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pith:OGQLLPO4

pith:2026:OGQLLPO4YP4Z4VHQCEIHFKKA2B
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Multi-mode Photonic Time Crystals Based on Time-Modulated Metasurface Waveguides

M. S. Mirmoosa, V. Asadchy, X. Wang, Z. Li

Time modulation of metasurface waveguides creates tilted intermodal band gaps in photonic time crystals, controllable by modulation phase.

arxiv:2605.14268 v1 · 2026-05-14 · physics.optics

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\usepackage{pith}
\pithnumber{OGQLLPO4YP4Z4VHQCEIHFKKA2B}

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Record completeness

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2 Internet Archive
3 Author claim open · sign in to claim
4 Citations open
5 Replications open
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Claims

C1strongest claim

temporal modulation in this platform gives rise not only to conventional intramodal band gaps associated with same-branch coupling, but also to tilted intermodal band gaps originating from coupling between different guided-mode branches... the modulation phase difference provides an effective symmetry-control parameter: by exploiting temporal glide symmetry, one can selectively suppress or enhance gap opening

C2weakest assumption

The metasurface waveguide remains impenetrable and supports the assumed guided surface and higher-order volume modes under the proposed time modulation without significant losses or fabrication imperfections that would close the intermodal gaps.

C3one line summary

Time-modulated metasurface waveguides enable multimode photonic time crystals with intramodal and tilted intermodal band gaps that support directional amplification and symmetry-based gap control.

References

44 extracted · 44 resolved · 0 Pith anchors

[1] Metamaterials with high degrees of freedom: space, time, and more, 2020
[2] Using time-varying systems to challenge fundamental limitations in electromagnetics: Overview and summary of applications, 2023
[3] V. Pacheco-Peña and N. Engheta, “Temporal aiming,” Light. Sci. & Appl.9, 129 (2020) 2020
[4] V. Pacheco-Peña and N. Engheta, “Antireflection temporal coatings,” Optica7, 323–331 (2020) 2020
[5] Temporal interface in dispersive hyperbolic media, 2025

Formal links

1 machine-checked theorem link

Receipt and verification
First computed 2026-05-17T23:39:10.422395Z
Builder pith-number-builder-2026-05-17-v1
Signature Pith Ed25519 (pith-v1-2026-05) · public key
Schema pith-number/v1.0

Canonical hash

71a0b5bddcc3f99e54f0111072a940d04971a81d61bc0537f12f152f225ec2d2

Aliases

arxiv: 2605.14268 · arxiv_version: 2605.14268v1 · doi: 10.48550/arxiv.2605.14268 · pith_short_12: OGQLLPO4YP4Z · pith_short_16: OGQLLPO4YP4Z4VHQ · pith_short_8: OGQLLPO4
Agent API
Verify this Pith Number yourself
curl -sH 'Accept: application/ld+json' https://pith.science/pith/OGQLLPO4YP4Z4VHQCEIHFKKA2B \
  | jq -c '.canonical_record' \
  | python3 -c "import sys,json,hashlib; b=json.dumps(json.loads(sys.stdin.read()), sort_keys=True, separators=(',',':'), ensure_ascii=False).encode(); print(hashlib.sha256(b).hexdigest())"
# expect: 71a0b5bddcc3f99e54f0111072a940d04971a81d61bc0537f12f152f225ec2d2
Canonical record JSON
{
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    "cross_cats_sorted": [],
    "license": "http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
    "primary_cat": "physics.optics",
    "submitted_at": "2026-05-14T02:12:06Z",
    "title_canon_sha256": "7b839bed6af60d2597edae44ee34f76465e6cfc09a15a2661ef7b1af2dd0e1cc"
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  "source": {
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    "kind": "arxiv",
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}