Laser Induced Damage Threshold (LIDT): (S-on-1 test procedure: ISO 11254 – 2) Request/contact person UAB “Altechna” Konstitucijos pr. 23C LT-08105 Vilnius (A. Galinis) Testing institute Testing institute: Tester/date: Vilnius University, Laser Research Center, Saulėtekio al. 10, Vilnius, Lithuania A. Melninkaitis/2011-09-19 Specimen Name of sample: Type of specimen: Storage, cleaning: Notch filter; Filter, AOI=45; Wrapping paper, no cleaning. Test specification Second harmonic of pulsed Nd:YAG NL303 G laser ( = 532 nm, linear polarization S, pulse duration 2,5 ns), /2 plate combined with additional polarizer attenuator, online scattered light damage detection, offline inspection of damage detection using Nomarski microscopy (100x). Laser parameters Wavelength: Angle of incidence: Polarisation state: Pulse repetition frequency: Spatial beam profile in target plane: Longitudinal beam profile: Beam diameter in target plane(1/e2): Pulse duration: 532 nm; 45 deg; linear S; 10 Hz; TEM00; Multimode; 170,2 µm (average from 30 pulses); 2,5 ± 0,4ns; Fig. 1. Spatial beam profile in target plane and pulse duration graph. Test procedure: S-on-1 test Number of sites per specimen: Arrangement of test sites: Minimum distance between sites: Damage detection: Storage of the specimen: Test environment: Cleaning: Definition of LIDT: 456; Equally spaced; 721 m; Scattered light diode; Plastic container; Industrial environment; No; Linear fit to 0% of damage probability; Test result of Notch filter Front surface: LIDT 1-on-1 = 5,55 ± 0,72 J/cm2 LIDT 1000-on-1 = 2,02 ± 0,58 J/cm2 Rear surface: LIDT 1-on-1 = 6,50 ± 0,76 J/cm2 LIDT 1000-on-1 = 4,75 ± 0,69 J/cm2 Fig. 2. Characteristic damage curve. Fig. 3. Typical front surface damage morphology (Energy density 8,68 J/cm2, damage after 1 pulse) Fig. 4. Typical front surface damage morphology (Energy density 4,11J/cm2, damage after 205 pulses) Fig. 5. Typical rear surface damage morphology (Energy density 8,81J/cm2, damage after 1 pulse) Fig. 6. Typical rear surface damage morphology (Energy density 8,88J/cm2, damage after 2 pulses) Technical Note 1 According to the ISO11254-2 norm for spatial beam profiling perpendicular to the direction of beam propagation and angles of incidence differing from 0 degrees, the cosine of the angle of incidence has to be included in the calculation of the effective area. Therefore the beam diameter increase due to the angle of incidence (AOI) is taken into account when calculating the laser fluency. Laser beam area A (1/e2): (Perpendicular to the propagation direction) Sample = 45 deg Area A’= (Area A)/cos()) (projection A’ of area A in the target plane @ 45 deg AOI) Fig. 7.
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