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REVIEW 4 major objections 4 minor 217 references

Transport resistance dominates the fill factor losses in record organic solar cells

T0 review · 4 major / 4 minor · reviewed 2026-08-11 · deepseek-v4-flash

Pith's one-line read This paper argues that transport resistance, not recombination, is the main remaining fill-factor loss in state-of-the-art organic solar cells.

desk verdict A useful, well-argued perspective whose central claim—transport resistance dominates FF loss in record OSCs—is plausible but rests on a Green-equation baseline that the paper's own Section 8 undermines; conditional on data release and direct validation. read the letter →

arxiv 2412.13694 v1 pith:Z2K7PWKN submitted 2024-12-18 cond-mat.mtrl-sci

classification cond-mat.mtrl-sci
keywords organicphotovoltaicstransportresistancefillfactorpseudo-fillnon-fullereneacceptorschargecarriermobilitysuns-Voccollectionlosses
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

This paper argues that the main remaining fill-factor loss in high-efficiency organic solar cells is not recombination but transport resistance: the voltage- and light-dependent cost of extracting charge carriers through a low-mobility absorber. Using the empirical Green equation with reported recombination ideality factors, the authors estimate pseudo-fill factors for 390 devices from 125 publications and find that the gap between measured fill factor and pseudo-fill factor is dominated by transport resistance even in fresh record cells. For a certified 19.1% cell the pseudo-fill factor is 87.4% against a measured fill factor of 79.6%, a 7.8-percentage-point loss attributed to transport resistance. If the claim holds, raising charge-carrier conductivity and balancing electron and hole mobilities should yield substantial efficiency gains, with one highlighted record system predicted to rise from 20.2% to about 22%.

What carries the argument

The load-bearing object is the pair $(FF, pFF)$ connected by the empirical Green equation $FF = (v_{\mathrm{oc}} - \ln(v_{\mathrm{oc}} + 0.72))/(v_{\mathrm{oc}} + 1)$ with $v_{\mathrm{oc}} = eV_{\mathrm{oc}}/(n_{\mathrm{app}} k_B T)$. Entering the measured recombination ideality factor $n_{\mathrm{id}}$ predicts the pseudo-fill factor $pFF$, the fill factor the device would have without transport resistance; entering the apparent ideality factor $n_{\mathrm{app}} = n_{\mathrm{id}} + \alpha$, or its refined form $n_{\mathrm{id}} + \beta$, predicts the real fill factor. The transport resistance itself is defined as $R_{\mathrm{tr}} = d/\sigma$, the active-layer thickness divided by the effective conductivity, causing a voltage drop $\Delta V_{\mathrm{tr}} = J R_{\mathrm{tr}}$; the figure of merit $\alpha$ relates to $J_{\mathrm{gen}}/\sigma_{\mathrm{oc}}$ and to thickness and mobility. The difference $pFF - FF$ is the paper's quantitative measure of transport-resistance loss.

What would settle it

Take a set of fresh high-efficiency non-fullerene cells and, for each, construct the transport-free $J(V_{\mathrm{imp}})$ curve directly from suns-$V_{\mathrm{oc}}$ data; compare the $pFF$ from that curve with the $pFF$ from the Green equation using the reported $n_{\mathrm{id}}$. If the two disagree systematically, or if the difference $pFF - FF$ can be reproduced by simulating field-dependent photogeneration and recombination with injected carriers alone, the attribution of the whole gap to transport resistance would be overturned.

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Extended reading notes

Core claim

The central claim is that transport resistance dominates the fill-factor and power-conversion-efficiency losses in the vast majority of non-fullerene-based organic solar cells, including the most efficient reported devices. The paper defines transport resistance as an internal, voltage- and light-intensity-dependent resistance $R_{\mathrm{tr}} = d/\sigma$ arising from finite charge-carrier conductivity in the active layer, and quantifies the fill-factor loss as the difference between the measured fill factor $FF$ and the pseudo-fill factor $pFF$ computed from the Green equation with the experimentally determined recombination ideality factor $n_{\mathrm{id}}$. On a dataset of 390 devices, $pFF - FF$ correlates with power conversion efficiency, and after excluding fullerene-based systems and cells with $n_{\mathrm{id}} \ge 1.5$, transport resistance accounts for most of the remaining loss. Even in a certified 19.1% binary cell the estimated loss is 7.8 percentage points; in a 20.2% record system the paper estimates that eliminating transport resistance would raise efficiency to about 22%.

Load-bearing premise

The whole quantification rests on the assumption that the pseudo-fill factor obtained by putting the measured recombination ideality factor $n_{\mathrm{id}}$ into the Green equation is exactly the fill factor the device would have without transport resistance, so that $pFF - FF$ cleanly isolates transport loss.

