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NeoScan

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[[Image:NEOWEB2.png|thumb|420px|Modulating the polarization state of an optical beam passing through an electro-optic crystal.]]
The operation of the [[NeoScan]] system is based on the Pockels electro-optic effect, which predicts the phase retardation and a change of the polarization state of an optical beam in an electro-optic (EO) crystal due to an impinging electric field. This effect is observed in non-centrosymmetric crystals when an electric field directed along certain crystal axes causes a change in the indices of refraction encountered by an incident optical beam. The electro-optic effect provides a means of modulating the phase or intensity of the optical radiation. It also makes it possible to detect the presence of an electric field impinging on an EO crystal. The polarization state of an optical beam travelling through an EO crystal is altered by the electric field in that crystal. A comparison of the original polarization states of the optical beam before and after interacting with the crystal allows a determination of the amplitude and phase of the impinging RF electric field. Since the electro-optic sensing phenomenon relies on small displacements of the atomic crystal structure, the response time of the process is extremely short. This short response time makes it possible to measure high-frequency electric fields up to the terahertz regime.
 
=== NeoScan Electro-Optic Field Probes ===
A typical EO probe is composed of an optical fiber affixed with an EO crystal, whose bottom surface is coated with a dielectric reflective layer. A low-noise 1550nm laser is used as the optical beam source. The beam is delivered to the optical probe through a fiber-based optical mainframe. The polarization of the beam is modulated by the electric field penetrating the EO crystal tip. The modulated beam is reflected back into the fiber, and back to the mainframe for analysis. The intensity of the output optical beam is linearly proportional to the strength of the external electric field at the probe tip location. This is then converted to an output RF signal by a high-speed photodetector.
 
The equation E=αV is used to calculate the electric field, where α is the calibration factor, or the slope between the electric field E (in V/m) and the measured EO signal V (in V/m/V). For instance, for a calibration factor of 1.082 V/m/V. a measured EO signal of 1000 V (0.001 V), corresponds to and electric field of 1.082 V/m/V  1000 V = 1082 V/m.
 
 
 
Due to its broad measurement bandwidth and high spatial resolution, the EO measurement technique is a promising means to characterize RF systems such as microwave and millimeter-wave integrated circuits and antennas. Unlike the conventional electrical measurement techniques which require some type of metal structure for the resonant detection of an RF signal, [[NeoScan]]’s unique real-time EO electric field measurement method requires no metal components. As a result, the field perturbation caused by introducing the probe tip within the vicinity of a device under test (DUT) is significantly reduced.
The [[NeoScan]] field probes are supplied with polarization maintaining (PM) fibers of certain lengths. The end of the fiber is connected to the [[NeoScan]]'s optical mainframe using an FC/APC fiber connector. Since [[NeoScan]]'s underlying principle of operation is based on the polarization modulation of an optical beam, the use of PM fiber plays a critical role in maintaining the integrity of the sampled field data. Our standard field probes come with fiber lengths of 10m, 20m and 50m. A large standoff distance allows you to place the probe far away from the optical mainframe. This is a significant advantage for probing high power microwave systems or for near-field scanning of high power transmitting phased array antennas.
 
=== Measuring Amplitude and Phase of Polarimetric Fields ===
 
A low noise 1550 nm laser diode is used as optical beam source. The optical connections are fiber-based. The beam is delivered to an optical probe. The polarization of the beam is modulated through an electro-optic crystal on the probe tip.
 
The modulated beam is reflected back into the fiber, and back to the mainframe for analysis. An optical analyzer converts the polarization change of the beam into an amplitude change. The amplitude is linearly proportional to the strength of the external electric field at the probe-crystal location. The equation E=αV is used to calculate the electric field, where α is the calibration factor, or the slope between the electric field E (in V/m) and the measured EO signal V (in V/m/V). For instance, for a calibration factor of 1.082 V/m/V. a measured EO signal of 1000 V (0.001 V), corresponds to and electric field of 1.082 V/m/V  1000 V = 1082 V/m.
Figure 1.3 shows the electric and magnetic fields distribution of a traveling RF wave with a normal probe shown in typical orientation. To detect the maximum electric field in this configuration, the propagation direction of the optical beam of the probe should be parallel to the E-field direction. In general, a normal EO probe is only sensitive to the electric field component parallel to the probe handle, whereas a tangential probe is sensitive to the electric field component perpendicular to the probe handle. Yet, the E-field sensitivity of a tangential probe depends on its crystal orientation sitting on its tip.
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