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Paper Citation Record · LEDGER

Photon drag at the junction between metal and 2d semiconductor

As of 13 August 2026, this Paper Citation Record lists 17 of 17 outbound references and 0 inbound Pith citation observations for arXiv:2411.14075.

A citation records a reference. It does not transfer a finding from one paper to another.

pith.paper-citation-record.v1
2411.14075 v1

Coverage vector

measured 17 of 17 reference resolution

Typed states for the displayed outbound observations.

Source: paper_references, paper_reference_links, observed 2026-08-12T15:41:39.047148Z

measured 17 of 17 standing notices

One-hop event checks from named stored sources.

Source: scholarly_work_events, retraction_status_cache, observed 2026-08-12T06:34:41.77262+00:00

measured 0 of 0 inbound itemization

Pith citing papers itemized under the disclosed page cap.

Source: paper_references, paper_reference_links

measured 0 of 1 external citation measurements

A source-named dated measurement, never combined with another source.

Source: cited_works

Reference resolution

17 of 17 outbound references displayed

  • verified exact1
  • verified fuzzy13
  • unresolved3
  • parse uncertain0
  • malformed identifier0
  • metadata mismatch0

External citation measurements

No source-named external measurement is stored.

Outbound references

Observation 1f6fee18-04fc-476c-ae6b-a02aaa89c5f7 · outbound

This paper cites 1 (A)], electromagnetic diffraction gives rise to the local z-component of electric field.

Photon drag at the junction between metal and 2d semiconductor 1 (A)], electromagnetic diffraction gives rise to the local z-component of electric field

Reference 1

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.499128Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:38.909361Z digest=sha256:ad300c168be24075b63b64f707964c710dd26cb9fa9380be6f52aee51e771bd3

Observation 861ab0e0-ef67-41dc-9c3c-a0c24698d401 · outbound

This paper cites We consider the most practical case of monochromatic waves, E(t) = Eω e−iωt + h .c., and similarly for other time-dependent quantities.

Photon drag at the junction between metal and 2d semiconductor We consider the most practical case of monochromatic waves, E(t) = Eω e−iωt + h .c., and similarly for other time-dependent quantities

Reference 4

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.459324Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:38.925060Z digest=sha256:f3f89007f1c6d07e4381b3dec63e835831dd7541e9787675f6a12d774c5708a7

Observation 3c44c8c1-a72b-44ea-9b71-a3771773584f · outbound

This paper cites (3) The superscript ‖ implies taking only the x and y com- ponents of the respective vector, it stems from the two- dimensional character of the current density.

Photon drag at the junction between metal and 2d semiconductor (3) The superscript ‖ implies taking only the x and y com- ponents of the respective vector, it stems from the two- dimensional character of the current density

Reference 5

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.433635Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:38.933617Z digest=sha256:84541396237a628e0e72e98fffbc5582ed853bc0d459adc24249936f24348dcc

Observation e9973c4a-44f7-4748-8e1d-0a7919fc0ac2 · outbound

This paper cites an unresolved cited work.

Photon drag at the junction between metal and 2d semiconductor Unresolved cited work

Reference 6

Resolution
unresolved
raw_fallback, observed 2026-08-12T15:41:39.537439Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:38.892880Z digest=sha256:5eaa78d75ad821e545dc68db50883d40af5f087c9a5b3270e6f58a755606e616

Observation 69933a8d-ea0b-4ff9-ba92-794918efdf7d · outbound

This paper cites Such photocurrent is often marked as ’plasmon drag’10, though the underlying electromagnetic forces are the same as in photon drag.

Photon drag at the junction between metal and 2d semiconductor Such photocurrent is often marked as ’plasmon drag’10, though the underlying electromagnetic forces are the same as in photon drag

Reference 7

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.519384Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:38.899797Z digest=sha256:284c72bdc7b9017226983d6f0c0fc6ec342f4044deba689f07f74233533ec66a

Observation 215efda9-163b-4143-8a35-70e1b11496ae · outbound

This paper cites At this stage, we assume that all angular harmonics of the second-order dc distribution function, except for the zeroth and the first ones, are damped.

Photon drag at the junction between metal and 2d semiconductor At this stage, we assume that all angular harmonics of the second-order dc distribution function, except for the zeroth and the first ones, are damped

Reference 8

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.406648Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:38.947311Z digest=sha256:a6522c9ca5621eaab60ab02cbbb79edff29e7c777d408d009c00b24ad92486a5

Observation a40859df-6d4b-4fdd-bf63-7c9405bf3d95 · outbound

This paper cites (27) We observe that ’ordinary’ photon drag differs from the ’junction drag’ by factors of η′ (absorbance factor) and kxLsd (light momentum factor).

Photon drag at the junction between metal and 2d semiconductor (27) We observe that ’ordinary’ photon drag differs from the ’junction drag’ by factors of η′ (absorbance factor) and kxLsd (light momentum factor)

Reference 11

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.169229Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:39.028268Z digest=sha256:e27040704927d78be139ca267e2e15cc88ff383fdd927f7e42f904cc62e6705c

Observation a96fc9ca-d2d3-4edb-8eec-a6cf00f7db47 · outbound

This paper cites an unresolved cited work.

