QPM almost eliminates spatial walk-off between interacting beams, enabling longer interaction lengths and higher conversion efficiency than birefringent phase matching (BPM in single crystals).
Highest effective nonlinear coefficient: PPKTP utilizes the largest nonlinear tensor element (d₃₃ = 16.9 pm/V), approximately three times larger than that of bulk KTP in birefringent phase matching.
Broad phase-matching range: Customizable frequency conversion across the entire KTP transparency range (350–4000 nm) by selecting the appropriate poling period, without the wavelength limitations of birefringent phase matching.
Superior thermal stability: PPKTP exhibits much lower temperature sensitivity than PPLN (3 μm/°C versus 52 μm/°C), enabling stable operation in fluctuating thermal environments.
High damage threshold: Laser-induced damage threshold of 600 MW/cm² (with coating) at 1064 nm for 10 ns pulses, suitable for high-power and high-energy applications.
Low photorefractive damage: Compared with PPLN and other ferroelectric crystals, PPKTP shows superior resistance to photorefractive effects, allowing room-temperature operation.
Lower coercive field: The coercive voltage for domain reversal in KTP is only about one-tenth that of LiNbO₃, facilitating the fabrication of thicker periodically poled wafers (up to 3 mm) for large-aperture, high-power devices.
Typical Specifications
Chemical formula: KTiOPO₄ (KTP)
Crystal structure: Orthorhombic, space group Pna2₁; ferroelectric multiple domains
Surface flatness: λ/6 @ 633 nm, Convex or Concave faces are available.
Operating temperature: 20-200 ℃ (customizable)
Coating options: AR/AR, AR/HR-PR, DBAR, TBAR, IAD or IBS (extra-cavity or intra-cavity)
Main Applications
Spontaneous parametric down-conversion (SPDC): PPKTP is the leading crystal for generating entangled photon pairs for quantum communication, quantum key distribution (QKD), and quantum imaging; Type-0 and Type-II configurations are available for polarization-entangled and energy-time-entangled sources.
Squeezed light generation: Used in optical parametric oscillators for continuous-variable quantum information, quantum-enhanced metrology, and gravitational-wave detection; PPKTP offers high nonlinearity and low loss for sub-shot-noise measurements.
Second-harmonic generation (SHG): Efficient frequency doubling for green and blue light generation; a bow-tie ring resonator with PPKTP achieved efficient 480 nm blue-light generation. PPKTP has demonstrated SHG conversion from 1319 nm to 659.5 nm.
Optical parametric oscillators and amplifiers (OPO/OPA): Tunable visible and near-infrared generation (680–2000 nm) with green pump sources; PPKTP enables compact, efficient OPO designs without walk-off limitations.
Quantum frequency conversion: Interfaces between different quantum systems and telecom wavelengths for quantum repeater and quantum network architectures.
Heralded single-photon sources: PPKTP-based SPDC produces high-purity heralded single photons for quantum sensing and ultra-sensitive temperature measurement.
Backward-wave OPO (BWOPO): Counter-propagating signal and idler waves enable cavity-free, compact, and robust OPO configurations with demonstrated efficiency >70%.
Chirped and aperiodic poling: For broadband or tailored spectral characteristics, including removal of spectral side lobes for enhanced spectral purity in quantum applications.