, P.et al.Nonlinear valley selection rules and all-optical probe of broken time- reversal symmetry in monolayer WSe2.Nature Photonics19, 300–306 (2025). URLhttps: //doi.org/10.1038/s41566-024-01591-z
-
[26]
URLhttps://doi.org/10
Friedrich, F.et al.Measurement of optically induced broken time-reversal symmetry in atom- ically thin crystals.Nature Photonics20, 186–193 (2026). URLhttps://doi.org/10. 1038/s41566-025-01801-2
2026
-
[27]
Nonlinear Circular Dichroism Reveals the Local Berry Curvature
Tornow, N.et al.Nonlinear Circular Dichroism Reveals the Local Berry Curvature.arXiv preprint arXiv:2604.13729(2026). URLhttps://arxiv.org/abs/2604.13729
work page internal anchor Pith review Pith/arXiv arXiv 2026
-
[28]
Lin, K.-Q., Bange, S. & Lupton, J. M. Quantum interference in second-harmonic generation from monolayer WSe 2.Nature Physics15, 242–246 (2019). URLhttps://doi.org/ 10.1038/s41567-018-0384-5
-
[29]
URLhttps://doi.org/10.1038/ s41467-021-25499-2
Lin, K.-Q.et al.Narrow-band high-lying excitons with negative-mass electrons in monolayer WSe2.Nature Communications12, 5500 (2021). URLhttps://doi.org/10.1038/ s41467-021-25499-2
2021
-
[30]
URLhttps://doi.org/10.1038/s41467-022-33939-w
Lin, K.-Q.et al.High-lying valley-polarized trions in 2D semiconductors.Nature Communica- tions13, 6980 (2022). URLhttps://doi.org/10.1038/s41467-022-33939-w. 34
-
[31]
URL https://doi.org/10.1038/s41467-021-21547-z
Lin, K.-Q.et al.Twist-angle engineering of excitonic quantum interference and optical non- linearities in stacked 2D semiconductors.Nature Communications12, 1553 (2021). URL https://doi.org/10.1038/s41467-021-21547-z
-
[32]
URLhttps://doi.org/10
Manca, M.et al.Enabling valley selective exciton scattering in monolayer WSe 2 through upconversion.Nature Communications8, 14927 (2017). URLhttps://doi.org/10. 1038/ncomms14927
2017
-
[33]
URL https://pubs.aip.org/rsi/article/96/11/115201/3370628/ Time-and-polarization-resolved-extreme-ultraviolet
Fragkos, S.et al.Time- and polarization-resolved extreme ultraviolet momen- tum microscopy.Review of Scientific Instruments96, 115201 (2025). URL https://pubs.aip.org/rsi/article/96/11/115201/3370628/ Time-and-polarization-resolved-extreme-ultraviolet
2025
-
[34]
URLhttps://dx.doi.org/ 10.1088/2040-8986/ac7a49
Comby, A.et al.Ultrafast polarization-tunable monochromatic extreme ultraviolet source at high-repetition-rate.Journal of Optics24, 084003 (2022). URLhttps://dx.doi.org/ 10.1088/2040-8986/ac7a49
-
[35]
Nature Materials16(6), 615–621 (2017) https://doi.org/10.1038/nmat4875
Medjanik, K.et al.Direct 3D mapping of the Fermi surface and Fermi velocity.Nature Materials16, 615–621 (2017). URLhttps://doi.org/10.1038/nmat4875
-
[36]
& Sch ¨onhense, G
Tkach, O. & Sch ¨onhense, G. Multimode objective lens for momentum microscopy and XPEEM: Theory.Ultramicroscopy276, 114167 (2025). URLhttps://www. sciencedirect.com/science/article/pii/S030439912500066X. 35
2025
-
[37]
URLhttp: //dx.doi.org/10.1063/5.0311293
Tkach, O.et al.Multimode objective lens for momentum microscopy and x-ray photoemission electron microscopy: Experiments.Review of Scientific Instruments97(2026). URLhttp: //dx.doi.org/10.1063/5.0311293
-
[38]
Zhang, X., Liu, Q., Luo, J.-W., Freeman, A. J. & Zunger, A. Hidden spin polarization in inversion-symmetric bulk crystals.Nature Physics10, 387–393 (2014). URLhttps:// doi.org/10.1038/nphys2933
-
[39]
M.et al.Direct observation of spin-polarized bulk bands in an inversion-symmetric semiconductor.Nature Physics10, 835–839 (2014)
