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Paper Citation Record · LEDGER

Crystallographic splitting theorem for band representations and fragile topological photonic crystals

As of 21 August 2026, this Paper Citation Record lists 21 of 21 outbound references and 0 inbound Pith citation observations for arXiv:1908.08541.

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pith.paper-citation-record.v1
1908.08541 v2

Coverage vector

measured 21 of 21 reference resolution

Typed states for the displayed outbound observations.

Source: paper_references, paper_reference_links, observed 2026-08-14T11:44:46.522462Z

measured 21 of 21 standing notices

One-hop event checks from named stored sources.

Source: scholarly_work_events, retraction_status_cache, observed 2026-08-21T06:32:19.484+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

21 of 21 outbound references displayed

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  • verified fuzzy15
  • unresolved5
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External citation measurements

No source-named external measurement is stored.

Outbound references

Observation 744eeb78-55b4-4046-a6db-ce3a72a6c989 · outbound

This paper cites an unresolved cited work.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals Unresolved cited work

Reference 1

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unresolved
raw_fallback, observed 2026-08-14T11:44:46.883126Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.429366Z digest=sha256:da42a6e93682a3e1e683348b4f7ea2fd1201879808c8562cea79968372730321

Observation 7f75ddef-69dc-4e8b-97d6-e271510b686d · outbound

This paper cites Since Pj is invariant under H [cf.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals Since Pj is invariant under H [cf

Reference 2

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Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.414674Z digest=sha256:3dc5cdb27957ec1af95e6552ff0d1dc7462375c156963dc02ade29f0e0316b23

Observation 9ac977a2-cdfc-4e76-a66d-b12089544068 · outbound

This paper cites an unresolved cited work.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals Unresolved cited work

Reference 3

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.422034Z digest=sha256:00d369406732ab5584a3cb10d459fdc4ef5a0deecaf8a53d933ef4c2e472c18d

Observation 79407668-2bd9-4ced-81e3-d410a4177ba5 · outbound

This paper cites V B that the splitting P = ⊕N j=1Px j into bands of the projected position operator [cf.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals V B that the splitting P = ⊕N j=1Px j into bands of the projected position operator [cf

Reference 4

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.434800Z digest=sha256:e0f052c72321285775afb59fa2b5b78e58201760b345f3be8a98450535b5047e

Observation fe54adab-e5e0-48c6-93db-f644414697cf · outbound

This paper cites The reduced real-space coordinates of the two pairs of orbitals are (0 , 0, 0), in an orthog- onal basis of Bravais lattice vectors.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals The reduced real-space coordinates of the two pairs of orbitals are (0 , 0, 0), in an orthog- onal basis of Bravais lattice vectors

Reference 5

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Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.440545Z digest=sha256:b6e5db053980e2841fc484f440f3f3079db3613172ed102f0647a57ef2b410ee

Observation 24b8fb8d-4af4-4189-bcc6-901702596ebf · outbound

This paper cites an unresolved cited work.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals Unresolved cited work

Reference 6

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Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.446289Z digest=sha256:95b82cd7f7556ca423593d5b7bd019051d5af1b3a3c30a9d23af6bd4a4b45f26

Observation ad717717-be14-421f-a95b-bd8bf3ae9b4a · outbound

This paper cites A finite group G is solvable if there exists a series of normal groups, i.e., C1 =G0◁G 1◁G 2...◁G k =G (F1) for a k ≥ 1, such that Gj+1/Gj is abelian for all j = 1,...,k − 1.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals A finite group G is solvable if there exists a series of normal groups, i.e., C1 =G0◁G 1◁G 2...◁G k =G (F1) for a k ≥ 1, such that Gj+1/Gj is abelian for all j = 1,...,k − 1

Reference 7

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.452226Z digest=sha256:ea1002f7b36af11c54dd85b093305702056ebf123a98edcd87ec0aadc97d7c39

Observation 935a0810-90d1-439e-8c01-e7b30112bd4f · outbound

This paper cites an unresolved cited work.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals Unresolved cited work

Reference 8

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raw_fallback, observed 2026-08-14T11:44:46.789692Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.457437Z digest=sha256:acccfb456a3f4e387b83f09fdb1d2bbfb55e623afb4684302a6221493ecfb058

Observation 172697d5-8716-4a3e-9ced-6873cac6e3ae · outbound

This paper cites The 11 point groups constructed in this way are S2, C2h, C3i, C4h, C6h, D2h, D3d, D4h, D6h, Th and Oh.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals The 11 point groups constructed in this way are S2, C2h, C3i, C4h, C6h, D2h, D3d, D4h, D6h, Th and Oh

Reference 9

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.462601Z digest=sha256:6d0243db8402b0d9bea1f26ab3606eee643484cd5f96b36c2b7ab47a5bbc087a

Observation 4a99fad9-9344-46cf-a8b4-c19737a60ad0 · outbound

This paper cites Review of the semi-direct product.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals Review of the semi-direct product

Reference 10

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.467865Z digest=sha256:49dd89c8bf1f8051f41812162c4f59629df17c4dd979d76aa3ba3823b72ee541

