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arxiv: 2606.17942 · v1 · pith:XKLKDF7Jnew · submitted 2026-06-16 · 📡 eess.SP

On the Optimum Energy-per-bit Launch Power in Coherent Hollow-core Fibre Transmission Systems

Pith reviewed 2026-06-26 22:51 UTC · model grok-4.3

classification 📡 eess.SP
keywords hollow-core fibreenergy per bitlaunch powercoherent transmissionpower consumptionoptical communicationsnonlinear penaltiesC-band
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The pith

A 1000 km C-band hollow-core fibre link reduces total power consumption by 41.5% at the minimum energy-per-bit launch power, with a 2.2% throughput penalty.

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

The paper investigates the launch power that minimizes energy per bit in coherent hollow-core fibre transmission systems. It shows that this optimum point delivers a 41.5% drop in overall power use for a 1000 km C-band link while limiting the throughput loss to 2.2%. The result follows from modeling how launch power trades off against nonlinear impairments and total system energy draw in hollow-core fibre. A reader would care because optical transmission accounts for large fractions of network energy use, and small adjustments in operating point could cut consumption without large capacity hits.

Core claim

In hollow-core fibre systems the energy per bit is minimized at a launch power where the increase in signal strength is balanced against the growth of nonlinear penalties. Operating a 1000 km C-band link at this point produces a 41.5% reduction in total power consumption accompanied by only a 2.2% reduction in throughput.

What carries the argument

The energy-per-bit quantity obtained from the link power-consumption model that includes launch power, amplifier consumption, and nonlinear penalties specific to hollow-core fibre.

If this is right

  • Total power consumption falls by 41.5% while throughput falls by only 2.2%.
  • The same minimum-energy-per-bit operating point applies to C-band coherent links over hollow-core fibre.
  • Nonlinear penalties set the location of the energy-per-bit minimum rather than linear loss alone.
  • Power savings scale with distance because the nonlinear contribution grows with length.

Where Pith is reading between the lines

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

  • Operators could reduce electricity cost and heat load by deliberately detuning launch power away from the usual maximum-capacity point.
  • The result may shift the economic case for replacing standard fibre with hollow-core spans in power-sensitive routes.
  • Further gains are possible if the same energy-per-bit minimization is combined with adaptive modulation or sleep-mode amplifiers.

Load-bearing premise

The link model used to compute energy-per-bit and throughput accurately captures all relevant power-consuming components and nonlinear penalties for hollow-core fibre at the stated distances and wavelengths.

What would settle it

Direct measurement of total electrical power draw and net throughput on a real 1000 km hollow-core fibre span when the launch power is set to the calculated minimum-energy-per-bit value.

Figures

Figures reproduced from arXiv: 2606.17942 by Eric Sillekens, Mindaugas Jarmolovicius, Polina Bayvel, Robert I. Killey, Ronit Sohanpal.

Figure 1
Figure 1. Figure 1: Dispersion and attenuation profile based on simulated 1st window DNANF HCF from [6, 7]. arXiv:2606.17942v1 [eess.SP] 16 Jun 2026 [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: C-band throughput versus total launch power for 1x200 km HCF and 3x67 km low-loss SMF (200 km total). We investigated UWB transmission across the O-band (1265 nm-1355 nm), E-band (1400 nm￾1460 nm), S-band (1470 nm-1520 nm), C-band (1530 nm-1565 nm) and L-band (1570 nm￾1620 nm) for 105, 59, 63, 29 and 32 channels respectively, shown in [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Energy-per-bit versus throughput for 200 km C-band transmission and increasing per-channel launch power (solid lines) for (a) SMF and (b) HCF. Insets indicate the minimum energy-per-bit (diamond) and maximum throughput (square) [PITH_FULL_IMAGE:figures/full_fig_p002_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Total energy per bit versus throughput for the C-, CL-, SCL-, ESCL- and OESCL-bands for increasing launch power for 5x200 km HCF (1000 km total). Markers indicate minimum energy per bit Emin b and maximum throughput T max tot . Energy per bit results Using the aforementioned model in the C-band, the total throughput versus power per channel is shown in [PITH_FULL_IMAGE:figures/full_fig_p003_4.png] view at source ↗
read the original abstract

We investigate the optimum energy per bit in hollow-core-fibre transmission systems. We show that a 1000 km C-band link can achieve a 41.5% reduction in total power consumption when operating at the minimum energy-per-bit launch power with only 2.2% throughput penalty.