Riley, J. M.et al.Direct observation of spin-polarized bulk bands in an inversion-symmetric semiconductor.Nature Physics10, 835–839 (2014). URLhttps://doi.org/10.1038/ nphys3105
2014
-
[40]
Razzoli, E.et al.Selective Probing of Hidden Spin-Polarized States in Inversion-Symmetric BulkMoS 2.Phys. Rev. Lett.118, 086402 (2017). URLhttps://link.aps.org/doi/ 10.1103/PhysRevLett.118.086402
-
[41]
Fanciulli, M.et al.Ultrafast Hidden Spin Polarization Dynamics of Bright and Dark Excitons in2H−WSe 2.Phys. Rev. Lett.131, 066402 (2023). URLhttps://link.aps.org/ doi/10.1103/PhysRevLett.131.066402
-
[42]
Beaulieu, S.et al.Revealing Hidden Orbital Pseudospin Texture with Time-Reversal Dichro- ism in Photoelectron Angular Distributions.Phys. Rev. Lett.125, 216404 (2020). URL https://link.aps.org/doi/10.1103/PhysRevLett.125.216404
-
[43]
Sch ¨uler, M.et al.Polarization-Modulated Angle-Resolved Photoemission Spectroscopy: To- ward Circular Dichroism without Circular Photons and Bloch Wave-function Reconstruc- 36 tion.Phys. Rev. X12, 011019 (2022). URLhttps://link.aps.org/doi/10.1103/ PhysRevX.12.011019
2022
-
[44]
J.et al.Valley-selective optical Stark effect in monolayer WS 2.Nature Materials14, 290–294 (2015)
Sie, E. J.et al.Valley-selective optical Stark effect in monolayer WS 2.Nature Materials14, 290–294 (2015). URLhttps://doi.org/10.1038/nmat4156
-
[45]
J.et al.Large, valley-exclusive Bloch-Siegert shift in monolayer WS 2.Sci- ence355, 1066–1069 (2017)
Sie, E. J.et al.Large, valley-exclusive Bloch-Siegert shift in monolayer WS 2.Sci- ence355, 1066–1069 (2017). URLhttps://www.science.org/doi/abs/10. 1126/science.aal2241.https://www.science.org/doi/pdf/10.1126/ science.aal2241
2017
-
[46]
Phys.: Condens
Giannozzi, P.et al.QUANTUM ESPRESSO: a modular and open-source software project for quantum simulations of materials.J. Phys.: Condens. Matter21, 395502 (2009). URL http://stacks.iop.org/0953-8984/21/i=39/a=395502
2009
-
[47]
A.et al.wannier90: A tool for obtaining maximally-localised Wannier func- tions.Computer Physics Communications178, 685–699 (2008)
Mostofi, A. A.et al.wannier90: A tool for obtaining maximally-localised Wannier func- tions.Computer Physics Communications178, 685–699 (2008). URLhttps://www. sciencedirect.com/science/article/pii/S0010465507004936
2008
-
[48]
Girotto Erhardt, N.et al.Ultrafast Nonequilibrium Enhancement of Electron-Phonon Inter- action in2H−MoTe 2.Phys. Rev. Lett.135, 146904 (2025). URLhttps://link.aps. org/doi/10.1103/dvlz-93t8
-
[49]
Commun.13, 4101 (2022)
Zhang, Q.et al.Prolonging valley polarization lifetime through gate-controlled exciton-to- trion conversion in monolayer molybdenum ditelluride.Nat. Commun.13, 4101 (2022). 37
2022
-
[50]
Bertoni, R.et al.Generation and Evolution of Spin-, Valley-, and Layer-Polarized Excited Carriers in Inversion-SymmetricWSe 2.Phys. Rev. Lett.117, 277201 (2016). URLhttps: //link.aps.org/doi/10.1103/PhysRevLett.117.277201
-
[51]
Commun.16, 5799 (2025)
Fragkos, S.et al.Floquet-Bloch valleytronics.Nat. Commun.16, 5799 (2025)
2025
-
[52]
& Queiroz, R
Verma, N. & Queiroz, R. Instantaneous response and quantum geometry of insulators.Pro- ceedings of the National Academy of Sciences122, e2405837122 (2025)
2025
-
[53]
URLhttps://doi.org/10.1038/s41535-025-00801-3
Yu, J.et al.Quantum geometry in quantum materials.npj Quantum Materials10, 101 (2025). URLhttps://doi.org/10.1038/s41535-025-00801-3
-
[54]