Photon drag at the junction between metal and 2d semiconductor Unresolved cited work

Reference 13

Resolution
unresolved
raw_fallback, observed 2026-08-12T15:41:39.382930Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:38.955482Z digest=sha256:ce400523eb4ae914420c9128d7ef4b7c52eb8012f89cfb7b87372cb6dbd14700

Observation e5d0adb2-21d8-490a-be7e-ec6b49977871 · outbound

This paper cites 7 All our consideration was based on assumption that the photovoltage at an individual metal contact (say, source) can be isolated from the photovoltage at the drain.

Photon drag at the junction between metal and 2d semiconductor 7 All our consideration was based on assumption that the photovoltage at an individual metal contact (say, source) can be isolated from the photovoltage at the drain

Reference 14

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.195024Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:39.018176Z digest=sha256:635a3827f63d7b6b9ac71d47b378a72e55d8f85062a9a039063aa9054c2eb0aa

Observation 178002fd-5195-403a-9fba-9c0bd522dbe0 · outbound

This paper cites We attempted to formulate the theory in terms of high- frequency 2d conductivity σω , independent of its micro- scopic nature.

Photon drag at the junction between metal and 2d semiconductor We attempted to formulate the theory in terms of high- frequency 2d conductivity σω , independent of its micro- scopic nature

Reference 16

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.134955Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:39.034391Z digest=sha256:040bc3af20a4c3b7334bd2aae7af4bc99fb82d4a428ed6976fd07a9ec9a7038b

Observation 6c2b63b8-979f-45d8-ba20-4fe719a32e77 · outbound

This paper cites Terahertz ratchet effects in graphene with a lateral superlattice.

Photon drag at the junction between metal and 2d semiconductor Terahertz ratchet effects in graphene with a lateral superlattice

Reference 17

Resolution
verified exact
local_arxiv, observed 2026-08-12T15:41:39.114645Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:39.047148Z digest=sha256:d9521abbe3946332f67a67dbe672785523b422bd72bd3762eabdf552a3481184

Observation 79f14547-42bd-44e7-9df8-a1cf92c44722 · outbound

This paper cites This results in αx = |Epl|2 |E0|2 { Reη × Qpl − Imη 2 } , (23) where Qpl = Reqp pl/Imqp pl is the quality factor of 2D plas- mons.

Photon drag at the junction between metal and 2d semiconductor This results in αx = |Epl|2 |E0|2 { Reη × Qpl − Imη 2 } , (23) where Qpl = Reqp pl/Imqp pl is the quality factor of 2D plas- mons

Reference 19

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.340128Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:38.973175Z digest=sha256:505cfa2f4591277faee00edeba04bed1c1078471acf7f2200409d4c589f1a4df

Observation 76eefdd7-e4a8-4710-9e09-bcac931c5a61 · outbound

This paper cites (25) As the momentum transfer coefficient αx ∼ 1, we observe that the only parameter governing the ratio of PTE and PD photovoltages is ωτε.

Photon drag at the junction between metal and 2d semiconductor (25) As the momentum transfer coefficient αx ∼ 1, we observe that the only parameter governing the ratio of PTE and PD photovoltages is ωτε

Reference 21

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.304539Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:38.985212Z digest=sha256:7092e482d73eeeaf9c9f3442481a9540aed0ed3ee4c00b73382f4b237353e860

Observation 5d3ad9fe-f143-4926-9c91-c6e1b1613dc8 · outbound

This paper cites The difference in effective dielectric functions in s- and p- polarizations results in different plasmon dispersion laws.

Photon drag at the junction between metal and 2d semiconductor The difference in effective dielectric functions in s- and p- polarizations results in different plasmon dispersion laws

Reference 33

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.363624Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:38.966254Z digest=sha256:f5df42c8ea8a2c1dfc1b04c3a350b9ca7b9760c925632f847358a6e773038c89

Observation 4342fada-ac87-4b57-9490-608b58767cda · outbound

This paper cites In the far infrared range ( λ0 = 10 µm), we estimate ωτε ≫ 1 even for the shortest energy relaxation time τε = 0.1 ps.

Photon drag at the junction between metal and 2d semiconductor In the far infrared range ( λ0 = 10 µm), we estimate ωτε ≫ 1 even for the shortest energy relaxation time τε = 0.1 ps

Reference 42

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.280996Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:39.000026Z digest=sha256:4132bf96104fd68ca625ea697eae0557e5fb3e98b9b3f13a822cdc295861cf33

Observation dcebf262-8300-4b55-bd5f-a3e593e78285 · outbound

This paper cites Relative polarity of carriers in the screening layer and in the 2DES bulk affects the photo- electric effects.

Photon drag at the junction between metal and 2d semiconductor Relative polarity of carriers in the screening layer and in the 2DES bulk affects the photo- electric effects

Reference 43

Resolution
verified fuzzy
raw_fallback, observed 2026-08-12T15:41:39.240280Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:39.006086Z digest=sha256:35b5c27e7bb7b2ec018181610ac76f5f082cc87c2a93b7da235dd2c8eb7f9f1d

Observation 419cb681-c2d9-4112-950f-f26152aee2d0 · outbound

This paper cites an unresolved cited work.

Photon drag at the junction between metal and 2d semiconductor Unresolved cited work

Reference 44

Resolution
unresolved
raw_fallback, observed 2026-08-12T15:41:39.216734Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T15:41:39.011993Z digest=sha256:5e59db61249125afd5021d3f4fac9f0c5728dd644675c59b59ac3f73d21cc4e2

Pith citing papers

No inbound Pith citation observations are available.