Abstract:
An electromagnetic radiation emitter which utilizes a precompensator, pulsed light signal, optical fiber cable, and a terahertz radiation generator. The present invention incorporates an optical precompensator to correct for the stretching of an optical signal as it travels through an optical fiber cable. The dispersion characteristics of the precompensator will be equal and opposite to the dispersion characteristics of the optical fiber cable, maintaining the fidelity of optical pulses as they travel through and exit the optical fiber cable striking a device that generates terahertz electromagnetic radiation.

Description:
RELATED APPLICATIONS 
     The present application claims priority to U.S. Provisional Patent Application Serial No. 60/079,590 filed on Mar. 27, 1998. 
    
    
     BACKGROUND OF THE INVENTION 
     The present invention relates to a precompensator to correct the dispersive effects of optical fiber. More specifically the present invention relates to a terahertz electromagnetic radiation emission and detection system that utilizes a precompensator, optical fiber, and pulsed laser. 
     In the present invention extremely short optical pulses in the femtosecond range generated by a laser are transferred from a laser to a terahertz generator by way of an optical fiber cable. The terahertz generator is comprised of a material that, when illuminated with a short optical pulse, generates electromagnetic radiation in the terahertz range (10 GHz to 50 THz). These materials fall principally into two large categories, photoconductive terahertz generators and non-linear optical generators. In the former category the incident photons generate electrical carriers, both holes and electrons, which are then accelerated by a voltage potential within the material that is either externally applied or internally present due surface potentials in semiconductors. This charge motion in turn generates an electromagnetic field that normally consists of a single or half-cycle of radiation in the terahertz range. The second category of THz generators consists of materials that utilize non-linear optical methods to generate THz radiation. These materials have a non-linear susceptibility, χ (2) , χ (3) , or χ (4)  that causes the input optical pulse to generate a polarization state due to the equation: 
     
       
           P   NL =χ (i) ( E ) i   
       
     
     Where P NL  is the non-linear polarization state of the material, and E is the electrical field of the incident optical pulse. This method is known by a number of names to describe the various physical processes taking place. Some of the effects known to occur are, the inverse Franz-Keldysh effect, electric-field-induced optical rectification, the Stark effect, and Cherenkov radiation. This effect will heretofore be referred to as optical rectification since the scientific literature generally accepts this term to encompass all of the effects. 
     In order to successfully deliver high contrast, sub-100 femtosecond pulses from a laser, one must effectively control the dispersion in an optical fiber through the use of a precompensation device. Dispersion is the spreading and/or distortion of a light pulse as it travels down the length of an optical fiber. Different wavelengths or colors of light travel at different velocities through a fiber, which tends to widen an optical pulse. This phenomena result from the non-linear frequency dependence of the refractive index of silica used in optical fibers. For a more detailed description with respect to optical dispersion see Steven John Kane, “High-Order-Dispersion Control for the Amplification and Compression of Femtosecond Laser Pulses” (1997) (Ph.D. dissertation, University of Michigan (Ann Arbor)) and James VanHartness Rudd, “Advanced Techniques for the Amplification of Sub-100-femtosecond Pulses in Ti:Sapphire-Based Laser Systems” (1996) (Ph.D. dissertation, University of Michigan (Ann Arbor)). 
     The dispersion of light leads to a potential corruption of the terahertz signal. The problem can be corrected by precompensating the signal for any stretching caused by the material dispersion characteristics of a fiber optic cable. An optical pulse may be given dispersion characteristics that are equal and opposite to the dispersion generated by an optical fiber, allowing the exact reconstruction of a pulse as it exits the optical fiber. 