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

2 major / 0 minor

Summary. The manuscript investigates the optimum energy-per-bit launch power in coherent hollow-core fibre (HC-PCF) transmission systems. It claims that a 1000 km C-band link achieves a 41.5% reduction in total power consumption when operated at the minimum energy-per-bit launch power, incurring only a 2.2% throughput penalty.

Significance. If the underlying power-consumption model and hollow-core-fibre nonlinear interference term are accurate and complete, the result would be significant for energy-efficient long-haul system design, as it identifies a practical operating point that trades minimal rate for substantial power savings in a technology with intrinsically lower nonlinearity.

major comments (2)
  1. The 41.5% power-reduction and 2.2% throughput-penalty figures are obtained by minimising total electrical power divided by throughput. No explicit model is supplied that enumerates every power-consuming block (transmitter, receiver, DSP, each EDFA stage) or that specifies the nonlinear interference coefficient and loss profile used for HC-PCF; without these, the location of the minimum and the reported percentages cannot be reproduced or stress-tested.
  2. The abstract states the result for a 1000 km C-band link but provides neither the capacity formula employed to convert SNR to achievable rate nor any validation against measured HC-fibre parameters at the stated wavelengths and distances; this renders the headline numbers unverifiable from the given material.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their comments on our manuscript. We provide point-by-point responses below, agreeing where additional detail is needed for reproducibility and indicating the corresponding revisions.

read point-by-point responses
  1. Referee: The 41.5% power-reduction and 2.2% throughput-penalty figures are obtained by minimising total electrical power divided by throughput. No explicit model is supplied that enumerates every power-consuming block (transmitter, receiver, DSP, each EDFA stage) or that specifies the nonlinear interference coefficient and loss profile used for HC-PCF; without these, the location of the minimum and the reported percentages cannot be reproduced or stress-tested.

    Authors: We agree that an explicit enumeration of all power-consuming blocks and the precise values of the nonlinear interference coefficient and loss profile for HC-PCF are required for full reproducibility. The revised manuscript will include a complete breakdown of the power model together with the exact coefficient and loss values employed. revision: yes

  2. Referee: The abstract states the result for a 1000 km C-band link but provides neither the capacity formula employed to convert SNR to achievable rate nor any validation against measured HC-fibre parameters at the stated wavelengths and distances; this renders the headline numbers unverifiable from the given material.

    Authors: The capacity formula is the standard Shannon formula applied to the SNR after nonlinear interference, and the fibre parameters are taken from published HC-PCF measurements. The revised manuscript will state the capacity formula explicitly and cite the specific measured parameters used for the C-band wavelengths and distances considered. revision: yes

Circularity Check

0 steps flagged

No circularity detected; derivation chain not visible in supplied text

full rationale

The abstract states a 41.5% power reduction at minimum energy-per-bit launch power but supplies no equations, fitting procedures, or self-citations. The reader's summary explicitly notes that no equations or fitting are visible, preventing any inspection for self-definitional, fitted-input, or self-citation circularity. Without load-bearing steps that reduce to inputs by construction, the result cannot be flagged as circular. The model is treated as an external computation whose completeness is a separate modeling question, not a circularity issue.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review; no equations, parameters, or assumptions are stated, so the ledger cannot be populated beyond noting that the central numerical claims rest on an unstated link model.

