Dynamics of a micro-VCSEL operated in the threshold region under low-level optical feedback
Pith reviewed 2026-05-25 13:15 UTC · model grok-4.3
The pith
Correlation functions can characterize optical feedback effects on micro-VCSEL dynamics near threshold and match traditional measurements.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Comparison of time traces, radiofrequency spectra, and correlation functions confirms the ability of correlation functions to satisfactorily characterize the action of feedback on the laser dynamics, with numerical predictions from a previously developed fully stochastic modeling technique providing very close agreement with the experimental observations.
What carries the argument
Correlation functions applied to intensity fluctuations, shown to capture feedback-induced changes equivalently to radiofrequency spectra in the threshold region.
If this is right
- Feedback studies become feasible in the low-coherence, low-power regime between pulsed emission and the accepted threshold.
- Correlation functions become a practical substitute for full time-resolved measurements when characterizing laser dynamics under reinjection.
- The close match between experiment and the stochastic model supports using the same model to predict nanolaser behavior.
Where Pith is reading between the lines
- If correlation functions prove reliable at the nanoscale, feedback control strategies developed on micro-VCSELs could transfer directly to single-emitter devices.
- The same surrogate approach might be tested on other laser types operated near threshold to check whether the correlation-function equivalence holds beyond VCSELs.
Load-bearing premise
The micro-VCSEL under feedback serves as a valid surrogate whose measured dynamics can be extended to nanolasers where only photon statistics are possible.
What would settle it
An experiment on an actual nanolaser in which correlation functions extracted from photon statistics disagree with the feedback signatures predicted by the stochastic model calibrated on the micro-VCSEL.
Figures
read the original abstract
Semiconductor lasers are notoriously sensitive to optical feedback, and their dynamics and coherence can be significantly modified through optical reinjection. We concentrate on the dynamical properties of a very small (i.e., microscale) Vertical Cavity Surface Emitting Laser (VCSEL) operated in the low coherence region between the emission of (partially) coherent pulses and ending below the accepted macroscopic lasing threshold, with the double objective of: 1. studying the feedback influence in a regime of very low energy consumption; 2. using the micro-VCSEL as a surrogate for nanolasers, where measurements can only be based on photon statistics. The experimental investigation is based on time traces and radiofrequency spectra (common for macroscale devices) and correlation functions (required at the nanoscale). Comparison of these results confirms the ability of correlation functions to satisfactorily characterize the action of feedback on the laser dynamics. Numerical predictions obtained from a previously developed, fully stochastic modeling technique provide very close agreement with the experimental observations, thus supporting the possible extension of our observations to the nanoscale.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports experimental measurements on a micro-VCSEL operated near threshold under weak optical feedback, employing time traces, RF spectra, and second-order correlation functions. It compares these data to predictions from a previously developed fully stochastic rate-equation model, finds close agreement, and concludes that correlation functions adequately characterize feedback effects while the model agreement supports possible extension of the findings to nanolasers accessible only via photon statistics.
Significance. The experimental validation of the stochastic model against micro-VCSEL data in the low-coherence regime is a useful result and the use of correlation functions as a diagnostic is well-motivated. Credit is due for the direct comparison between experiment and the fully stochastic model. However, the claimed support for nanoscale extrapolation rests on an untested assumption that the same model remains quantitatively predictive when β approaches unity and Purcell effects dominate; without that demonstration the significance for nanolasers is limited.
major comments (2)
- [Abstract] Abstract (and concluding discussion): the assertion that the micro-VCSEL results and model agreement 'support the possible extension of our observations to the nanoscale' is not accompanied by any scaling analysis, parameter study, or additional simulation showing that the stochastic noise terms and rate equations remain accurate when cavity volume shrinks by orders of magnitude, β→1, or Purcell-enhanced spontaneous emission becomes dominant. Agreement at the micro scale therefore does not automatically license the extrapolation that is presented as the second objective of the work.
- [Model comparison section (inferred from abstract)] The manuscript provides no quantitative assessment of how sensitive the reported agreement is to the specific values of the model parameters (gain, loss, feedback strength, noise amplitudes) taken from the prior work; without this it is difficult to judge whether the 'very close agreement' is robust or could be reproduced by other parameter choices.
minor comments (2)
- [Experimental methods] Additional details on the experimental data processing (e.g., how intensity time traces are converted to g^(2)(τ), binning, normalization, and any statistical uncertainties) would strengthen the claim that correlation functions 'satisfactorily characterize' the feedback action.
