APPARATUS AND SYSTEM FOR A QUASI LONGITUDINAL MODE ELECTRO OPTIC SENSOR FOR HIGH POWER MICROWAVE TESTING

• US 20100264904A1
• Filed: 07/01/2010
• Published: 10/21/2010
• Est. Priority Date: 09/06/2007
• Status: Active Grant

• Current Assignee: US Gov'T Represented By Secretary Of The Navy Chief Of Naval Research
• Original Assignee: US Gov'T Represented By Secretary Of The Navy Chief Of Naval Research
• Inventors: Garzarella, Anthony, Wu, Dong Ho
• Granted Patent: US 8,358,415 B2
• Time in Patent Office: Days
• US Class Current: 324/97
• CPC Class Codes: G01R 29/0885 using optical probes, e.g. electro-optical, luminescent, glow discharge, or optical interferometers
• CPC Class Codes: G01R 31/308 using non-ionising electromagnetic radiation, e.g. optical radiation investigating or analysing materials by the use of optical means G01N21/00; image analysis G06T7/00

Abstract

An apparatus, for measuring an applied electrical field and for reducing perturbation to the electrical field being measured, includes a laser integrated into an electro optic crystal sensor head prior to the output fiber. A probe beam is passed along the crystal direction of low birefringence of nearly circular optical indicatrix, rather than one of high EO modulation. The EO crystal is placed between two crossed polarizers and oriented such that a small tilt angle is subtended between its optic axis and the path of the probe beam. Improved optical coupling is achieved by using a large core multimode fiber at the output, to reduce optical insertion losses. A collimating lens emits the intensity modulated laser beam back to a photodetector, where the intensity modulated laser beam is converted to an electrical signal representing both field strength and phase of the electrical field applied to the sensor head.

Claims

1. An apparatus for measuring an electric field while minimally perturbing the electric field being measured, the apparatus comprising:

a probe beam stage having a laser, wherein the laser emits a laser probe beam passing through an electro optic crystal, having an optic axis, exposed to the electric field;

a sensor head forming an electro optic sensor that detects the electric field, wherein the sensor head is optically coupled to the probe beam stage by a first optical fiber lead, wherein the sensor head includes a holder, wherein residing in the holder is a first polarizer, a second polarizer, and the electro optic crystal between two collimating lenses, wherein the electro optic crystal is disposed in the holder at a tilt angle Theta about the optic axis of the electro optic crystal, such that the tilt angle Theta is subtended between the optic axis and the path of the probe beam; and

a photodetector that receives the laser probe beam and converts the laser probe beam into an electrical signal which is displayed on an RF readout instrument obtaining measurements of the electric field for system warnings, activation of countermeasures, and activation of communications systems, and wherein the photodetector is optically coupled to the sensor head by a second optical fiber lead.

2. The apparatus according to claim 1, wherein the tilt angle Theta has a tilt range of about zero degrees up to about ten degrees, with the same output result within the tilt range of about zero degrees up to about ten degrees.

3. The apparatus according to claim 1, wherein the tilt angle Theta typically operates at a tilt range of less than about one degree and up to about three degrees.

4. The apparatus according to claim 1, wherein the tilt angle Theta provides a stable phase shift in the laser probe beam, which increases optical modulation and field strength sensitivity of the electro optic sensor.

5. The apparatus according to claim 1, wherein the RF readout instrument includes one or more of a digital multi-meter, a specialized network analyzer, a spectrum analyzer, a vector analyzer, a power analyzer and an oscilloscope.

6. The apparatus according to claim 1, wherein the holder is a non-metallic holder.

7. The apparatus according to claim 6, wherein the non-metallic holder is a ceramic holder.

8. The apparatus according to claim 1, wherein the second polarizer integrated into the holder in the sensor head is disposed close to the electro optic crystal at a distance ranging from about zero millimeters to about ten millimeters, and because of the tilt angle Theta of the electro optic crystal, a requirement is eliminated for a plurality of additional optical components.

9. The apparatus according to claim 8, wherein the additional optical components, for which the requirement is eliminated, include:

a quarter wave plate, and an external wave retardation plate thereby reducing a plurality of optical components and insertion losses.