pith-pipeline@v0.9.1-grok · 5584 in / 993 out tokens · 21148 ms · 2026-06-26T22:51:42.342288+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

14 extracted references · 6 canonical work pages

  1. [1]

    Opportunities and Chal- lenges for Long-Distance Transmission in Hollow-Core Fibres

    P . Poggiolini and F . Poletti, “Opportunities and Chal- lenges for Long-Distance Transmission in Hollow-Core Fibres”,Journal of Lightwave Technology, vol. 40, no. 6, pp. 1605–1616, Mar. 2022.DOI: 10.1109/JLT.2021. 3140114

  2. [2]

    The Potential for Span Length Increase with NANF

    P . Poggiolini, G. Bosco, Y . Jiang, and F . Poletti, “The Potential for Span Length Increase with NANF”, in2023 IEEE Photonics Conference (IPC), Nov. 2023, pp. 1–2. DOI:10.1109/IPC57732.2023.10360569

  3. [3]

    On High-Power Optical Amplification in Hollow Core Fibers for Energy Efficiency and Network Throughput Maximization

    G. Sticca, M. Ibrahimi, N. Di Cicco, F . Musumeci, and M. Tornatore, “On High-Power Optical Amplification in Hollow Core Fibers for Energy Efficiency and Network Throughput Maximization”, inECOC 2024; 50th Euro- pean Conference on Optical Communication, Sep. 2024, pp. 1010–1013

  4. [4]

    Challenges and Breakthroughs in Modeling and Designing Ultrawideband Optical Fibre Communication Systems and Networks

    J. Y ang, M. Jarmoloviˇcius, Z. Gan, H. Buglia, R. So- hanpal, R. Aparecido, E. Sillekens, R. I. Killey, and P . Bayvel, “Challenges and Breakthroughs in Modeling and Designing Ultrawideband Optical Fibre Communication Systems and Networks”,Journal of Lightwave Tech- nology, vol. 44, no. 3, pp. 944–954, Feb. 2026.DOI: 10.1109/JLT.2025.3640009

  5. [5]

    450 Tb/s GMI, 42.4 THz, OESCL- Band Transmission Over a Field-Deployed Fiber

    R. S. Luis, J. Y ang, R. Aparecido, M. Jarmoloviˇcius, E. Sillekens, R. Sohanpal, Z. Gan, A. Donodin, V. Mikhailov, J. Luo, D. DiGiovanni, N. Fontaine, L. Dallachiesa, M. Mazur, R. Ryf, H. Chen, D. Neilson, I. D. Phillips, W. Forysiak, S. K. Turitsyn, D. Orsuti, H. Furukawa, R. I. Killey, and P . Bayvel, “450 Tb/s GMI, 42.4 THz, OESCL- Band Transmission O...

  6. [6]

    Broadband optical fibre with an attenuation lower than 0.1 decibel per kilometre

    M. Petrovich, E. Numkam Fokoua, Y . Chen, H. Sakr, A. I. Adamu, R. Hassan, D. Wu, R. Fatobene Ando, A. Papadimopoulos, S. R. Sandoghchi, G. Jasion, and F . Poletti, “Broadband optical fibre with an attenuation lower than 0.1 decibel per kilometre”,Nature Photonics, vol. 19, no. 11, pp. 1203–1208, Nov. 2025.DOI: 10 . 1038/s41566-025-01747-5

  7. [7]

    First Dual-Band Hybrid Window Antiresonant HCF with 0.13 dB/km loss at 1 µm and 0.11 dB/km at 1.55 µm

    G. A. Mahdiraji, S. M. A. Mousavi, D. Wu, T. Varghese, N. K. Baddela, K. Wisniowski, S. B. Gorajoobi, A. Shak- iba, M. Rahman, G. Guerra, E. N. Fokoua, Y . Chen, G. Jasion, and F . Poletti, “First Dual-Band Hybrid Window Antiresonant HCF with 0.13 dB/km loss at 1 µm and 0.11 dB/km at 1.55 µm”, inOptical Fiber Communication Conference (OFC), Th4B.8, 2026