- [Results] The abstract states 'very close agreement' between experiment and model; a quantitative metric (e.g., RMS deviation or overlap integral) and the precise parameter values used in the stochastic simulations should be reported.
Simulated Author's Rebuttal
We thank the referee for the constructive and detailed report. We address each major comment below and indicate the revisions that will be incorporated.
read point-by-point responses
-
Referee: [Abstract] Abstract (and concluding discussion): the assertion that the micro-VCSEL results and model agreement 'support the possible extension of our observations to the nanoscale' is not accompanied by any scaling analysis, parameter study, or additional simulation showing that the stochastic noise terms and rate equations remain accurate when cavity volume shrinks by orders of magnitude, β→1, or Purcell-enhanced spontaneous emission becomes dominant. Agreement at the micro scale therefore does not automatically license the extrapolation that is presented as the second objective of the work.
Authors: The manuscript positions the micro-VCSEL experiment as a surrogate for nanolasers precisely because the same fully stochastic rate-equation model (developed in our prior work) is intended to remain applicable when β approaches unity. The quantitative agreement obtained here with unadjusted parameters therefore provides supporting evidence for that modeling framework. We nevertheless agree that an explicit scaling study or Purcell-factor analysis is absent and would overstate the direct support for nanoscale extrapolation. In the revised manuscript we will modify the abstract and concluding discussion to state that the results 'indicate the potential applicability' of the approach to nanolasers rather than claiming that they 'support the possible extension'. revision: yes
-
Referee: [Model comparison section (inferred from abstract)] The manuscript provides no quantitative assessment of how sensitive the reported agreement is to the specific values of the model parameters (gain, loss, feedback strength, noise amplitudes) taken from the prior work; without this it is difficult to judge whether the 'very close agreement' is robust or could be reproduced by other parameter choices.
Authors: All model parameters were taken unchanged from the earlier publication and were not adjusted or fitted to the present data set; the comparison therefore constitutes an a-priori test of the model. The fact that the same fixed parameter set reproduces time traces, RF spectra, and second-order correlation functions simultaneously lends support to the robustness of the agreement. A systematic sensitivity study would certainly be valuable but lies outside the scope of this primarily experimental validation. We will add a short clarifying sentence in the revised text stating that the parameters originate from independent prior work and were not tuned to the current measurements. revision: partial
Circularity Check
Minor self-citation to prior stochastic model; core experimental results independent
full rationale
The paper reports direct experimental measurements (time traces, RF spectra, correlation functions) on a micro-VCSEL under feedback and compares them to predictions from a 'previously developed, fully stochastic modeling technique.' This reference is a self-citation but is not load-bearing: the experimental characterization stands on its own, the model is external to the present dataset, and no quantity is fitted from the current data then relabeled as a prediction. The cautious statement that agreement 'support[s] the possible extension' to nanoscale does not create a self-definitional or fitted-input reduction. No other patterns (ansatz smuggling, uniqueness theorems, renaming) appear.
