Measuring pulses requires the use of certain materials such as silica. A measurement system must have at least one material to obtain a nonlinear effect. T he materials in the measuring system, unfortunately, could cause chirp in the pulse and stretch the pulse to be measured. Although chirp from the materials in a system is generally negligible in long pulses, it is not for some short pulses. Therefore, one must be mindful of the materials used in a measuring system. The table below shows how much chirp is introduced by materials and how much pulses are stretched by the materials.
Transform limited pulse length at 800nm | 10fs | 25fs | 100fs | |
Bandwidth FWHM | 80nm | 32nm | 8nm | |
10mm fused silica | Chirp | 361fs^2/rad | ||
Stretched pulse length | 85fs | 36fs | 102fs | |
Error (%) | 300 % | 44 % | 2 % | |
10mm BK7 | Chirp | 446fs^2/rad | ||
Stretched pulse length | 248fs | 102fs | 103fs | |
Error (%) | 952% | 308% | 3 % | |
1mm BBO crystal | Chirp | 75fs^2/rad | ||
Stretched pulse length | 43fs | 30fs | 100.1fs | |
Error (%) | 132% | 20% | 0.1% |