Li, Y . & Liu, C.-C. Quantum-Metric-Based Optical Selection Rules.Phys. Rev. Lett.136, 046901 (2026). URLhttps://link.aps.org/doi/10.1103/bdhy-hnd2
-
[55]
& Vishwanath, A
Ahn, J., Guo, G.-Y ., Nagaosa, N. & Vishwanath, A. Riemannian geometry of resonant optical responses.Nature Physics18, 290–295 (2022). URLhttps://doi.org/10.1038/ s41567-021-01465-z
2022
-
[56]
Orenstein, J.et al.Topology and Symmetry of Quantum Materials via Non- linear Optical Responses.Annu. Rev. Condens. Matter Phys.12, 247–272 (2021). URLhttps://www.annualreviews.org/doi/10.1146/ annurev-conmatphys-031218-013712
2021
-
[57]
& Nagaosa, N
Morimoto, T. & Nagaosa, N. Topological nature of nonlinear optical effects in solids.Science Advances2, e1501524 (2016). URLhttps://www.science.org/doi/10.1126/ sciadv.1501524. 38
2016
-
[58]
Nanotechnol.16, 869–873 (2021)
Lai, S.et al.Third-order nonlinear Hall effect induced by the Berry-connection polarizabil- ity tensor.Nat. Nanotechnol.16, 869–873 (2021). URLhttps://www.nature.com/ articles/s41565-021-00917-0
2021
-
[59]
Aversa, C. & Sipe, J. E. Nonlinear optical susceptibilities of semiconductors: Results with a length-gauge analysis.Phys. Rev. B52, 14636–14645 (1995). URLhttps://link.aps. org/doi/10.1103/PhysRevB.52.14636
-
[60]
Sipe, J. E. & Shkrebtii, A. I. Second-order optical response in semiconductors.Phys. Rev. B 61, 5337–5352 (2000). URLhttps://link.aps.org/doi/10.1103/PhysRevB. 61.5337
-
[61]
Zhang, L. & Niu, Q. Chiral Phonons at High-Symmetry Points in Monolayer Hexagonal Lattices.Phys. Rev. Lett.115, 115502 (2015). URLhttps://link.aps.org/doi/ 10.1103/PhysRevLett.115.115502
-
[62]
URLhttps://opg.optica
Cheng, J.et al.Chiral selection rules for multi-photon processes in two-dimensional hon- eycomb materials.Optics Letters44, 2141–2144 (2019). URLhttps://opg.optica. org/ol/abstract.cfm?URI=ol-44-9-2141
2019
-
[63]
URLhttps://doi.org/10.1038/ s41566-025-01823-w
Gucci, F.et al.Encoding and manipulating ultrafast coherent valleytronic information with lightwaves.Nature Photonics20, 266–272 (2026). URLhttps://doi.org/10.1038/ s41566-025-01823-w. 39
2026
-
[64]
Uzan-Narovlansky, A. J.et al.Observation of light-driven band structure via multiband high- harmonic spectroscopy.Nature Photonics16, 428–432 (2022). URLhttps://doi.org/ 10.1038/s41566-022-01010-1
-
[65]
J.et al.Observation of interband Berry phase in laser- driven crystals.Nature626, 66–71 (2024)
Uzan-Narovlansky, A. J.et al.Observation of interband Berry phase in laser- driven crystals.Nature626, 66–71 (2024). URLhttps://doi.org/10.1038/ s41586-023-06828-5
2024
-
[66]
P.et al.An open-source, end-to-end workflow for multidimensional photoemis- sion spectroscopy.Scientific Data7, 442 (2020)
Xian, R. P.et al.An open-source, end-to-end workflow for multidimensional photoemis- sion spectroscopy.Scientific Data7, 442 (2020). URLhttps://doi.org/10.1038/ s41597-020-00769-8
2020
-
[67]
P., Rettig, L
Xian, R. P., Rettig, L. & Ernstorfer, R. Symmetry-guided nonrigid registration: The case for distortion correction in multidimensional photoemission spectroscopy.Ultramicroscopy202, 133 – 139 (2019). URLhttp://www.sciencedirect.com/science/article/ pii/S0304399118303474
2019
-
[68]
& Sentef, M
Sch ¨uler, M. & Sentef, M. A. Theory of subcycle time-resolved photoemission: Application to terahertz photodressing in graphene.Journal of Electron Spectroscopy and Related Phe- nomena253, 147121 (2021). URLhttps://www.sciencedirect.com/science/ article/pii/S0368204821000736. 40
2021
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