Skip to content
DraconiticResearch
Search Sources API
197,768 studies31 sourcesUpdated 18 min ago
PreprintCC BY 4.0arXiv

Grid Optimization for Wide Field Modulation Collimators

Abstract

Wide-field localization of transient sources such as gamma-ray bursts (GRBs) places new demands on the grid design of modulation collimators, whose usable field of view (FOV) is normally limited by self-vignetting. A grid slat thick enough to be opaque at the energies of interest also clips off-axis rays, shrinking the effective slit width and ultimately defining the FOV itself. Historical bigrid or rotating-modulation-collimator (RMC) designs have been designed with this trade-off as an unavoidable consequence of geometric optics. We explore whether the cross-sectional shape of the grid slats can be optimized for wide FOV applications. We derive a general transmission-function framework for a bigrid pair in terms of an effective slit width that depends on slat geometry and use it to compare four slat cross sections: the conventional rectangular slat, an idealized diamond profile, a hexagonal profile that approximates photochemical etching, and the circular wire grids of early X-ray astronomy. We show that for the same bigrid pitch and thickness, a diamond profile extends the FOV and eliminates clipping throughout most of the field. We also demonstrate that a hexagonal profile achievable with standard tungsten etching factors captures many of the benefits of the idealized diamond profile. Extending the analysis to the four-phase demodulation, we show that slat shape directly sets the extent of the resulting phase-space blind spots, and that the diamond profile removes them entirely across a target FOV where the rectangular baseline cannot. We further show that finite grid opacity is a largely separable effect. Leakage through the grid leaves the geometric blind-spot boundaries unchanged. These results identify slat cross-sectional shape as a design parameter that can substantially increase throughput and widen the blind-spot-free field of view of a wide-field modulation collimator.

Related

  1. Wide Field Localization Using Fixed Modulation Collimators
    Steven E. Boggs
    arXivPreprintCC BY 4.0Full textHigh-energy astrophysicsInstrumentation & methodsarXiv
  2. An X-ray Extremely wide-field Spectroscopic Surveyor (XESS, or "chess")
    W. P. Maksym, M. Ulmer, S. Friedrich +20
    arXivPreprintarXiv licenceFull textGalaxiesHigh-energy astrophysicsarXiv
  3. Nancy Grace Roman Space Telescope Wide Field Instrument: Grism Saturation Response to Bright Sources during Thermal-Vacuum Testing
    Lipika Chatur, Dana R. Louie, Joshua E. Schlieder +3
    arXivPreprintCC BY 4.0Full textInstrumentation & methodsarXiv
  4. Refurbishment and Cryocooler Upgrade of the CPAPIR Wide-Field Near-Infrared Camera: Design, Integration, and Lessons Learned
    Philippe Vallee, Jonathan St-Antoine, Lison Malo +5
    arXivPreprintarXiv licenceFull textInstrumentation & methodsarXiv
  5. LenNet: Direct Detection and Localization of Strong Gravitational Lenses in Wide-Field Sky Survey Images
    Pufan Liu, Hui Li, Ziqi Li +9
    arXivPreprintCC BY 4.0Full textGalaxiesarXiv
BibTeX
@misc{boggs2026grid,
  title = {{Grid Optimization for Wide Field Modulation Collimators}},
  author = {Steven E. Boggs},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.05523},
  eprint = {2610.05523},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.05523},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Grid Optimization for Wide Field Modulation Collimators
AU  - Steven E. Boggs
PY  - 2026
DA  - 2026/10/04
PB  - arXiv
DO  - 10.48550/arxiv.2610.05523
UR  - https://arxiv.org/abs/2610.05523
AB  - Wide-field localization of transient sources such as gamma-ray bursts (GRBs) places new demands on the grid design of modulation collimators, whose usable field of view (FOV) is normally limited by self-vignetting. A grid slat thick enough to be opaque at the energies of interest also clips off-axis rays, shrinking the effective slit width and ultimately defining the FOV itself. Historical bigrid or rotating-modulation-collimator (RMC) designs have been designed with this trade-off as an unavoidable consequence of geometric optics. We explore whether the cross-sectional shape of the grid slats can be optimized for wide FOV applications. We derive a general transmission-function framework for a bigrid pair in terms of an effective slit width that depends on slat geometry and use it to compare four slat cross sections: the conventional rectangular slat, an idealized diamond profile, a hexagonal profile that approximates photochemical etching, and the circular wire grids of early X-ray astronomy. We show that for the same bigrid pitch and thickness, a diamond profile extends the FOV and eliminates clipping throughout most of the field. We also demonstrate that a hexagonal profile achievable with standard tungsten etching factors captures many of the benefits of the idealized diamond profile. Extending the analysis to the four-phase demodulation, we show that slat shape directly sets the extent of the resulting phase-space blind spots, and that the diamond profile removes them entirely across a target FOV where the rectangular baseline cannot. We further show that finite grid opacity is a largely separable effect. Leakage through the grid leaves the geometric blind-spot boundaries unchanged. These results identify slat cross-sectional shape as a design parameter that can substantially increase throughput and widen the blind-spot-free field of view of a wide-field modulation collimator.
ER  -