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  1. H. E. Bennett, J. O. Porteus, J. Opt. Soc. Amer. 51, 123 (1961).
    [CrossRef]
  2. H. Davies, Proc. Inst. Elec. Engrs. 101, 209 (1954).
  3. K. E. Torrence, “Monochromatic Directional Distribution of Reflected Thermal Radiation from Roughened Dielectric Surfaces,” M.S. Thesis, University of Minnesota (1964).
  4. H. E. Bennett, “Influence of Surface Roughness, Surface Damage, and Oxide Films on Emittance,” in Symposium on Thermal Radiation of Solids, NASA SP-55 (Govt. Printing Office, Wash., D.C., 1964), pp. 145–152.

1961 (1)

H. E. Bennett, J. O. Porteus, J. Opt. Soc. Amer. 51, 123 (1961).
[CrossRef]

1954 (1)

H. Davies, Proc. Inst. Elec. Engrs. 101, 209 (1954).

Bennett, H. E.

H. E. Bennett, J. O. Porteus, J. Opt. Soc. Amer. 51, 123 (1961).
[CrossRef]

H. E. Bennett, “Influence of Surface Roughness, Surface Damage, and Oxide Films on Emittance,” in Symposium on Thermal Radiation of Solids, NASA SP-55 (Govt. Printing Office, Wash., D.C., 1964), pp. 145–152.

Davies, H.

H. Davies, Proc. Inst. Elec. Engrs. 101, 209 (1954).

Porteus, J. O.

H. E. Bennett, J. O. Porteus, J. Opt. Soc. Amer. 51, 123 (1961).
[CrossRef]

Torrence, K. E.

K. E. Torrence, “Monochromatic Directional Distribution of Reflected Thermal Radiation from Roughened Dielectric Surfaces,” M.S. Thesis, University of Minnesota (1964).

J. Opt. Soc. Amer. (1)

H. E. Bennett, J. O. Porteus, J. Opt. Soc. Amer. 51, 123 (1961).
[CrossRef]

Proc. Inst. Elec. Engrs. (1)

H. Davies, Proc. Inst. Elec. Engrs. 101, 209 (1954).

Other (2)

K. E. Torrence, “Monochromatic Directional Distribution of Reflected Thermal Radiation from Roughened Dielectric Surfaces,” M.S. Thesis, University of Minnesota (1964).

H. E. Bennett, “Influence of Surface Roughness, Surface Damage, and Oxide Films on Emittance,” in Symposium on Thermal Radiation of Solids, NASA SP-55 (Govt. Printing Office, Wash., D.C., 1964), pp. 145–152.

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Figures (1)

Fig. 1
Fig. 1

Reflected energy vs σ0/λ.

Tables (1)

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Table I Mechanical and Optical Roughness Values

Equations (2)

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R = R o exp [ - ( 4 π σ o ) 2 / λ 2 ] + R o [ ( 2 5 π 4 ) / m 2 ] ( σ o / λ ) 4 ( Δ θ ) 2 .
R R o = exp [ - ( 4 π σ o / λ ) 2 cos 2 θ ] + 2 5 π 3 m 2 ( σ o λ ) 4 cos 3 θ Δ ω ,

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