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Brewster windows are critical uncoated optical components in high-power laser systems, enabling zero‑reflection-loss transmission for p‑polarized light at Brewster's angle while suppressing s-polarized light. This paper reviews the working principle, material selection, angle tolerance control, surface quality specifications, and typical applications of Brewster windows for high‑power lasers, providing a complete design framework for high-efficiency, high‑damage‑threshold laser cavities.

In high-power laser resonators, minimizing insertion loss and ensuring polarization purity are essential. A Brewster window is a tilted plane parallel plate mounted at Brewster's angle to the optical axis. It eliminates reflective loss for p-polarized light without coatings, suppresses s-polarized light via selective reflection, and improves beam polarization purity and output stability.
Brewster windows operate based on Brewster’s angle and Fresnel equations.
● When light is incident at Brewster's angle θ_B, the reflected beam is purely s-polarized, and p-polarized light has zero reflectance and fully transmits.
● The reflected and refracted beams are mutually perpendicular.
● Brewster's angle formula:θ_B = arctan(n)where n is the refractive index of the window material.
● For fused silica (n≈1.46@633 nm), θ_B≈55.57°.
● For ZnSe (n≈2.4@10.6 μm), θ_B≈67.4°.
In a laser cavity, multiple round trips strongly attenuate s-polarized light, resulting in high-purity linearly polarized output.
Key requirements: high laser-induced damage threshold (LIDT), low absorption, wide transparency, good thermal conductivity, and stable mechanical properties.
● Transparency: 185 nm–2.1 μm
● n≈1.46; θ_B≈55.57°
● High LIDT, low fluorescence, low thermal expansion
● Preferred for solid-state, fiber, and ultrafast lasers
● Transparency: 350 nm–2.0 μm
● n≈1.51; θ_B≈56.5°
● Good polishability and low cost
● Used for low-to-medium power systems
● Transparency: 0.5 μm–22 μm
● n≈2.4@10.6 μm; θ_B≈67.4°
● High IR transmission
● Standard for CO₂ high-power lasers
● High hardness, thermal conductivity, and LIDT
● Used in extreme high-power and harsh environments
Angle error directly degrades p-polarization transmittance and increases loss.
● Angle tolerance: ≤±0.1° for high-power systems
● Parallelism: ≤5–10 arcseconds to avoid beam deflection
● Tilt error >0.5° causes noticeable reflection loss and reduced polarization purity
High-power laser demands strict surface quality to avoid scattering, absorption, and damage.
● Laser grade: 10–5 or 20–10 scratch-dig
● Minimizes particle-induced damage
● ≤ λ/10 @ 632.8 nm over clear aperture
● Preserves wavefront quality
● 90% of the minor axis
● Ensures full beam passage
● Fine ground edges for mechanical stability
● Uncoated for highest LIDT; optional hydrophobic film for contamination resistance
Used in He–Ne, CO₂, solid-state, and fiber lasers to generate linearly polarized output with low loss.
Reduces reflective loss and thermal lensing in high-power transmission systems.
Improves polarization extinction ratio in scientific and industrial setups.
Fused silica Brewster windows support high-peak-power, ultrafast systems.
● Principle: θ_B = arctan(n); p-polarization transmits with zero reflection loss.
● Materials: fused silica (UV–NIR), ZnSe (IR), BK7 (general purpose).
● Tolerance: angle ±0.1°, parallelism ≤10 arcsec.
● Surface: 10–5 scratch-dig, flatness ≤λ/10.
● Applications: laser cavities, beam delivery, polarization control.
Brewster windows are indispensable in high-power laser systems. Proper design—material choice, tight angle tolerance, and laser-grade surface specs—ensures low loss, high damage threshold, and stable polarization output. They will remain key in advanced high-power laser development.

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