Axiom & Free-Parameter Ledger
Reference graph
Works this paper leans on
-
[1]
Instability of semiconductor lasers due to optical feedback from distant reflectors,
C. H. Henry and R. Kazarinov, “Instability of semiconductor lasers due to optical feedback from distant reflectors,” IEEE J. Quantum Electron. , vol. QE-22, p. 294, 1986
work page 1986
-
[2]
C. Serrat, S. Prins, and R. Vilaseca, “Dynamics and coherence of a multimode semiconductor laser with optical feedback in an intermediate- length external-cavity regime,” Phys. Rev. A , vol. 68, pp. 053804(1-7), 2003
work page 2003
-
[3]
Dynamics of semiconductor lasers with optical feedback,
J. Ohtsubo, “Dynamics of semiconductor lasers with optical feedback,” Semiconductor Lasers , pp. 113-182, 2017
work page 2017
-
[4]
Optical Spectra of a Semiconductor Laser with Incoherent Optical Feedback,
J.S. Cohen, F. Wittgrefe, Maarten D. Hoogerland, and J.P. Woerdman, “Optical Spectra of a Semiconductor Laser with Incoherent Optical Feedback,” IEEE Journal of Quantum Electronics , vol. 26, pp. 982-990, 1990. 7
work page 1990
-
[5]
Dynamic Regimes in Semiconductor Lasers Subject to Incoherent Optical Feedback,
R. Ju and P.S. Spencer, “Dynamic Regimes in Semiconductor Lasers Subject to Incoherent Optical Feedback,” J. Lightwave Technol., vol. 23 (8), 2513-2523, 2005
work page 2005
-
[6]
External Optical Feedback Phenomena in Semiconduc- tor Lasers
K. Petermann, “External Optical Feedback Phenomena in Semiconduc- tor Lasers”, IEEE J. Sel. Topics Quantum Electron, 1 (2), 480-489 (1995)
work page 1995
-
[7]
Nonlinear Dynamics of Vertical-Cavity Surface-Emitting Lasers,
K. Panajotov, M. Sciamanna, I. Gatare, M. Arteaga, and H. Thienpont, “Nonlinear Dynamics of Vertical-Cavity Surface-Emitting Lasers,” Adv. Opt. Technol., vol. 2011, 1-16, 2011
work page 2011
-
[8]
M. Giudici, S. Balle, T. Ackemann, S. Barland, and J.R. Tredicce, “Polarization dynamics in vertical-cavity surface-emitting lasers with optical feedback: experiment and model,” J. Opt. Soc. Am. B, vol. 16 (11), 2114-2123, 1999
work page 1999
-
[9]
Optical Feedback in Vertical-Cavity Surface-Emitting Lasers,
A. Hsu, J.-F.P. Seurin, S.L. Chuang, and K.D. Choquette, “Optical Feedback in Vertical-Cavity Surface-Emitting Lasers,” IEEE J. Quantum Electron., vol. 37 (12), 1643-1649, 2001
work page 2001
-
[10]
M. Sondermann, H. Bohnet, M. Weinkath, and T. Ackemann, “Dynamics and Polarization Effects in small-area vertical-cavity surface-emitting Lasers in free-running Mode and with time-delayed Feedback,” Proc. SPIE, vol. 4942, 92-102, 2003
work page 2003
-
[11]
Optical feedback induces polarization mode hopping in vertical-cavity surface-emitting lasers,
M. Sciamanna, K Panajotov, H. Thienpont, I. Veretennicoff, P. M ´egret, and M. Blondel, “Optical feedback induces polarization mode hopping in vertical-cavity surface-emitting lasers,” Opt. Lett., vol. 28 (17), 1543- 1545, 2003
work page 2003
-
[12]
VCSEL-Based Interconnects for Current and Future Data Centers,
J.A. Tatum, D.Gazula, L.A. Graham, J.K. Guenter, R.H. Johnson, J. King, Ch. Kocot, G.D. Landry,I. Lyubomirsky, A.N. MacInnes, E.M. Shaw, K. Balemarthy, R. Shubochkin, D. Vaidya, M. Yan, and F. Tang, “VCSEL-Based Interconnects for Current and Future Data Centers,” IEEE J. Lightwave Technol., vol. 33 (4), 727-732, 2015
work page 2015
-
[13]
D.M. Kuchta, A.V . Rylyakov, F.E. Doany, C.L. Schow, J.E. Proesel, Ch.W. Baks, P.Westbergh, J.S. Gustavsson, and A. Larsson, “VCSEL- Based Optical Link,”, IEEE Phot. Technol. Lett., vol 27 (6), 577-580 , 2015
work page 2015
-
[14]
