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REVIEW 2 major objections 4 minor 27 references

Site selective synthesis of in situ Ni filled multiwalled carbon nanotubes using Ni(salen) as a catalyst source

T0 review · 2 major / 4 minor · reviewed 2026-08-14 · deepseek-v4-flash

Pith's one-line read This paper reports that a photoresist loaded with Ni(salen) can be patterned by ordinary lithography and, in a single atmospheric-pressure CVD step, grow nickel-filled multiwalled carbon nanotubes only on the patterned regions.

desk verdict The Ni(salen)/photoresist route to site-selective Ni-filled CNT growth is a real, modest synthesis advance, but the coercivity claim is oversold by one unsubtracted SQUID curve on the whole as-grown film. read the letter →

arxiv 1908.04516 v1 pith:UVQY63HA submitted 2019-08-13 physics.app-ph cond-mat.mtrl-sci

classification physics.app-phcond-mat.mtrl-sci
keywords Ni-filledcarbonnanotubesNi(salen)modifiedphotoresistsite-selectivegrowthchemicalvapordepositionphotolithographyferromagneticinsitufilling
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

The paper reports a single-step, photolithographic route to nickel-filled multiwalled carbon nanotubes. It mixes the nickel complex Ni(salen) into a conventional photoresist, patterns the mixture by ordinary exposure and development, and then grows the tubes by atmospheric-pressure chemical vapor deposition with propane at 850 °C. The authors claim the tubes grow by a tip-growth mechanism, are partially filled with nickel nanowires during growth, are well graphitized (Raman $I_D/I_G = 0.32$), and are ferromagnetic with a coercivity of 94 Oe at 5 K. The reason a reader would care is that the approach removes a separate metal-filling step and places filled magnetic nanotubes exactly where a device needs them.

What carries the argument

The load-bearing object is the modified photoresist, 'Mod-PR': a conventional positive photoresist (HPR 504) in which 0.2 M of Ni(salen), $N,N'$-bis(salicylidene)ethylenediiminato nickel(II), is dispersed. It does two jobs at once. Lithographically, exposure and development leave catalyst patterns wherever they are drawn; chemically, the 900 °C anneal decomposes the complex into 10–100 nm Ni particles. During growth, the tubes advance by a tip-growth mechanism, and the paper invokes capillary action of liquid-like Ni particles at the nucleation stage to explain how nickel is drawn into the tube cavity, producing the partial filling.

What would settle it

Measure the hysteresis loop of the same as-grown Ni-filled film after selectively removing the catalyst particles at the nanotube tips (for example by mild chemical etching that leaves the tubes intact) and compare it with the as-grown loop: if the 94 Oe coercivity at 5 K drops toward the bulk nickel value, then the nanowire filling is not what produces the reported magnetic enhancement.

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Extended reading notes

Core claim

The central claim is that simply dissolving Ni(salen) in a standard positive photoresist (HPR 504) turns the photoresist itself into a catalyst source that both defines where nanotubes grow and supplies the metal that fills them. After spin-coating and a 400 °C anneal, the modified resist forms uniformly distributed Ni catalyst particles 10–100 nm in size. Hydrogen annealing and propane CVD at 850 °C then produce long, clean multiwalled nanotubes whose tips carry catalyst particles, indicating tip growth, and whose cavities contain continuous nickel nanowires with 0.21 nm lattice fringes matching the Ni(111) planes. The paper states that this is the first use of Ni(salen) as a carbon-nanotube catalyst, and that the method is scalable and site-selective.

Load-bearing premise

The coercivity claim assumes the SQUID signal is dominated by the nickel nanowires inside the nanotubes; the measurement was made on the whole as-grown film, which also contains nickel catalyst particles at the nanotube tips, and no control or subtraction separates the two contributions.

Editorial extensions

If this is right

  • Standard photolithography alone can place Ni-filled carbon nanotubes at predefined locations, removing a barrier to integrating filled nanotubes into devices.
  • The as-grown film is ferromagnetic at 5 K with a coercivity of 94 Oe, about 130 times the bulk nickel value of 0.7 Oe and higher than the 40 Oe earlier reported for the same material at 2 K.
  • Atmospheric-pressure CVD with propane yields well-graphitized multiwalled nanotubes with $I_D/I_G = 0.32$, clean outer surfaces, and no metal residue outside the tubes.
  • Because the nickel filling is formed in situ rather than by a separate infiltration step, the entire fabrication is a single growth run.