Editorial extensions

If this is right

  • Even fresh record cells lose fill factor to transport resistance: the certified 19.1% cell has an estimated $pFF$ of 87.4% versus a measured $FF$ of 79.6%, a gap of 7.8 percentage points.
  • Across 390 devices from 125 publications, transport resistance, not recombination, is the dominant fill-factor and efficiency loss in most non-fullerene organic solar cells once fullerene systems and cells with $n_{\mathrm{id}} \ge 1.5$ are excluded.
  • If transport resistance were removed from the 20.2% record system D18:Z8:L8-BO, its power conversion efficiency could rise to about 22%.
  • Increasing active-layer thickness from 100 nm to 500 nm roughly doubles or triples the transport-resistance loss, so scalable printing will need ternary blends, layer-by-layer deposition, or higher-mobility materials.
  • The refined ideality factor $\beta$ lets the Green equation reproduce measured fill factors across material systems, temperatures, and light intensities, giving a simple way to predict fill factor from $n_{\mathrm{id}}$, $\alpha$, and the transport ideality factor $n_{\sigma}$.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • If transport resistance is as large as this paper argues, then efforts to reduce non-radiative recombination losses at open-circuit are hitting a ceiling that only mobility and conductivity engineering can lift; the next several percentage points of efficiency are likely to come from charge transport, not from further $V_{\mathrm{oc}}$ gains.
  • The Green-equation shortcut could be tested directly on a fresh record cell by constructing $J(V_{\mathrm{imp}})$ from suns-$V_{\mathrm{oc}}$ data and comparing the resulting $pFF$ with the Green-equation prediction; disagreement would reveal recombination-related fill-factor losses misattributed to transport resistance.
  • Because the photoshunt product $R_{\mathrm{photo}}\Phi$ predicts fill factor across temperature and intensity, it could serve as a fast inline screening metric for transport-resistance losses in roll-to-roll module production, where full current-voltage analysis is impractical.
  • The paper's thickness scaling suggests a quantitative target: for a given generation current and recombination prefactor, an effective mobility above roughly $10^{-3}\,\mathrm{cm^2/Vs}$ keeps $\alpha$ below 1 in a 100 nm layer, so material discovery programmes can screen candidates against this threshold.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

4 major / 4 minor

Summary. This Perspective argues that transport resistance, rather than recombination alone, dominates the fill-factor and efficiency losses in state-of-the-art organic solar cells. The paper combines a literature meta-analysis of 390 devices from 125 publications, an analytical framework connecting continuity and diode models through a voltage- and intensity-dependent transport resistance, a practical protocol for extracting transport resistance from suns-Voc and illuminated JV data, and a discussion of figures of merit, alternative viewpoints, and mitigation strategies. The headline quantitative claims are that a certified 19.1% cell loses about 7.8 percentage points of fill factor to transport resistance (pFF 87.4% vs. FF 79.6%), and that transport resistance is the dominant FF/PCE loss in most non-fullerene devices. The theoretical sections are coherent and the experimental protocol is plausible, but the central meta-analytic claim rests on an unpublished dataset and on an approximation whose validity as a transport-free baseline is not demonstrated.

Significance. If the central claim is correct, it refocuses the OPV loss discussion from non-radiative voltage losses toward charge transport and has direct implications for material design, active-layer thickness, and processing choices. The paper provides a valuable service by unifying the transport-resistance terminology, presenting explicit equations connecting the continuity and diode models, and giving step-by-step instructions for quantifying transport resistance. The drift-diffusion simulations in Sections 3 and 8 illustrate the concept in a concrete way. However, the quantitative meta-analysis that carries the strongest claim is not reproducible from the manuscript: no per-device dataset is supplied, no error bars are propagated, and the Green-equation pFF is used without validation against the J(Vimp) reconstruction that the same paper recommends. These issues make the central quantitative statement premature, although the qualitative concept is well grounded.