P. Besnard, M.L. Char `es, and G. St´ephan, F. Robert, “Switching between polarized modes of a vertical-cavity surface-emitting laser by isotropic optical feedback,” J. Opt. Soc. Am. B, vol. 16 (7), 1059-1063, 1999
work page 1999
-
[15]
A.V . Naumenko, N.A. Loiko, M. Sondermann, and T. Ackemann, “Description and analysis of low-frequency fluctuations in vertical- cavity surface-emitting lasers with isotropic optical feedback by a distant reflector,” Phys. Rev. A, vol. 68, 033805, 2003
work page 2003
-
[16]
M. Sondermann, H. Bohnet, and T. Ackemann, “Low-frequency fluctua- tions and polarization dynamics in vertical-cavity surface-emitting lasers with isotropic feedback,” Phys. Rev. A, vol. 67, 021802(R), 2003
work page 2003
-
[17]
Optical feedback in Vertical-Cavity Surface-Emitting lasers,
K. Panajotov, M. Sciamanna, M.A. Arteaga, and H. Thienpont, “Optical feedback in Vertical-Cavity Surface-Emitting lasers,” IEEE J.Sel. Topics Quantum Electron., vol. 19, 1700312, 2012
work page 2012
-
[18]
GaInAsP/InP surface emitting injection lasers,
H. Soda, K.-I. Iga, C. Kitahara, and Y . Suematsu, “GaInAsP/InP surface emitting injection lasers,” Jpn. J. Appl. Phys., vol. 18, 2329-2330, 1979
work page 1979
-
[19]
Surface-Emitting LaserIts Birth and Generation of New Opto- electronics Field,
K. Iga, “Surface-Emitting LaserIts Birth and Generation of New Opto- electronics Field,” IEEE J. Sel. Topics Quantum Electron., V ol. 6 (6), 1201-1215, 2000
work page 2000
-
[20]
Demonstration of coherent emission from high-β photonic crystal nanolasers at room temperature,
R. Hostein, R. Braive, L. Le Gratiet, A. Talneau, G. Beaudoin, I. Robert-Philip, I. Sagnes, and A. Beveratos, “Demonstration of coherent emission from high-β photonic crystal nanolasers at room temperature,” Opt. Lett., vol. 35 (8), 1154-1156, 2010
work page 2010
-
[21]
R.-M. Ma. and R.F. Oulton, “Applications of nanolasers,” Nature Nan- otechnology, vol. 14, 12-22, 2019
work page 2019
-
[22]
M. Smit, J.J. van der Tol, M. Hill, “Moore’s law in photonics,” Laser & Photonics Reviews, vol. 6 (1), 1-3, 2012
work page 2012
-
[23]
Large data centers interconnect bottlenecks,
A. Ghiasi, “Large data centers interconnect bottlenecks,” Opt. Express, vol. 23 (3), 2018-2090, 2015
work page 2018
-
[24]
C. Santori, D. Fattal, J. Vukovi, G. S. Solomon, and Y . Yamamoto, Indistinguishable photons from a single-photon device, Nature, vol. 419, 594, 2002
work page 2002
-
[25]
S. Ates, S. M. Ulrich, S. Reitzenstein, A. L ¨offler, A. Forchel, and P. Michler, Post-selected indistinguishable photons from the resonance fluorescence of a single quantum dot in a microcavity, Phys. Rev. Lett., vol. 103, 167402, 2009
work page 2009
- [26]
-
[27]
A. Schlehahn, A. Thoma, P. Munnelly, M. Kamp, S. H ¨ofling, T. Heindel, C. Schneider, and S. Reitzenstein, An electrically driven cavity-enhanced source of indistinguishable photons with 61% overall efficiency, APL Photon., vol. 1, 011301, 2016
work page 2016
-
[28]
Observing chaos for quantum-dot microlasers with external feedback,
F. Albert, C. Hopfmann, S. Reitzenstein, Ch. Schneider, S. H ¨ofling, L. Worschech, M. Kamp, W. Kinzel, A. Forchel, and I. Kanter, “Observing chaos for quantum-dot microlasers with external feedback,” Nature Communications, vol. 2, 336 (1-5), 2011
work page 2011
-
[29]
C. Hopfmann, F. Albert, C. Schneider, S. H ¨ofling, M. Kamp, A. Forchel, I. Kanter, and S. Reitzenstein, “Nonlinear emission characteristics of quantum dotmicropillar lasers in the presence of polarized optical feedback,” New J. Phys. , vol. 15, 025030 (1-17), 2013
work page 2013
-
[30]