Reading between the lines

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

  • I infer that the photoresist-mixing strategy should extend to other metal–salen or metal–organic precursors whose decomposition temperatures match the CVD anneal, giving site-selective iron- or cobalt-filled nanotubes for other magnetic or catalytic uses; the paper only demonstrates nickel.
  • A testable extension is to tune the filling fraction through growth time, temperature, and propane flow, since the paper explains filling as capillary uptake during nucleation but does not report such a sweep.
  • Because the SQUID measurement was made on the whole as-grown film, the natural control is to measure the film after selectively removing the tip catalyst particles; the paper does not include that control, so the 94 Oe value is best read as a film-level observation rather than a nanowire-only property.
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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

2 major / 4 minor

Summary. The manuscript reports the growth of Ni-filled multiwalled carbon nanotubes by atmospheric-pressure chemical vapor deposition at 850 °C using propane on Si, with a modified photoresist containing Ni(salen) as the catalyst source. The authors claim that this simple photolithographic route enables scalable, site-selective growth of high-quality, partially Ni-filled MWCNTs. Evidence includes SEM showing uniform CNT growth and tip-growth morphology, HRTEM showing Ni nanowires encapsulated in the tubes with a 0.21 nm (111) Ni lattice spacing, EDX confirming Ni filling, and Raman spectroscopy with an ID/IG ratio of 0.32. Magnetic measurements by SQUID at 5 K are reported to show ferromagnetic behavior with a coercivity of 94 Oe, which the authors compare to bulk Ni and to a previously reported Ni-filled CNT value.

Significance. If the claims are supported, the photoresist-based patterning method would be a practically useful advance for integrating Ni-filled CNTs into devices, since it avoids separate catalyst deposition and achieves in situ filling. The TEM and EDX evidence for encapsulated Ni nanowires is direct and convincing for the synthesis claim, and the site-selective growth shown in Figure 10 is a clear strength. The Raman data support the high-quality claim. However, the magnetic characterization, which is a headline quantitative result, is not yet sufficiently controlled to support the stated ferromagnetic and shape-anisotropy conclusions. The paper is suitable for an applied-physics journal if this load-bearing gap is addressed.

major comments (2)
  1. [§3, Figure 9] The coercivity of 94 Oe is measured on the whole as-grown film, which contains Ni catalyst particles at the nanotube tips (Figures 4 and 5(c)) and may contain residual surface Ni particles from the annealed Mod-PR film (Figure 2). No control measurement on a sample without filling, no subtraction of the exposed-Ni contribution, and no acid-wash or selective-etch experiment are reported. Therefore the hysteresis loop cannot be attributed specifically to the encapsulated Ni nanowires, and the comparison to bulk Ni and to ref [28] does not establish the claimed shape-anisotropy enhancement. The authors should either isolate the filling contribution or temper the magnetic claim accordingly.
  2. [§3, coercivity comparison paragraph] The comparison with ref [28] compares a coercivity measured at 5 K with a value reported at 2 K. Since coercivity is strongly temperature-dependent in ferromagnetic nanomaterials, the temperature difference alone prevents a meaningful quantitative comparison. The authors should either remeasure at the same temperature, report the temperature dependence, or discuss the expected effect of the temperature difference. The same paragraph also quotes bulk Ni Hc = 0.7 Oe without specifying the measurement temperature, which should be provided.
minor comments (4)
  1. [§3, EDX analysis] The text states that EDX analysis of the as-grown CNTs 'is not shown here'; including this spectrum, or a representative one, in the main text or supporting information would strengthen the compositional claim.
  2. [Figure 9] The magnetization curve in Figure 9 lacks visible axis labels and units, and the sample mass is not reported. Since the manuscript presents quantitative magnetic data, the authors should provide calibrated axes and report the magnetization normalization (per gram or per volume of Ni).
  3. [§3, growth model] The growth model for partial Ni filling is referenced to ref [25] but not summarized. For self-containedness, please add one or two sentences describing the capillary-action mechanism and how it applies to the present experimental conditions.
  4. [Figure 10] The site-selectivity claim would be easier to evaluate if the SEM images in Figure 10 included scale bars and if the text quantified the contrast between patterned and unpatterned regions (e.g., presence or absence of CNTs outside the catalyst patterns).

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: the paper reports direct experimental observations with no fitted-input or self-citation chain that reduces a 'prediction' to its inputs.

full rationale

This is an experimental synthesis-and-characterization paper. The central claims—site-selective growth, Ni-filled MWCNTs, high quality evidenced by Raman, and ferromagnetic behavior with measured coercivity—are supported by direct SEM, TEM, EDX, Raman, and SQUID measurements. There is no derivation chain in which an output quantity is constructed to equal an input quantity. The only self-citation is reference [25], invoked for the growth model: 'The details of the growth model are discussed elsewhere [25].' That citation explains a proposed mechanism for partial Ni filling, but it is not load-bearing for the reported observations; the filling is directly imaged by TEM and identified by HRTEM lattice spacing and EDX, and the growth model is not used to generate or predict the measured coercivity or the Raman ID/IG ratio. The coercivity comparison to bulk Ni (0.7 Oe, ref [27]) and to a prior Ni-filled nanotube value (40 Oe at 2 K, ref [28]) is an external benchmark, not an input to the experiment. No fitted parameter is renamed as a prediction, and no uniqueness or existence theorem from prior work by these authors is invoked to force a conclusion. Consequently, the circularity burden is minimal; the finding is no significant circularity.