major comments (4)
  1. [Section 2, Eq. (1)] The meta-analysis computes pFF from the empirical Green equation using reported nid values, then attributes pFF - FF entirely to transport resistance. This identification requires that the Green equation with the suns-Voc ideality factor equals the FF the device would have in the absence of transport resistance. The paper does not validate this equivalence for the surveyed devices, nor does it provide the underlying dataset or uncertainty propagation. Please make the 390-device data and code available, report per-device pFF values, and benchmark Eq. (1) against the J(Vimp) reconstruction of Section 5 for at least a representative subset.
  2. [Figure 2(c)] The post-hoc filtering that excludes fullerene devices and devices with nid >= 1.5 is introduced with the statement that it 'effectively filter most outliers'. Because the conclusion 'transport resistance dominates the FF and PCE loss in the vast majority of non-fullerene-based OSC devices' is derived only from the filtered subset, the filter must be justified more rigorously. Show the unfiltered analysis, report the number of excluded devices, and discuss whether the conclusion survives without this selection.
  3. [Section 8] The paper itself identifies two additional fill-factor loss mechanisms, field-dependent photogeneration and recombination with injected charge carriers, that 'have a similar appearance as the transport resistance, but have to be considered separately' and are independent of light intensity. A suns-Voc-derived nid captures recombination only at zero current and cannot detect these mechanisms. Therefore pFF - FF as computed in Section 2 may overstate transport resistance. Please quantify the possible contribution of these mechanisms to the 7.8 percentage-point gap for the 19.1% cell, or explicitly present the attributed transport loss as an upper bound.
  4. [Section 5, Eq. (21)] The J(Vimp) reconstruction described in Section 5 is the proper transport-free baseline, but the meta-analysis uses the Green-equation approximation instead. The paper says the Green equation can be used as an approximation, but no evidence is given that this approximation is accurate for modern non-fullerene devices. A comparison of pFF from Eq. (1) and from the J(Vimp) reconstruction on the same devices would be a decisive test and should be included.
minor comments (4)
  1. [Section 3 and Section 7] Several cross-references are duplicated, e.g. 'section 77.1' and 'section 88.1'; these should be corrected throughout.
  2. [Figure 7(b)] The caption refers to 'the analytical expression (Equation (4))', but the relevant expression appears to be Equation (1) or (23); please verify the equation number.
  3. [Figure 2(c)] The grey dashed line is described as showing a correlation, but no fit function, correlation coefficient, or confidence band is reported. Please provide the numerical fit parameters or remove the line.
  4. [Abstract and Introduction] The text says 'even the highest efficiency organic solar cells reported to-date', but the specific example is a certified 19.1% binary cell, not the overall record; the wording should be more precise to avoid overstatement.

Circularity Check

0 steps flagged · score 2.0 of 10

No reduction-to-input circularity: pFF-FF is an empirical Green-equation estimate with independent drift-diffusion support, but the meta-analysis leans on the authors' prior validation of the Green-equation framework.

full rationale

The central metric pFF-FF is not fitted to the measured FF. In Section 2 the paper computes pFF by inserting the independently measured suns-Voc ideality factor nid into the empirical Green equation (Eq. 1), an external benchmark from Green 1982. This is a model-based counterfactual, not a fitted parameter renamed as a prediction. Section 5 provides a direct construction of J(Vimp) from suns-Voc data as an alternative transport-free baseline, and Section 3's drift-diffusion simulations independently show that increasing mobility (removing transport resistance) raises FF toward the recombination-limited curve. The reliance on the authors' own refs 9 and 143 to state that the Green equation 'was confirmed to hold' for organic cells when the ideality factor is adapted for transport is a self-citation, but it is not load-bearing circularity: the Green equation has independent standing, and the cited framework is externally falsifiable through the J(Vimp) method and through simulation. The paper's own Section 8 noting that field-dependent photogeneration and injection-induced recombination 'have a similar appearance as the transport resistance, but have to be considered separately' is a limitation on the attribution of pFF-FF to transport, but it is a correctness risk, not a circularity, since pFF is not defined in terms of FF or of those mechanisms. No equation in the paper reduces by construction to its own input.

Assumptions & free parameters 2 free parameters · 3 assumptions · 0 invented entities

The central claim rests on the empirical Green equation, the reported nid values from 125 papers, and the assumption that pFF computed with nid isolates transport losses. No new material entities are introduced. The framework is based on standard drift-diffusion and diode models.

free parameters (2)
  • Green equation empirical constants = FF = (voc - ln(voc + 0.72)) / (voc + 1)
    The pseudo-fill factor used to define transport loss is computed with this empirical formula. The constants 0.72 and the functional form are fitted to ideal-diode JV curves in the prior literature and are not derived in this paper. The central pFF-FF estimate depends on them.
  • Section 8 CT dissociation simulation parameters = Vbi = 1.16 V, Voc = 0.85 V, d = 100 nm, nid = 1, r = 1 nm, CT lifetime = 2.5 ns
    Hand-picked typical values used to argue that field-dependent photogeneration has a minor impact on fill factor relative to transport resistance. The conclusion that transport dominates CT dissociation is conditional on these choices, though the paper notes they are typical.
assumptions (3)
  • domain assumption The Green equation with the recombination ideality factor nid yields the fill factor the device would have in the absence of transport resistance.
    This is the load-bearing link between measured FF and transport loss. It is stated in Section 2 and supported mainly by the authors' prior work (refs 9 and 143), not by a per-device verification across the 390 surveyed cells.
  • domain assumption The recombination ideality factor nid reported in the surveyed publications is measured from suns-Voc and is an accurate description of the recombination losses entering the Green equation.
    The meta-analysis pools nid values from 125 papers without re-analysis. Publication and measurement inconsistencies across labs could bias the pFF estimates.
  • standard math Standard drift-diffusion and diode models, including the relation J = (sigma/e) grad EF (Eq. 7), accurately describe charge transport in the organic solar cells discussed.
    The theoretical sections rest on the continuity equation, QFL gradients, and diode models, which are standard device physics. These are not in question for this review.