Single Photon Delayed Feedback: AWay to Stabilize Intrinsic Quantum Cavity Electrodynamics,
A. Carmele, J. Kabuss, F. Schulze, S. Reitzenstein, and A. Knorr, “Single Photon Delayed Feedback: AWay to Stabilize Intrinsic Quantum Cavity Electrodynamics,” Phys. Rev. Lett. , vol. 110, 013601, 2013
work page 2013
-
[31]
On-chip optoelectronic feedback in a micropillar laser-detector assembly,
P. Munnelly, B. Lingnau, M.M. Karow, T. Heindel, M. Kapp, S. H ¨ofling, K. L ¨udge, Ch. Schneider, and S. Reitzenstein, “On-chip optoelectronic feedback in a micropillar laser-detector assembly,” Optica, vol. 4 (3), 303-306, 2017
work page 2017
-
[32]
S. Holzinger, Ch. Redlich, B. Lingnau, M. Schmidt, M. von Helversen, J. Beyer, Ch. Schneider, M. Kamp, S. H ¨ofling, K. L ¨udge, X. Porte, and S. Reitzenstein, “Tailoring the mode-switching dynamics in quantum- dot micropillar lasers via time-delayed optical feedback,” Opt. Express, vol. 26 (17), 22457-22470, 2018
work page 2018
-
[33]
Determining the linewidth enhancement factor via optical feedback in quantum dot micropillar lasers,
S. Holzinger, S. Kreinberg, B.H. Hokr, Ch. Schneider, S. H ¨ofling, W.W. Chow, X. Porte, and S. Reitzenstein, “Determining the linewidth enhancement factor via optical feedback in quantum dot micropillar lasers,” Opt. Express, vol. 26 (24), 31363-31371, 2018
work page 2018
-
[34]
S. Holzinger, Ch. Schneider, S. H ¨ofling, X. Porte, and S. Reitzenstein, “Quantum-dot micropillar lasers subject to coherent time-delayed optical feedback from a short external cavity,” Sci. Rep., vol. 9, 631 (1-8), 2019
work page 2019
-
[35]
Nonlinear dynamics of Fano lasers with optical feedback,
T.S. Rasmussen and J. Mørk, “Nonlinear dynamics of Fano lasers with optical feedback,” International Symposium on Physics and Applications of Laser Dynamics, 2018
work page 2018
-
[36]
Modes, stability, and small-signal response of photonic crystal Fano lasers,
T.S. Rasmussen, Y . Yu, and J. Mørk, “Modes, stability, and small-signal response of photonic crystal Fano lasers,” Opt. Express, vol. 26 (13), 16365-16376, 2018
work page 2018
-
[37]
Dynamical buildup of lasing in mesoscale devices,
T. Wang, G. P. Puccioni and G. L. Lippi, “Dynamical buildup of lasing in mesoscale devices,” Sci. Rep. , vol. 5, 15858, 2015
work page 2015
-
[38]
Exploration of VCSEL Ultra-low Biasing Scheme for Pulse Generation,
T. Wang, G. Wang, G.P. Puccioni, and G.L. Lippi, “Exploration of VCSEL Ultra-low Biasing Scheme for Pulse Generation,” J. Opt. Soc. Am. B vol. 36 (3), 799-804, 2018
work page 2018
-
[39]
Nonlinear dynamics at the meso- and nanoscale: stochasticity meets determinism,
T. Wang, G.P. Puccioni, and G.L. Lippi, “Nonlinear dynamics at the meso- and nanoscale: stochasticity meets determinism,”, in 2018 IEEE Workshop on Complexity in Engineering (COMPENG), pp. 1-5. IEEE, 2018
work page 2018
-
[40]
Stochastic simulator for modelling the transition to lasing,
G. P. Puccioni, and G. L. Lippi, “Stochastic simulator for modelling the transition to lasing,” Optics Express, vol. 23, 2369-2374, 2015
work page 2015
-
[41]
Threshold dynamics in meso- and nanoscale lasers: why Vertical Cavity Surface Emitting Lasers?,
T. Wang, G.P. Puccioni, G.L. Lippi, “Threshold dynamics in meso- and nanoscale lasers: why Vertical Cavity Surface Emitting Lasers?,” Proc. SPIE, vol. 10682, Semiconductor Lasers and Laser Dynamics VIII, 106820Q (1-14), 2018. Freely available for personal use at: https://sites.google.com/site/gianlucalippi
work page 2018
-
[42]
Manufacturer’sspecifications:https://www.thorlabs.de/drawings/ d6e6bf60a1b18408-F0BC92E1-BA82-C641-BB9776F0E1974E15/ VCSEL-980-MFGSpec.pdf/