     The present invention is concerned with the generation of terahertz electromagnetic radiation by a pulsed laser in a commercially packaged system. In previous applications such as in a lab environment a laser can be pointed directly through space at an optical switching element with negligible dispersive effects. To allow the commercial use of such a system the present invention must be industrially hardened and packaged. A laser pulse in a room environment may be deflected by objects or people and will suffer degradation from atmospheric effects, unacceptable conditions in an industrial environment. By incorporating an optical fiber cable into the present invention, the laser light is given a predetermined path of travel and allows the present invention to be precisely aligned, ruggedly seated, and bundled into compact form. Given the need for an optical fiber cable to package the system the problem of dispersion now exists, necessitating a precompensation device to maintain the fidelity of the optical pulses traveling through the optical fiber cable. 
     Further objects, features and advantages of the invention will become apparent from a consideration of the following description and the appended claims when taken in connection with the accompanying drawings. 
     SUMMARY OF THE INVENTION 
     The present invention is an electromagnetic radiation emitter which utilizes a precompensator, pulsed light signal, optical fiber cable, and a photoconductive element or an element that exhibits optical rectifiction to generate high frequency electromagnetic radiation in the terahertz range. The present invention incorporates an optical precompensator to correct for the stretching of an optical signal as it travels through an optical fiber cable. The dispersion characteristics of the precompensator will be equal and opposite to the dispersion characteristics of the optical fiber cable, maintaining the fidelity of optical pulses as they travel through and exit the optical fiber cable striking a photoconductive or electro-optic element to generate terahertz electromagnetic radiation. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG. 1 is a diagrammatic view of a terahertz electromagnetic radiation emission and detection system; 
     FIG. 2 is a diagrammatic view of a Treacy grating pair precompensator; 
     FIG. 3 is a diagrammatic view of a three-bounce grating precompensator; 
     FIG. 4 is a diagrammatic view of a grism pair precompensator; 
     FIG. 5 is a diagrammatic view of a hybrid grating-prism pulse precompensator; and 
     FIGS. 6 a  and  6   b  are diagrammatic views of the photoconductive elements used in one embodiment of the present invention. 
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT 
     FIG. 1 is a diagrammatic view of a terahertz electromagnetic radiation emission and detection system shown generally as  10 . An optical source  12  comprising a Ti:sapphire laser producing sub-100 femtosecond pulses at 800 nm is coupled to a precompensator  14 . Although a Ti:sapphire laser is the preferred optical source  12  other short pulse sources may be used such as: a modelocked Er-doped fiber laser frequency doubled to produce pulses at 750-800 nm; a colliding- pulse modelocked (CPM) laser; an amplified Ti:sapphire laser consisting of a seed pulse that is amplified to higher energies; a frequency-doubled, modelocked Nd based glass laser; a modelocked laser based on any of the chromium doped hosts: LiCaF, LiSrAlF, or LiSrGaAlF; or any laser source producing femtosecond output pulses at megahertz repetition rates but is not limited to such. 
     In order to achieve a transform-limited pulse at the output of single mode optical fibers  18  and  19 , a precompensator  14  adds dispersion of a sign opposite to the dispersion acquired in the fibers. Dispersion is the name given to the property of group velocity variation with wavelength. This will tend to spread, stretch, and/or distort an optical pulse shape, making it indistinct. The simplest form of dispersion comes from the propagation of light through bulk material. The source of this dispersion is the non-linear frequency-dependent index of refraction. It is one of the goals of the present invention to exactly or in the least closely reproduce the original optical pulse entering the optical fiber at the exit of the optical fiber. 
     The physical origin of the index of refraction and its consequent frequency-dependent nature are resonances in the material structure. Most optical materials have a strong resonant absorption in the ultraviolet portion of the spectrum and another in the mid infrared that leads to group velocity dispersion (GVD) being positive in the ultraviolet and visible portion of the spectrum and negative in the near-infrared portion of the spectrum. GVD is related to the second derivative of the index of refraction with respect to wavelength. Positive GVD is the condition where longer wavelength light packets will travel faster through the optical fiber than shorter wavelength light packets. Negative GVD is the opposite condition, shorter wavelength light packets will travel faster through the optical fiber than longer wavelength light packets. The preferred wavelength of the optical source generating the sub-100 femtosecond optical pulses is 600-900 nanometers. At these wavelengths the single mode optical fiber we will be using has positive GVD. To counteract the positive GVD of the optical fibers  18  and  19  a precompensator  14  having a negative GVD is incorporated into the system  10 . 
