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References

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  1. R. D. Deslattes, “Avogadro’s Constant,” Ann. Rev. Phys. Chem. 31, 435 (1980).
    [CrossRef]
  2. R. D. Deslattes, “Reference Wavelengths. Infrared to Gamma Rays, Avogadro’s Constant, Mass and Density,” “Enrico Fermi,” International School of Physics, Course 68, A. FerroMilone et al., Eds. (North-Holland, New York, 1980), p. 93.
  3. A. Peuto, A. Sacconi, “Precision Measurements on Solid Artifacts for a Redetermination of the Water Density,” Natl. Bur. Stand. Spec. Publ. 617 (1984), p. 449.
  4. W. Angele, “Finishing High Precisions Quartz Balls,” Precis. Eng. 2, 119 (1980).
    [CrossRef]
  5. J. Seckold, G. Zosi, “Polishing Silicon Surfaces Strain-Free and Flat to Better than λ/20,” Appl. Opt. 25, 3006 (1986).
  6. Micro Abrasive Co., Westfield, MA.
  7. Model 1, Rank Taylor Hobson, Ltd., Leicester, England.
  8. Tivoli Werke AG, Hamburg, F.R.G.
  9. Union Carbide, Indianapolis, IN.
  10. Imperial Chemical Industries, Sydney, Australia.
  11. R. Panciera, A. Sacconi, “Misure di Rontondità sul Profilo di Campioni di Massa Volumica,” Istituto di Metrologia, Turin, RT-88 (1979).

1986

1984

A. Peuto, A. Sacconi, “Precision Measurements on Solid Artifacts for a Redetermination of the Water Density,” Natl. Bur. Stand. Spec. Publ. 617 (1984), p. 449.

1980

W. Angele, “Finishing High Precisions Quartz Balls,” Precis. Eng. 2, 119 (1980).
[CrossRef]

R. D. Deslattes, “Avogadro’s Constant,” Ann. Rev. Phys. Chem. 31, 435 (1980).
[CrossRef]

Angele, W.

W. Angele, “Finishing High Precisions Quartz Balls,” Precis. Eng. 2, 119 (1980).
[CrossRef]

Deslattes, R. D.

R. D. Deslattes, “Avogadro’s Constant,” Ann. Rev. Phys. Chem. 31, 435 (1980).
[CrossRef]

R. D. Deslattes, “Reference Wavelengths. Infrared to Gamma Rays, Avogadro’s Constant, Mass and Density,” “Enrico Fermi,” International School of Physics, Course 68, A. FerroMilone et al., Eds. (North-Holland, New York, 1980), p. 93.

Panciera, R.

R. Panciera, A. Sacconi, “Misure di Rontondità sul Profilo di Campioni di Massa Volumica,” Istituto di Metrologia, Turin, RT-88 (1979).

Peuto, A.

A. Peuto, A. Sacconi, “Precision Measurements on Solid Artifacts for a Redetermination of the Water Density,” Natl. Bur. Stand. Spec. Publ. 617 (1984), p. 449.

Sacconi, A.

A. Peuto, A. Sacconi, “Precision Measurements on Solid Artifacts for a Redetermination of the Water Density,” Natl. Bur. Stand. Spec. Publ. 617 (1984), p. 449.

R. Panciera, A. Sacconi, “Misure di Rontondità sul Profilo di Campioni di Massa Volumica,” Istituto di Metrologia, Turin, RT-88 (1979).

Seckold, J.

Zosi, G.

Ann. Rev. Phys. Chem.

R. D. Deslattes, “Avogadro’s Constant,” Ann. Rev. Phys. Chem. 31, 435 (1980).
[CrossRef]

Appl. Opt.

Natl. Bur. Stand. Spec. Publ.

A. Peuto, A. Sacconi, “Precision Measurements on Solid Artifacts for a Redetermination of the Water Density,” Natl. Bur. Stand. Spec. Publ. 617 (1984), p. 449.

Precis. Eng.

W. Angele, “Finishing High Precisions Quartz Balls,” Precis. Eng. 2, 119 (1980).
[CrossRef]

Other

R. D. Deslattes, “Reference Wavelengths. Infrared to Gamma Rays, Avogadro’s Constant, Mass and Density,” “Enrico Fermi,” International School of Physics, Course 68, A. FerroMilone et al., Eds. (North-Holland, New York, 1980), p. 93.

Micro Abrasive Co., Westfield, MA.

Model 1, Rank Taylor Hobson, Ltd., Leicester, England.

Tivoli Werke AG, Hamburg, F.R.G.

Union Carbide, Indianapolis, IN.

Imperial Chemical Industries, Sydney, Australia.

R. Panciera, A. Sacconi, “Misure di Rontondità sul Profilo di Campioni di Massa Volumica,” Istituto di Metrologia, Turin, RT-88 (1979).

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Figures (2)

Fig. 1
Fig. 1

Arrangement of cones A and B during final polishing. Cone A rotates around the fixed axis Oo′; cone B, while rotating around the axis Oo″, is driven by the extremity T of an oscillating arm (not shown in the figure). The suspension of titanium dioxide and water is added through the hole Hw; slurry flows out of cone A through the hole Hs. P indicates the pitch ring, and Si is the silicon sphere.

Fig. 2
Fig. 2

Talyrond (10,000 magnification, no filter) diagram indicating a deviation from ideal sphericity ΔR equal to ±75 nm in the worst case. In the diagram, one division represents 0.2 μm.

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