Abstract:
A device comprising a single photon generator and a waveguide, wherein a single photon generated by the single photon generator is coupled to the waveguide

Description:
FIELD  
       [0001]     The invention relates to the field of photons nanotechnology, and more specifically, to a new and useful method for coupling a single photon to a waveguide.  
       BACKGROUND  
       [0002]     Nanotechnology and quantum information technology are emerging branches of science that involve the design of extremely small electronic and optical circuits that are built at the molecular level. Traditional opto-electronic circuits are fabricated using semiconductor wafers to form chips. Circuits are etched into the semiconductor wafers or chips. The etching process removes material from certain regions or layers of the chips. In contrast, nanotechnology generally deals with devices built upward by adding material, often a single atom at a time. This technique results in a device where every particle could have a purpose. Thus, extremely small devices, much smaller than devices formed by etching, are possible. For example, a logic gate could be constructed from only a few atoms. An electrical conductor can be built from a “nanowire” that is a single atom thick. A bit of data could be represented by the presence or absence of a single proton.  
         [0003]     Quantum information technology provides a new avenue for creating smaller and potentially more powerful computers. Scientific theories such as quantum superposition and quantum entanglement are now being used to explore the possibility of creating smaller, more powerful computing devices. The development in this field has lead to the use of light particles, or photons, to convey information. Light has the ability to be polarized into various states (e.g., horizontally polarized, vertically polarized). Exploiting this property allows a single photon to represent a single quantum bit of information.  
       SUMMARY  
       [0004]     A method and apparatus for coupling a single photon to a waveguide is provided. In an illustrative implementation, a device comprising a single photon generator and waveguide is provided wherein a single photon generated by the single photon generator is coupled to the waveguide. 
     
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0005]     For the purpose of illustrating the invention, there is shown in the drawings one exemplary implementation; however, it is understood that this invention is not limited to the precise arrangements and instrumentalities shown.  
         [0006]      FIG. 1  illustrates a nanowire laser in accordance with an exemplary embodiment of the invention.  
         [0007]      FIG. 2  illustrates a nanowire laser coupled to a waveguide in accordance with an exemplary embodiment of the invention.  
         [0008]      FIG. 3  illustrates a nanowire laser coupled to a waveguide in accordance with an exemplary embodiment of the invention.  
         [0009]      FIG. 4  illustrates a nanowire laser coupled to a waveguide in accordance with an exemplary embodiment of the invention.  
         [0010]      FIG. 5  illustrates a nanowire laser coupled to a waveguide in accordance with an exemplary embodiment of the invention.  
         [0011]      FIG. 6  illustrates a nanowire laser coupled to a waveguide in accordance with an exemplary embodiment of the invention. 
     