     The precompensator  14  may consist of numerous embodiments having a negative GVD. The precompensator  14  may be comprised of prisms, gratings, grisms, Bragg-fiber gratings, Gires-Tournier interferometer, or any other combination thereof that results in a negative group-velocity dispersion system. 
     A prism pair is a dispersive device and may be used to provide negative GVD for an optical pulse. A prism disperses light because its geometry causes light of different wavelengths passing through it to separate and deviate by different amounts. Although the materials used to make prisms generally have positive dispersion it has been found that with proper ingenuity one can fashion a system that provides either positive or negative GVD. Making different portions of the pulse spectrum traverse different amounts of glass, thus effectively changing their relationship in the pulse does this. 
     Diffraction grating systems are devices that may be used to add either negative or positive GVD to an optical pulse. We will concern ourselves only with those systems that provide negative GVD. A Treacy grating pair with parallel gratings  34  is shown generally as  32  in FIG.  2 . Incident light  36  enters the grating pair and exits as negatively dispersed temporally and spatially distributed light  38 . In a typical Treacy grating pair system the light  38  is retroreflected back on itself to double the dispersive power and recombine the laser beam. Its GVD may be defined as:          G                 V                 D     =     -         λ   3          N   2        G       π                   c   2          cos   3        θ                                
     where N is equal to the groove density, λ is equal to the wavelength of light, G is equal to the distance between the gratings, and c is equal to the speed of light. Since all diffracted angles θ will be between ±90° the GVD will be negative no matter what wavelength or grating is used. Transmission gratings are shown but reflection gratings will work in the same manner. Gratings of this type can be used to offset the positive GVD encountered in up to ten meters of optical fiber. The length of fiber is limited by the residual high-order dispersion that it caused by this style of grating system. This higher-order dispersion, typically referred to as third-order dispersion, causes the output pulse to be a distorted version of the input. The optimal Treacy grating pair is used at a Littrow input angle. This condition is met when the incident angle is equal to the diffracted (output) angle. Most gratings can achieve their highest efficiency at this angle. 
     A second grating design utilizing a first and second grating to introduce negative GVD on an optical pulse is shown generally as  60  in FIG.  3 . The second grating  62  has a groove spacing d which is one-half of that of the first grating  64  (it&#39;s groove density is twice that of the first grating). Therefore, the second grating  62  can be made more efficient owing to its higher groove density. The second grating  62  is depicted as a reflection grating, though it could be a transmission grating. This system works when the incident light  66  hits the first grating  64  at normal incidence. The diffracted light from the first grating  64  obeys the equation:          sin                   θ   d     (   1   )         =     -     λ     d   ′                                
     and this diffracted angle θ (1)   d  becomes the incident angle on to the second grating: 
      θ i   (2) =θ d   (1)   
     The light diffracted from the second grating is governed by:          sin                   θ   d     (   2   )         =       -       2      λ     d       +     sin                   θ   i     (   2   )                                  
     which, after substitution, becomes: 
     
       
         θ d   (2) =−θ i   (2)   
       
     
     Therefore, every ray satisfies the Littrow condition where the input angle equals the output angle and diffracts back on top of itself. This compressor therefore requires only a total of three bounces off gratings  62  and  64  to generate the required GVD thus providing a more efficient method of compensating for positive GVD in a fiber. This system has the same amount of GVD and third order dispersion as a Treacy grating pair used at normal incidence as long as the groove density of the first grating  64  is the same as the groove density in the Treacy gratings  34 . However, since the first grating must be used at normal incidence, this arrangement causes more 3 rd -order dispersion for an equivalent amount of GVD as compared to a Treacy pair used at Littrow incidence angle. 