-
[43]
S.J. Jiang, Z.Q. Pan, M. Dagenais, R. A. Morgan, and K. Kojima, “Influence of external optical feedback on threshold and spectral char- acteristics of vertical cavity surface emitting lasers,” IEEE photonics technology letters, vol. 6, 34-36, 1994
work page 1994
-
[44]
Dynamics at threshold in mesoscale lasers,
T. Wang, H. Vergnet, G.P. Puccioni, and G.L. Lippi, “Dynamics at threshold in mesoscale lasers,” Phys. Rev. A, vol. 96, 013803, 2017
work page 2017
-
[45]
T. Wang, G. P. Puccioni, and G. L. Lippi, “Onset of Lasing in Small Devices: The identification of the first threshold through autocorrelation resonance,” Ann. Phys. , vol. 530, 1800086(1-7), 2018
work page 2018
-
[46]
How mesoscale lasers can answer fundamental questions related to nanolasers,
T. Wang, G.P. Puccioni, and G.L. Lippi, “How mesoscale lasers can answer fundamental questions related to nanolasers,” Proc. SPIE, vol. 9884, Nanophotonics VI, 98840B (1-20), 2016. Freely available for personal use at: https://sites.google.com/site/gianlucalippi
work page 2016
-
[47]
M. Sondermann and T. Ackemann, “Correlation properties and drift phenomena in the dynamics of vertical-cavity surface-emitting lasers with optical feedback,” Opt. Express, vol. 13 (7), 2707-2715, 2005
work page 2005
-
[48]
Nontrivial photon statistics in small scale lasers,
T. Wang, D. Aktas, O. Alibart, ´E. Picholle, G.P. Puccioni, S. Tanzilli, and G.L. Lippi, “Nontrivial photon statistics in small scale lasers,”, arXiv:1710.02052, 2017
-
[49]
Low-frequency fluctuations in vertical cavity lasers: Experiments versus Lang- Kobayashi dynamics,
A. Torcini, S. Barland, G. Giacomelli, and F. Marin, “Low-frequency fluctuations in vertical cavity lasers: Experiments versus Lang- Kobayashi dynamics,” Phys. Rev. A vol. 74, 063801, 2006
work page 2006
-
[50]
External feedback effects on semiconductor laser properties,
R. Lang and K. Kobayashi, “External feedback effects on semiconductor laser properties,” IEEE J. Quantum Electron. , vol. QE-16, p. 347, 1980. 8
work page 1980
-
[51]
G.L. Lippi, J. Mørk, and G.P. Puccioni, “Numerical solutions to the Laser Rate Equations with noise: technical issues, imple- mentation and pitfalls,” Proc. SPIE, vol. 10672, Nanophotonics VII, 106722B (1-14), 2018. Freely available for personal use at: https://sites.google.com/site/gianlucalippi
work page 2018
-
[52]
Analytical vs. Numerical Langevin Description of Noise in Small Lasers
G.L. Lippi, J. Mørk, and G.P. Puccioni, “Analytical vs. Numerical Langevin Description of Noise in Small Lasers”, arXiv:1903.08859, 2019
work page internal anchor Pith review Pith/arXiv arXiv 1903
-
[53]
Determinis- tic chaos in laser with injected signal,
F.T. Arecchi, G.L. Lippi, G.P. Puccioni, and J.R. Tredicce, “Determinis- tic chaos in laser with injected signal,” Opt. Commun., vol. 51, 308-314, 1985
work page 1985
-
[54]
Instabilities in lasers with an injected signal,
J.R. Tredicce, F.T. Arecchi, G.L. Lippi, and G.P. Puccioni, “Instabilities in lasers with an injected signal,” J. Opt. Soc. Am. B, vol. 2, 173-183, 1985
work page 1985
-
[55]
Zur Quantentheorie der Strahlung,
A. Einstein,“Zur Quantentheorie der Strahlung,” Physikalische Zeitschr., vol. 18, 121-128, 1917. Tao Wang received his Ph.D. degree in physics from the Universit ´e de Nice- Sophia Antipolis, France, in 2016. From 2013 to 2016, he worked in the Institut Non Lin ´eaire de Nice (now the Institut de Physique de Nice) as a PhD student. Since 2016, he was an p...
work page 1917
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.