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Table 1

Intrinsic phase retardation of high reectivity mirrors. R is the reported reflectivity, F is the correspond-ing finesse, Δ their retardation, Nm the number of mirrors of the measured set, and Λ the wavelength used. The sym- bol † indicates data already reported in [6]

Ref. R F × 10−3 δ(rad) Nm λ(nm)
[1] 0.99 0.3 2.3×10-3 1 633
[17] 0.998 1.6 (3.±1)×10-4 17
<10-6 2 05
[18] 0.996 0.8 (12.5±9.5)×10-5 5 514
[8] 09983 1.8 (4.6±)×10-4 1 633
[19] 0.999524 6.6 (2.7±1.7)×10-6 2 633
[20] 0.9895 0.3 1.2×10-3 1 633
[21] 0.999975 126 3×10-6 1 540
[22] 0.9988 2.6 (7.3±3.1)×10-7 2 633
[23] 0.999969 101 (15.7±8.3)×10-7 3 ()1064
<10-7 1
[24] 0.999923 41 1.8×10-6 1 633
[25] 0.999963 85 (3.0±0.1)×10-6 2 575
[26] 0.99994 52 (5.2±0.4)×10-6 2 1312
[27] 0.999991 349 (5.8±4.2)×10-7 2 1652
[6] 0.999396 5.2 (4.6±0.3)×10-4 2 1064
0.999972 112 (4.5±0.2)×10-6 3
[28] 0.999987 242 (9.6±0.4)×10-7 2 413
[29] 0.9999935 483 (7.1±0.1)×10-7 2 1064
[30] 0.9999959 766 (7.1±)×10-6 2 1064
[31] 0.999991 349 (2.96±0.02)×10-6 2 1064
[32] 0.9999895 299 (2.85±0.1)×10-6 2 1064
0.999836 19 (1.43±0.56)×10-6 1
[7] 0.999850 21 (2.93±0.13)×10-6 1 633
0.999853 21 (6.87±0.36)×10-6 1

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