     The preferred embodiment of the precompensator  14  is a grism pair shown generally as  40  in FIG. 4. A grism is a dispersive optical element that has physical characteristics of both a prism and a grating. The grisms  42   a  and  42   b  used in the present invention are comprised of prisms  43   a  and  43   b  with gratings  44   a  and  44   b  adjacent to the surfaces of the prism  43   a  and  43   b.  Dispersively, a grism acts like a grating with a high dielectric on one side. The equation for the GVD due to a grism is the same as for a regular grating pair. However, the angle θ has a different relationship with the input angle θ i  given by the grating equation: 
       n  sin θ i   = mλN +sin θ D   
     where n=index of refraction, λ=wavelength, N=groove density, and m=diffraction order (usually ±1). The advantage of the grism pair comes from the higher-order dispersive characteristics. In order to compensate properly for the dispersion introduced by a fiber one needs to compensate not only for GVD but also for the higher order dispersive terms. These higher-order terms can be ignored for short lengths of fiber (&lt;10 meters), but start to dominate the pulse shape when trying to compensate the dispersion encountered in longer lengths of fiber. The grisms can be designed for such an application. In the present invention the grisms  42   a  and  42   b  are configured to generate a negative GVD and positive third order dispersion in order to compensate exactly for the optical fiber&#39;s positive GVD and negative third order dispersion. This is in contrast to the Treacy pair of gratings which generate negative GVD and negative third-order dispersion. Grisms with 1000 lines/mm, an index of refraction of 1.7, and an angle of incidence of 66.7° (λ=800 nm) may compensate for optical fibers up to a kilometer in length. 
     Referring to FIG. 4, the operation of the grism pair  40  is demonstrated. An incident light ray  46  travels through the first grism  42   a  and is diffracted. The diffracted beam  48  then travels through the second grism  44   a  and is recollimated. Due to the optical path length as a function of wavelength being nonlinear, the pair provides dispersion. In the present invention the light pulse  50  is then retroreflected back through the two grisms  42   b  and  42   a  and exits the grism pair  40  on the same path it entered in its original form  46 . Once this light is separated from the input it is then focused into an optical fiber for transmission. 
     Additional negative dispersive elements may include a Gires-Tournois interferometer, hybrid grating-prism precompensator and a Bragg-Fiber grating system. A hybrid grating-prism precompensator generally shown as  80  in FIG. 5 is a combination of gratings  82 , mirrors  84 , and prisms  86 . The dispersion of the hybrid system  80  can be modified by changing the characteristics of any of its components. In particular the third-order dispersion can be controlled independently of the GVD by adjusting the spacing of the prisms  86 . A Bragg-Fiber grating utilizes a multilayer construct with varied depth grading between layers to reflect different wavelengths of light at different depths. Since specific wavelengths of light are reflected at only certain depths, these wavelengths of light will travel disparate distances creating both GVD and third-order dispersion. With proper construction Bragg-Fiber gratings are able to perfectly compensate for dispersion seen in long lengths of optical fiber. 
     The exact precompensation characteristics of any of the cited precompensation devices may be configured to match the dispersive characteristics of multiple fiber lengths and materials. For example, the spacing of the grating precompensation devices may be varied to change the dispersion of the gratings. 
