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Stress Birefringence in Optical Glass

Stress birefringence of optical glass: Δn = C(σ₁ − σ₂) and the retardance R = C d (σ₁ − σ₂) for fused silica and twelve Schott glasses, in nm/cm as glass catalogs quote it, with the stress that gives a half-wave retardance.

Model: Textbook approximation

For uniaxial stress (σ₂ = 0), a positive value is tension and a negative one compression.

Stress-optic coefficient C

3.55 ×10⁻¹² Pa⁻¹

Jog 1957 (Filon & Harris), 649.5 nm

Birefringence Δn = C·σ

3.550e-5

signed

Phase Γ = 2πR/λ

3.524 rad

fringe order R/λ = 0.5608

Retardance R in 10 mm

355 nm

signed: flips between tension and compression

Retardance per cm

355 nm/cm

the unit glass catalogs use for stress birefringence

Stress for half-wave retardance

8.915 MPa

R = λ/2 at this thickness and wavelength

Retardance against stress

Glasses at 10 MPa

GlassC (×10⁻¹² Pa⁻¹)R per cm (nm/cm)Source
Fused silica3.55355Jog 1957 (Filon & Harris), 649.5 nm
N-BK72.77277Schott data sheet (N-BK7HT)
N-BAK42.9290Schott data sheet
N-FK51A0.770Schott data sheet
F22.81281Schott data sheet
SF101.95195Schott data sheet
SF111.33133Schott data sheet
N-SF112.94294Schott data sheet
SF60.6565Schott data sheet
N-SF62.82282Schott data sheet
SF570.022Schott data sheet
N-SF572.78278Schott data sheet
N-LASF91.72172Schott data sheet

Click a row to select the glass.

Model

R = C d (σ₁ − σ₂), Γ = 2πR/λ

The principal stress axes are the birefringence axes. C comes from the Schott data sheets (K in 10⁻⁶ mm²/N = 10⁻¹² Pa⁻¹; SF57's 0.02 is the near-zero-K lead glass used for polarization-preserving optics) and from Jog 1957 for fused silica (3.55 at 649.5 nm, rising to 3.75 at 460 nm). The sign of R flips between tension and compression.

Crystals are not listed because they have a stress-optic tensor, so their birefringence depends on the stress and light directions. Liquids carry no static shear stress.

Model and references

Textbook approximation. A standard approximation from the literature (for example paraxial, plane-wave or Gaussian-beam), valid within the range the page states. About the tiers

Linear stress-optic law for isotropic glass at one wavelength (C varies a few percent across the visible; the page warns outside 0.4–2.5 µm). Crystals are not covered: they have a stress-optic tensor, so their birefringence depends on the stress and light directions.

  1. SCHOTT AG (2017). Optical glass data sheets, 2017-01-20: stress optical coefficient K. refractiveindex.info
  2. Jog E. S. (1957). The dispersion of the stress optical coefficient of vitreous silica. J. Indian Inst. Sci. 39(2), 93. Table I. journal.iisc.ac.in
  3. Dally J. W., Riley W. F. (2005). Experimental Stress Analysis, 4th ed. College House Enterprises. Theory of photoelasticity.
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