Editing Electro–optic effect (section)

==Applications==

===Electro-optic modulators===
{{main|Electro-optic modulator}}
Electro-optic [[modulator]]s are usually built with electro-optic crystals exhibiting the [[Pockels effect]]. The transmitted beam is [[Phase modulation|phase modulated]] with the electric signal applied to the crystal. [[Amplitude modulator]]s can be built by putting the electro-optic crystal between two linear [[polarizer]]s or in one path of a [[Mach–Zehnder interferometer]].
Additionally, [[Amplitude modulator]]s can be constructed by deflecting the beam into and out of a small aperture such as a fiber.  This design can be low loss (<3&nbsp;dB) and polarization independent depending on the crystal configuration.

===Electro-optic deflectors===
Electro-optic deflectors utilize [[prism (optics)|prisms]] of electro-optic crystals. The index of refraction is changed by the [[Pockels effect]], thus changing the direction of propagation of the beam inside the prism. Electro-optic deflectors have only a small number of resolvable spots, but possess a fast response time. There are few commercial models available at this time. This is because of competing [[Acousto-optic effect|acousto-optic]] deflectors, the small number of resolvable spots and the relatively high price of electro-optic crystals.

===Electro-optic field sensors===
The electro-optic [[Pockels effect]] in nonlinear crystals (e.g. KDP, BSO, K*DP) can be used for electric field sensing via polarisation state modulation techniques. In this scenario, an unknown electric field results in polarisation rotation of a laser beam propagating through the electro-optic crystal; through inclusion of polarisers to modulate the light intensity incident on a photodiode, a time-resolved electric field measurement can be reconstructed from the obtained voltage trace. As the signals obtained from the crystalline probes are optical, they are inherently resistant to electrical noise pickup, hence can be used for low-noise field measurement even in areas with high levels of electromagnetic noise in the vicinity of the probe. Furthermore, as the polarisation rotation due to the [[Pockels effect]] scales linearly with electric field, ''absolute'' field measurements are obtained, with no need for numerical integration to reconstruct electric fields, as is the case with conventional probes sensitive to the time-derivative of the electric field. 

Electro-optic measurements of strong electromagnetic pulses from intense laser-matter interactions have been demonstrated in both the nanosecond and picosecond (sub-petawatt) laser pulse driver regimes. <ref>{{cite journal|last1=Consoli|first1=F.|last2=De Angelis|first2=R.|last3=Duvillaret|first3=L.|last4=Andreoli|first4=P. L.|last5=Cipriani|first5=M.|last6=Cristofari|first6=G.|last7=Di Giorgio|first7=G.|last8=Ingenito|first8=F.|last9=Verona|first9=C.|title=Time-resolved absolute measurements by electro-optic effect of giant electromagnetic pulses due to laser-plasma interaction in nanosecond regime|journal=Scientific Reports|date=15 June 2016|volume=6|issue=1|pages=27889|doi=10.1038/srep27889|pmid=27301704|pmc=4908660|bibcode=2016NatSR...627889C}}</ref><ref>{{cite journal|last1=Robinson|first1=T. S.|last2=Consoli|first2=F.|last3=Giltrap|first3=S.|last4=Eardley|first4=S. J.|last5=Hicks|first5=G. S.|last6=Ditter|first6=E. J.|last7=Ettlinger|first7=O.|last8=Stuart|first8=N. H.|last9=Notley|first9=M.|last10=De Angelis|first10=R.|last11=Najmudin|first11=Z.|last12=Smith|first12=R. A.|title=Low-noise time-resolved optical sensing of electromagnetic pulses from petawatt laser-matter interactions|journal=Scientific Reports|date=20 April 2017|volume=7|issue=1|pages=983|doi=10.1038/s41598-017-01063-1|pmid=28428549|bibcode=2017NatSR...7..983R|pmc=5430545}}</ref>