     Referring to FIG. 1, after the optical pulse is stretched or precompensated by precompensator  14  and split by fiber splitter  15  it will enter optical fibers  18  and  19 . Optical fibers  18  and  19  can comprise numerous commercially available single mode fibers. In the preferred embodiment optical fibers  18  and  19  with a length up to a thousand meters long can be compensated for. As the optical pulse exits the optical fiber  18  it will strike a terahertz transmitter, which will emit a single-cycle or half-cycle of electromagnetic radiation. The preferred embodiment employs a photoconductive element as the terahertz transmitter, generating electron-hole pairs and an impulse electrical current. The photoconductive element may be a pn-junction diode, pin photodiode, metal-semiconductor-metal photodiode, point-contact photodiode, heterojunction photodiode, or a simple semiconductor, which can be fabricated with any semiconductor element comprised of low temperature grown GaAs (LT-GaAs), Semi-insulating-GaAs, Silicon (crystalline or ion-implanted) on Sapphire (SOS), InP, InGaAs, or any other photoactive element but is not limited to such. The photoconductive element used to generate a terahertz pulse can also be of the kind outlined in U.S. Pat. No. 5,420,595 entitled “Microwave Radiation Source” which issued to Zhang et al. on May 30, 1995, and is incorporated by reference herein. The physics governing this latter style of device concerns both photoconductive and non-linear optical physics and is covered in the article by B. I. Greene, et al, “Far-Infrared Light Generation at Semiconductor Surfaces and Its Spectroscopic Applications,”  IEEE J. Quantum Electron.,  vol. 28, pp. 2302-2312, 1992. This latter-style terahertz transmitter can work with either an externally applied electric field or an induced surface field due to the semiconductor-air interface. This style of internal field can also be due to a semiconductor-semiconductor or metal-semiconductor boundary. This induced field is perpendicular to the surface of the material, so that in order for any terahertz radiation to be radiated into free space, the incident optical pulse must strike the material at a non-zero incidence angle. 
     The optical pulse striking the photoconductive element will generate a current pulse. The variation in current will generate electromagnetic radiation. The temporal shape of the electromagnetic radiation is determined both by the shortness of the input optical pulse and the metal antenna structure that is coupled to the photoconductive element. In the preferred embodiment the antenna is in a dipole configuration. The antenna configuration for this preferred embodiment is outlined in U.S. Pat. No. 5,729,017, “Terahertz Generator and Detector” which issued to Brenner et al. on May 17, 1998, and is incorporated by reference herein. The radiation in the preferred mode will be from 50 gigahertz to 5 terahertz, but any electromagnetic frequency above or below this preferred range is possible. 
     An example of a transmitting element  90  having a photoconductive element is shown in FIG. 6 a.  A bias  104  is applied to a bias electrode  92  that is coupled to a dipole antenna  98 . The dipole antenna  98  serves as the radiation emitter and the photoconductive gap at the center of the dipole antenna  98  is where carriers are generated. An ultrashort laser pulse in the femtosecond range will strike the focus spot  100  located in the gap  102  between the dipoles shorting the bias electrodes through the dipole antenna  98 . The dipole antenna  98  thereby radiates electromagnetic energy in the terahertz range. Suitable electrodes can be made of 0.5 micron thick gold with linewidths from 1 micron to 100 microns separated by a gap of 5 to 100 μm depending on what wavelength radiation is preferred, although they are not limited to such. 
     As outlined in U.S. Pat. No. 5,710,430, “Method and Apparatus for Terahertz Imaging,” which issued to Martin Nuss on Jan. 20, 1998, and is incorporated by reference herein, certain materials and objects can be characterized by a frequency-dependent absorption, dispersion, and/or reflection of terahertz transients which pass through, or reflect off, a sample. The electromagnetic radiation receiver  20  in FIG. 1 is configured to detect electromagnetic radiation in the terahertz range, after being conditioned by a sample. The receiver can be placed at any position surrounding a sample, so as to detect absorbed, reflected, refracted or scattered radiation. The electromagnetic radiation receiver  20  will then generate an electrical signal, which is interpreted, scaled, and/or digitized by any known data acquisition system. The receiver  20  is synchronized to the transmitter  16  by optical pulses traveling through optical fiber  19 . 
     FIG. 6 b  is a diagrammatic drawing of the terahertz-receiving element  110 . In the preferred embodiment, the terahertz-receiving element  110  is an identical structure to the transmitting element  90  except for the absence of a bias voltage. In other structures the material making up the receiver can be either photoconductive (LT-GaAs, SOS, LT-InGaAs) or electro-optic (ZnTe, GaP, LiNbO 3 ). The receiving element  110  is connected to an amplifier  112 , which enables the received terahertz radiation to be examined. 
     It is to be understood that the invention is not limited to the exact construction illustrated and described above, but that various changes and modifications may be made without departing from the spirit and scope of the invention as defined in the following claims.