Assumptions & free parameters 0 free parameters · 4 assumptions · 0 invented entities

The paper introduces no new theoretical entities. It depends on material assumptions about precursor decomposition, carbon source roles, magnetic signal attribution, and sample representativeness.

assumptions (4)
  • domain assumption Ni(salen) mixed in photoresist decomposes during the 900 C anneal into metallic Ni nanoparticles that catalyze CNT growth.
    Invoked in Section 2; only indirectly supported by the SEM image after annealing, with no phase or composition analysis of the nanoparticles.
  • domain assumption Propane is the carbon source and the carbonized photoresist neither contributes carbon nor poisons growth.
    No control experiment with photoresist alone or without Ni(salen) is reported in Section 2 or 3.
  • domain assumption The bulk SQUID magnetization and coercivity are attributed to encapsulated Ni nanowires rather than to catalyst particles at tips or on the substrate.
    The measurement in Section 3 is on the entire film; no subtraction or control isolates the filling.
  • domain assumption A single Raman spectrum and selected TEM images represent the quality and filling state of the whole sample.
    Raman and HRTEM results in Section 3 are presented without statistics or spatial mapping.

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Cite this review

Pith. "Pith review of Site selective synthesis of in situ Ni filled multiwalled carbon nanotubes using Ni(salen) as a catalyst source." pith.science (2026). https://pith.science/paper/UVQY63HA

@misc{pith2026190804516,
  author       = {Pith},
  title        = {Pith review of: Site selective synthesis of in situ Ni filled multiwalled carbon nanotubes using Ni(salen) as a catalyst source},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/UVQY63HA}},
  note         = {Machine review of arXiv:1908.04516}
}
read the original abstract

The synthesis of Ni filled multiwalled carbon nanotubes was performed by atmospheric pressure chemical vapor deposition with propane on Si at 850 C using a simple mixture of Ni(salen), and a conventional photoresist. Analysis of the carbon nanotubes using scanning electron microscopy together with high resolution transmission electron microscopy show that the nanotubes have grown by a tip growth mechanism and exhibit a multi walled structure with partial Ni filling. The high quality of the Ni filled nanotubes is evidenced by Raman spectroscopy. The magnetic properties of Ni filled nanotubes were analyzed using a superconducting quantum interference device which revealed their ferromagnetic behavior with large coercivity. A scalable as well as site selective growth of high quality Ni filled carbon nanotubes is achieved by a simple photolithographic method.

Figures

Figures reproduced from arXiv: 1908.04516 by the authors.

Figure 1
Figure 1. SEM image of the Ni(salen) powder [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. SEM micrograph of the catalytic nanoparticles prepared from Mod-PR film over the Si(111) substrate after annealing at 900 ◦C [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗
Figure 3
Figure 3. SEM micrograph of the MWCNTs synthesized using Mod-PR by CVD growth. of crystallite sizes [PITH_FULL_IMAGE:figures/full_fig_p002_3.png] view at source ↗
Figures from the paper (6 more)
Figure 4
Figure 4. Figure 4: High magnification SEM micrograph of the MWCNTs synthesized using Mod-PR by CVD growth indicating the tip-growth mechanism. seen that most of the CNTs are nearly straight and long with a high number density. Furthermore, the wall surfaces of the CNTs appear relatively …
Figure 5
Figure 5. Figure 5: (a) and (b) TEM images of Ni-filled CNTs exhibiting continuous filling. (c) TEM images of as-formed MWCNTs indicating the tip-growth mechanism. 3 [PITH_FULL_IMAGE:figures/full_fig_p003_5.png]
Figure 6
Figure 6. Figure 6: (a) TEM image of an as-formed MWCNT encapsulating a metal nanowire, (b) high-resolution TEM image of the CNT-encapsulated nanowire as indicated in (a). (c) High-resolution TEM image of the nanotube wall as indicated in (a) [PITH_FULL_IMAGE:figures/full_fig_p004_6.png]
Figure 8
Figure 8. Figure 8: Raman spectrum (514.5 nm excitation) of the Ni-filled MWCNT film grown by CVD on Si using Mod-PR. from the HRTEM image (figure 6(b)). The Cu signals are due to the copper grid supporting the sample. The growth model of partially Ni-filled nanotubes can be explained by …
Figure 9
Figure 9. Figure 9: Magnetic hysteresis loop at T = 5 K of Ni-filled MWCNTs grown by CVD using Mod-PR. graphitic materials. The intensity ratio of the D peak to the G peak, which measures quality, as derived from figure 8 is R = ID/IG = 0.32, indicating that the grown CNTs are highly crys…
Figure 10
Figure 10. Figure 10: Site-selective growth of Ni-filled MWCNTs by direct photolithographic route using Mod-PR: (a) SEM image of a Mod-PR pattern, (b) SEM image of the Mod-PR pattern after CNT growth and (c) SEM image of another patterned growth of CNTs using Mod-PR. 5 [PITH_FULL_IMAGE:fi…

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Reviewed August 14, 2026 · model on record in the stance chip above.