ATST Scattered Light Issues How will mirror microroughness

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ATST Scattered Light Issues • How will mirror microroughness likely impact the coronagraphic performance

ATST Scattered Light Issues • How will mirror microroughness likely impact the coronagraphic performance of ATST? • How do these limitations compare to what we can expect from dust and other particulate contamination on the mirror surface? • How frequently will the ATST primary mirror need to be cleaned to maintain acceptable coronagraphic performance?

The ASAP Model • Define a set of parallel rays representing a point source

The ASAP Model • Define a set of parallel rays representing a point source at the position of the sun’s center. • Introduce these rays onto a “scatter” surface just in front of the primary mirror (M 1). Scatter the parent rays into a half-degree cone centered on the specular direction. • Add a scatter function to M 1 that represents a clean, polished surface, or a surface contaminated by dust.

Sample Positions 2. 0 1. 5 1. 1

Sample Positions 2. 0 1. 5 1. 1

Mirror Signature from Microroughness Typical scatter versus angle for a clean, polished glass surface

Mirror Signature from Microroughness Typical scatter versus angle for a clean, polished glass surface

…In Direction Cosine Space Plotting log 10 | sin – sin 0 | versus

…In Direction Cosine Space Plotting log 10 | sin – sin 0 | versus log 10 BSDF

The Harvey Model b Figure courtesy of Gary Peterson, Breault Research Organization.

The Harvey Model b Figure courtesy of Gary Peterson, Breault Research Organization.

RMS Microroughness and Harvey The single RMS roughness parameter ( ) contains insufficient information

RMS Microroughness and Harvey The single RMS roughness parameter ( ) contains insufficient information to completely characterize the BSDF of the polished surface, even assuming a powerlaw relationship.

Ranges of Slopes All four curves integrate to yield the same total integrated scatter

Ranges of Slopes All four curves integrate to yield the same total integrated scatter predicted for a 20 Ångstrom RMS surface.

Results for 20 Ångstrom Microroughness: S = – 1. 5 = 1. 0 Microns

Results for 20 Ångstrom Microroughness: S = – 1. 5 = 1. 0 Microns

Results for 12 Ångstrom Microroughness: S = – 1. 5 = 1. 0 Microns

Results for 12 Ångstrom Microroughness: S = – 1. 5 = 1. 0 Microns

Scatter due to Contamination (dust) Figure courtesy of Gary Peterson, Breault Research Organization.

Scatter due to Contamination (dust) Figure courtesy of Gary Peterson, Breault Research Organization.

MIL-STD 1246 C The number of particles per square foot with diameters greater than

MIL-STD 1246 C The number of particles per square foot with diameters greater than s microns is given by: log(n) = 0. 926 [ (log(c))2 - (log(s))2 ] s = particle diameter ( m) c = cleanliness level n = number of particles per square-foot with diameters greater than s Courtesy of Gary Peterson, Breault Research Organization.

The Mie Model for 0. 01% Coverage (Level ~230)

The Mie Model for 0. 01% Coverage (Level ~230)

UKIRT Emissivity data

UKIRT Emissivity data

Scatter Versus Time

Scatter Versus Time

Scatter Versus Time: Apache Point Rate of change ≈ 0. 04% per hour!

Scatter Versus Time: Apache Point Rate of change ≈ 0. 04% per hour!

Power Spectral Density Figure courtesy of Gary Peterson, Breault Research Organization.

Power Spectral Density Figure courtesy of Gary Peterson, Breault Research Organization.

Profile of a Star

Profile of a Star