10. An apparatus for measuring an electric field while minimally perturbing the electric field being measured, the apparatus comprising:

a probe beam stage having a laser, wherein the laser emits a laser probe beam passing through an electro optic crystal, having an optic axis, exposed to the electric field;

a sensor head forming a quasi-longitudinal-mode EO sensor that detects the electric field, wherein the sensor head is optically coupled to the probe beam stage by a first polarization maintaining optical fiber lead, wherein the sensor head includes a holder, wherein residing in the holder is a first polarizer, a second polarizer in a crossed-polarization configuration, and the electro optic crystal between two collimating lenses, wherein the electro optic crystal is disposed in the holder at a tilt angle Theta about the optic axis of the electro optic crystal, such that the tilt angle Theta is subtended between the optic axis and the path of the probe beam; and

a photodetector that receives the laser probe beam and converts the laser probe beam into an electrical signal which is displayed on an RF readout instrument obtaining measurements of the electric field for system warnings, activation of countermeasures, and activation of communications systems, and wherein the photodetector is optically coupled to the sensor head by a multi-mode optical fiber lead.

11. The apparatus according to claim 10, wherein the tilt angle Theta typically operates at a tilt range of less than about one degree and up to about three degrees.

12. The apparatus according to claim 10, wherein the tilt angle Theta provides a stable phase shift in the laser probe beam, which increases optical modulation and field strength sensitivity of the electro optic sensor.

13. The apparatus according to claim 10, wherein the multimode fiber and the electro optic crystal disposed in the holder at a tilt angle minimize optical noise.

14. The apparatus according to claim 10, wherein the RF readout instrument includes one or more of a digital multi-meter, a specialized network analyzer, a spectrum analyzer, a vector analyzer, a power analyzer and an oscilloscope.

15. The apparatus according to claim 10, wherein the holder is a non-metallic holder.

16. The apparatus according to claim 15, wherein the non-metallic holder is a ceramic holder.

17. The apparatus according to claim 10, wherein the second polarizer integrated into the holder in the sensor head is disposed close to the electro optic crystal at a distance ranging from about zero millimeters to about ten millimeters, and because of the tilt angle Theta of the electro optic crystal, a requirement is eliminated for a plurality of additional optical components.

18. The apparatus according to claim 17, wherein the additional optical components, for which the requirement is eliminated, include:

a quarter wave plate, and an external wave retardation plate thereby reducing a plurality of optical components and insertion losses.

19. A system for detecting and measuring an applied electric field using a quasi-longitudinal-mode EO sensor, the system comprising:

a probe beam stage having a laser, wherein the laser emits a laser probe beam passing through an electro optic crystal, having an optic axis, exposed to the electric field;

a sensor head forming an electro optic sensor that detects the electric field, wherein the sensor head is optically coupled to the probe beam stage by a first optical fiber lead, wherein the sensor head includes a holder, wherein residing in the holder is a first polarizer, a second polarizer, and the electro optic crystal between two collimating lenses, wherein the electro optic crystal is disposed in the holder at a tilt angle Theta about the optic axis of the electro optic crystal, such that the tilt angle Theta is subtended between the optic axis and the path of the probe beam;

a photodetector that receives the laser probe beam and converts the laser probe beam into an electrical signal which is displayed on an RF readout instrument;

obtaining measurements of the electric field for system warnings, activation of countermeasures, and activation of communications systems, and wherein the photodetector is optically coupled to the sensor head by a second optical fiber lead; and

a computer controller having computer a executable program, and wherein when the computer executable program is executed by the computer controller, the computer executable program causes the computer controller to automatically measure an intensity of the intensity modulated laser probe beam converted into the electrical signal which is displayed on the RF readout instrument obtaining measurements of the electric field for system warnings, activation of countermeasures, and activation of communications systems, and wherein the photodetector is optically coupled to the sensor head by a second optical fiber lead.

20. The system according to claim 19, further comprising a reflecting prism positioned between the electro optic crystal and the second collimating lens, wherein all optical fibers are positioned in the same collinear direction causing the sensor head and all optical fibers to aligned in a wand configuration.