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Cite this review

Pith. "Pith review of Transport resistance dominates the fill factor losses in record organic solar cells." pith.science (2026). https://pith.science/paper/Z2K7PWKN

@misc{pith2026241213694,
  author       = {Pith},
  title        = {Pith review of: Transport resistance dominates the fill factor losses in record organic solar cells},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/Z2K7PWKN}},
  note         = {Machine review of arXiv:2412.13694}
}
read the original abstract

Organic photovoltaics are a promising solar cell technology well-suited to mass production using roll-to-roll processes. The efficiency of lab-scale solar cells has exceeded 20% and considerable attention is currently being given to understanding and minimising the remaining loss mechanisms preventing higher efficiencies. While recent efficiency improvements are partly owed to reducing non-radiative recombination losses at open-circuit, the low fill factor due to a significant transport resistance is becoming the Achilles heel of organic photovoltaics. The term transport resistance refers to a voltage and light intensity dependent charge collection loss in low-mobility materials. In this Perspective, we demonstrate that even the highest efficiency organic solar cells reported to-date have significant performance losses that can be attributed to transport resistance and that lead to high fill factor losses. We provide a closer look at the transport resistance and the material properties influencing it. We describe how to experimentally characterise and quantify the transport resistance by providing easy to follow instructions. Furthermore, the causes and theory behind transport resistance are detailed. In particular, we integrate the relevant figures of merit and different viewpoints on the transport resistance. Finally, we outline strategies that can be followed to minimise these charge collection losses in future solar cells.

Figures

Figures reproduced from arXiv: 2412.13694 by the authors.

Figure 1
Figure 1. Current–voltage characteristics of a solar cell [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. (a) Parameters nid, Jsc, and Voc of various organic solar cells plotted as a function of their respective PCE. (b) Different types of fill factor versus PCE of solar cells, the cityscape line represents the binning of assembled data. (c) Estimated transport resistance loss versus PCE, the grey dashed line shows the correlation. (d) Comparison of pFF and FF in OSCs (PCE > 19%) based on different donor–acceptor blends… view at source ↗
Figure 3
Figure 3. FF loss due to transport resistance for solar cells grouped by: (a) active layer thickness, with devices using binary (circles) and ternary (stars) BHJ or LBL-deposited (triangles) active layers. PCE is indicated for reference; (b) active layers processed from halogenated vs. non-halogenated solvents (left of the dashed line), and spin-coated vs. non-spin-coated active layers (right of the dashed line). non-spin-coa… view at source ↗
Figures from the paper (10 more)
Figure 4
Figure 4. Figure 4: Drift–diffusion simulation based on a 200 nm thick PM6:Y6 solar cell. [PITH_FULL_IMAGE:figures/full_fig_p006_4.png]
Figure 5
Figure 5. Figure 5: JV curves of solar cells with high and low mobility, calculated using Equation (9). The schematic energy-level diagrams show that: at open-circuit, Vext = Vimp, and the QFLs are flat; at short-circuit, low mobility leads to a larger QFL gradient and difference between …
Figure 6
Figure 6. Figure 6: Experimental data for transport resistance evaluation with details given in the text. (a) [PITH_FULL_IMAGE:figures/full_fig_p011_6.png]
Figure 7
Figure 7. Figure 7: (a) Current–voltage curves calculated using Equation (23). The generation current is kept constant, while [PITH_FULL_IMAGE:figures/full_fig_p014_7.png]
Figure 8
Figure 8. Figure 8: (a) The fill factor of PM6:Y6 shows a good correlation to the FoM [PITH_FULL_IMAGE:figures/full_fig_p015_8.png]
Figure 9
Figure 9. Figure 9: (a) Shifted JV curves of the PM6:Y6 solar cell at 300 K. The near-ohmic current at low forward bias increases significantly with light intensity Φ, indicating an apparent light-intensity-dependent parallel resistance. (b) Photoshunt Rphoto and total parallel resistance…
Figure 10
Figure 10. Figure 10: Depending on the electrostatics of the device geometry, charge-transport losses can have different effects [PITH_FULL_IMAGE:figures/full_fig_p019_10.png]
Figure 11
Figure 11. Figure 11: Influence of charge photogeneration on the [PITH_FULL_IMAGE:figures/full_fig_p021_11.png]
Figure 12
Figure 12. Figure 12: The impact of recombination with injected charge carriers [PITH_FULL_IMAGE:figures/full_fig_p022_12.png]
Figure 13
Figure 13. Figure 13: Spatial distribution of the recombination rate at [PITH_FULL_IMAGE:figures/full_fig_p023_13.png]

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