  8. [8]

    CO2 Elim- ination in Hollow-Core Fibre via Post-Processing

    R. Sohanpal, J. Y ang, E. Sillekens, H. Buglia, M. Tan, D. Pratiwi, R. I. Killey, and P . Bayvel, “Measurement and Analysis of the Power Consumption of Hybrid-Amplified SCL-Band Links”, in2025 European Conference on Optical Communications (ECOC), Sep. 2025, pp. 1–4. DOI:10.1109/ECOC66593.2025.11263434

  9. [9]

    Ultra-Wideband Transmission Systems From an En- ergy Perspective: Which Band is Next?

    R. Sohanpal, M. Jarmolovi ˇcius, J. Y ang, E. Sillekens, R. Aparecido, V. Mikhailov, J. Luo, D. J. DiGiovanni, R. S. Luis, H. Furukawa, R. I. Killey, and P . Bayvel, “Ultra-Wideband Transmission Systems From an En- ergy Perspective: Which Band is Next?”, inOptical Fiber Communication Conference (OFC), M3C.3, 2026

  10. [10]

    222-km-long Hybrid Span Transmission Systems made of Support Tube Hollow Core Fiber and of Standard Single Mode Fiber using High Power Doped Fiber Amplifier

    H. Mardoyan, R. S. B. Ospina, C. C. Carrero, A. Ghazisaeidi, R. Boddeda, P . Li, L. Zhang, J. Luo, C. Fu, C. Hu, and J. Renaudier, “222-km-long Hybrid Span Transmission Systems made of Support Tube Hollow Core Fiber and of Standard Single Mode Fiber using High Power Doped Fiber Amplifier”,Optical Fiber Com- munication Conference, 2026

  11. [11]

    Trans- mitter Power Optimization for Uniform Performance Multi- Span Hollow-Core Fiber Transmission

    Y . Hong, M. Kamalian-Kopae, A. Ali, B. Gholizadeh, S. Bawn, J. Hooley, S. B. Gorajoobi, C. Wallace, J. Gaudette, D. J. Richardson, and B. J. Puttnam, “Trans- mitter Power Optimization for Uniform Performance Multi- Span Hollow-Core Fiber Transmission”,Optical Fiber Communication Conference, 2026

  12. [12]

    CO2 Elim- ination in Hollow-Core Fibre via Post-Processing

    Y . Xiong, R. Zhao, D. Ge, S. Gao, Y . Sun, D. Wang, D. Zhang, H. Li, W. Ding, and Y . Wang, “CO2 Elim- ination in Hollow-Core Fibre via Post-Processing”, in 2025 European Conference on Optical Communica- tions (ECOC), W.02.01.08, Sep. 2025, pp. 1–4.DOI: 10.1109/ECOC66593.2025.11263127

  13. [13]

    Leveraging Digital Subcarrier Multiplexing for Long-Haul Transmission over HCFs in the Presence of IMI

    R. S. B. Ospina, C. C. Carrero, H. Mardoyan, A. Ghazisaeidi, R. Boddeda, P . Li, L. Zhang, J. Luo, and J. Renaudier, “Leveraging Digital Subcarrier Multiplexing for Long-Haul Transmission over HCFs in the Presence of IMI”,Optical Fiber Communication Conference, 2026, Th1J.3

  14. [14]

    Repeater Power Conversion Efficiency in Submarine Optical Com- munication Systems

    X. Liang, J. D. Downie, and J. E. Hurley, “Repeater Power Conversion Efficiency in Submarine Optical Com- munication Systems”,IEEE Photonics Journal, vol. 13, no. 1, pp. 1–10, Feb. 2021.DOI: 10.1109/JPHOT.2021. 3054624