Observation 18e3f031-7613-40bc-b10d-21cc6365ca31 · outbound

This paper cites This two-fold rotational symmetry generates C′′ 2.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals This two-fold rotational symmetry generates C′′ 2

Reference 11

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.473265Z digest=sha256:a08b1f2025918630afbceea237ff8a600a0bffa9f5e5c71d829394d751986b87

Observation 8744502c-0b68-496b-bb90-19e0217a4706 · outbound

This paper cites F 1 to prove that all 27 noncubic double point groups [class (2)] are monomial.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals F 1 to prove that all 27 noncubic double point groups [class (2)] are monomial

Reference 12

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.478443Z digest=sha256:43716deb20064e93a96a6d9840cd52e6630a96957bdf4fbbe5450077ad9f0e13

Observation 2c99cca6-6757-454a-956e-543d688260bf · outbound

This paper cites F 4 b that allP in class (2)A are monomial; then, according to the Lemma for monomial direct-product groups in App.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals F 4 b that allP in class (2)A are monomial; then, according to the Lemma for monomial direct-product groups in App

Reference 13

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.483601Z digest=sha256:822e10d5a9b32a82926416834f0b0ab1f1c297af65f307a8b6f1234165a989dc

Observation 237aefc1-0385-4bb9-9d94-3ce2ea68dad2 · outbound

This paper cites Our proof relies on Wigner’s seminal result, 104 namely that all irreps ofPT =P× ZT 2 are induced from irreps of the crystallographic point group P.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals Our proof relies on Wigner’s seminal result, 104 namely that all irreps ofPT =P× ZT 2 are induced from irreps of the crystallographic point group P

Reference 14

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.488286Z digest=sha256:c88cfb5c498ce0cf550784665d2278301b6298f1c476ff4c1e4cffac213d66cb

Observation 399383a8-f46b-472d-9610-f1969f457de2 · outbound

This paper cites ˜T and ˜O are standard examples of non-monomial groups.188 Example of non-monomial irrep of double cubic point group ˜T.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals ˜T and ˜O are standard examples of non-monomial groups.188 Example of non-monomial irrep of double cubic point group ˜T

Reference 15

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.492925Z digest=sha256:ffb370fe115f025e3733b6a4f5efa94b76ad616eebc00c65f18fa8ec04fe9efc

Observation e717ca84-c5ba-4ed5-8583-832754fdebdf · outbound

This paper cites an unresolved cited work.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals Unresolved cited work

Reference 16

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.497697Z digest=sha256:58bca85b95054320eb7bcfc48dba13d92998869b4726f837b8bbe07d24d296ef

Observation ed83186e-e3b0-4d53-8c1f-e3a305188e2a · outbound

This paper cites Of the three remaining double cubic point groups, two have the direct-product form: ˜Th = ˜T× Zi 2 and ˜Oh = ˜O× Zi.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals Of the three remaining double cubic point groups, two have the direct-product form: ˜Th = ˜T× Zi 2 and ˜Oh = ˜O× Zi

Reference 17

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.502800Z digest=sha256:585f1331472d896db84e72a5f209c1fc217eda08ef7557a1f905777f7ce9bbce

Observation 85b91ad0-2251-45fd-a234-988bf675c1c7 · outbound

This paper cites F 4.) Since ˜O and ˜T are non-monomial, it follows that ˜Oh and ˜Th must also be non-monomial, according to the Lemma for monomial direct-product groups in App.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals F 4.) Since ˜O and ˜T are non-monomial, it follows that ˜Oh and ˜Th must also be non-monomial, according to the Lemma for monomial direct-product groups in App

Reference 18

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verified fuzzy
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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.507184Z digest=sha256:9816153eb11283f0322c14cd957d95d09a76abc23141c5066adc55fee7d3bf17

Observation 35b29194-213f-4990-bdc6-3ce43cefb05f · outbound

This paper cites A 1 from the perspective of band theory.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals A 1 from the perspective of band theory

Reference 19

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.512544Z digest=sha256:29e785d14dc633d23146510404b37cbd5255b66f78583eec5a0e5f9da3b63e3c

Observation 7366a28e-bdae-4949-a34a-ae26e89b98b5 · outbound

This paper cites For simplicity, let us consider a rank-N BR(G, ϖ,D ).

Crystallographic splitting theorem for band representations and fragile topological photonic crystals For simplicity, let us consider a rank-N BR(G, ϖ,D )

Reference 20

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.517435Z digest=sha256:6dd7a03e58796d4d20bc21af43ebfa2094f9a09be09e3fae8f9e887bb1144e3f

Observation f1c69a6b-29ae-4645-a39d-e614052c5b7c · outbound

This paper cites Wilson loop approach to fragile topology of split elementary band representations and topological crystalline insulators with time reversal symmetry.

Crystallographic splitting theorem for band representations and fragile topological photonic crystals Wilson loop approach to fragile topology of split elementary band representations and topological crystalline insulators with time reversal symmetry

Reference 21

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No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.

source=pdf_text observed=2026-08-14T11:44:46.522462Z digest=sha256:0e5198f05de91b2fb7218c1f114a4c4c78e0c4b4977c07a10b2e35366751d417

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