    
     DETAILED DESCRIPTION  
       [0000]     Overview  
         [0012]     The use of quantum bits provides researchers with significant potential advancements in computing technology. The ability to understand and utilize the theories of photon superposition and entanglement to generate information is a new field around which there is significant interest. However, one important issue that surrounds potential use of photons as quantum bits is the need to generate a photon on demand at the location where it is desired.  
         [0013]     Generating a usable photon is essentially a two step process. First, a system or element is needed that will emit a photon on demand. Recent advances have been made in this area by using electrically driven or optically driven quantum dots. Quantum dots are capable of generating a single photon when excited by an electrical charge or an optical laser. A quantum dot may be incorporated into a nanowire laser, which can be electrically or optically coupled to a power source. This allows the quantum dot to be excited and thus causes a photon to be generated. A technique for using a quantum dot in a nanowire laser to generate a single photon is disclosed in U.S. patent application Ser. No. 11/084,886 filed Mar. 21, 2005 entitled “A nano-VCSEL Device and Fabrication Thereof Using Nano-Colonnades,” which is fully incorporated herein by reference.  
         [0014]      FIG. 1  illustrates an exemplary nanowire laser  101  that may be used for generating a photon. The nanowire laser  101  typically comprises a nanowire  107  and an active region  103 . The nanowire  107  is typically grown in a semiconductor substrate. Group IV, Group III-V, or Group II-VI semiconductor materials may be used. A typical material may comprise Si or GaAs. A nanowire  107  is grown on either side of an active region  103 . The nanowire  107  is very small in diameter relative to a wavelength of light produced by the active region. Typically, the nanowire portion  107  of the nanowire laser  101  is approximate  10-100  nm in diameter.  
         [0015]     An active region  103  resides within the nanowire  107 . The active region  103  comprises a quantum dot. A quantum dot is typically formed from a material that has a bandgap that is different from the bandgap of the material that comprises the nanowire. This allows the quantum dot to be excited, either electrically excited by supplying a charge via current supply leads  115   a ,  115   b , or optically excited via a laser (not shown), in order to emit a photon. For example, a semiconductor material such as InGaAs may be used to form a quantum dot within a nanowire that comprises InP. InGaAs has a low bandgap relative to InP.  
         [0016]     The structure of the nanowire laser  101  typically results in a generated photon typically traveling within the laser in a lengthwise direction, towards a first end  109  or a second end  111 . At each end of the laser  101 , a Bragg mirror  113   a ,  113   b  is grown in the crystal material. Bragg mirrors are known within the art and are used in applications that require high reflectivity. The Bragg mirror  113   b  at one end of the laser (shown as the second end  111  in  FIG. 1 ) is constructed to be of a higher reflectivity that the Bragg mirror  113   a  at the opposite end of the laser (shown as first end  109  in  FIG. 1 ). As a result, the probability that a generated photon will exit the laser from the first end  109  is increased.  
         [0017]     Once a photon is generated, it must still be captured and carried to a location where it can be used. Thus, the second step in photon use is the ability to detect and capture the photon. Detecting and capturing a single photon can be a difficult task in light of the small size of a nanowire laser in comparison to traditional optical lasers. Traditionally, generated photons have been detected by directing the photons onto a photo-detector capable of detecting the presence of photons. In order to allow the photo-detector to determine the presence of photons, the photons may be focused on the photo-detector by placing a large lens in close proximity to the photon source. The lens functions to re-direct the path of any photons striking it onto the photo-detector. However, even with an increased probability that the photon will exit a particular end of the nanowire laser (e.g., first end  109 ), the direction of a photon generated from a nanowire is often unpredictable. The use of the lens allows an increase in the probability that generated photons will be detected by the photo-detector, but many photons may still simply be lost because the lens fails to either capture the photons or focus the photons onto the center of the detector&#39;s image plane. Additionally, this technique is somewhat limited because the generated photons are not able to be easily transported (e.g., via a waveguide) where it can be more efficiently used for quantum computation.  
         [0000]     Photon Coupling Technique  
         [0018]     Referring to  FIG. 2 , an exemplary embodiment of a device for coupling a single photon to an optical fiber in accordance with the present invention is shown. The exemplary embodiment shown in  FIG. 2  can couple a single photon between a nanowire laser  201  and a waveguide  203  without incorporating an independent lens or photodetector. The coupling technique used comprises capturing a photon that is generated by a nanowire laser  201  and emitted from one end  206  of the nanowire laser  201  in an optical fiber waveguide  203 . In one exemplary embodiment, the optical fiber waveguide  203  has a lens  205  polished on the end  202  facing the laser  201 . The lens  205  facilitates entry of the photon into the fiber by increasing the angular acceptance of the fiber end  202 . An anti-reflection coating may be applied to the fiber end to reduce its reflectivity. One of several known techniques may be used to form the lens  205 , for example, by using a CO 2  laser to melt and reshape the fiber tip.  
         [0019]     While this technique improves the likelihood of capturing a photon generated by the laser  201 , maintaining the desired mechanical positioning relationship between the laser  201  and the fiber  203  is difficult. To overcome this difficulty, the fiber  203  can be precisely positioned on the surface of a substrate  207 . Typically, the nanowire  201  laser is grown within a substrate  207  such as silicon. Alignment fiducials  211 ,  213  may be etched into the surface of the substrate  207 . This creates an indexing recess  204  into which the fiber  203  can be positioned. By accurately indexing the fiber  203  to the location of the laser  201 , the mechanical positioning between the laser  201  and the fiber  203  can be better maintained and, as a result, the probability of capturing a generated photon is increased. To maintain the alignment, the fiber  203  may be secured in place using known techniques, such as using an adhesive.  
         [0020]     In some instances, fabricating a structure to perform the coupling as described above and shown in  FIG. 2  can be difficult. The direct coupling process may be improved by using a configuration as shown in  FIG. 3 . A nanowire laser  301  may be embedded into a substrate  300  that comprises a two dimensional photonic crystal  302 . Two dimensional photonic crystals can provide Bragg reflections and large index dispersion in a two dimensional plane. At each interface within the crystal, light is partly reflected and partly transmitted. By using this property of photonic crystals, the photon emitted by the laser can be better mode matched to the fundamental mode of a fiber  303 .  
         [0021]     Additionally, by embedding the nanowire laser  301  in the two dimensional photonic crystal  302 , the evanescent fields emitted by the laser are controlled. Evanescent fields are energy fields that escape from the laser through the laser sides. For example, light will propagate a short distance beyond the plane of total internal reflection, which in this case is the edges of the nanowire laser  301 . By embedding the nanowire laser  301  into the a two dimensional photonic crystal substrate  302 , such as glass coated with a InGaAs or Si/SiO 2  coating, evanescent fields are prevented from emanating from the laser  301 . A fiber  303  having a lens  307  formed on the fiber end is positioned in close proximity (e.g., less than one micron) to the laser  301  to capture a generated photon. A pattern of holes  309  may be etched into the two dimensional photonic crystal, which may be used for aligning the fiber in a precise mechanical position relative to the laser  301 .  
         [0022]     An alternative embodiment for enabling direct coupling of a nanowire laser to a waveguide is shown in  FIG. 4 . In the embodiment shown in  FIG. 4 , a photonic crystal fiber  403  is used instead of a tapered fiber. Photonic crystal fiber, referred to as “holey” fiber, comprises a plurality of airhole passages  402  residing within the fiber  403 . A nanowire laser  401  is positioned such that it extends into an airhole passage  402  of the fiber  403 . The nanowire laser  401  is grown in a substrate  400 . An indexing hole  408  is etched in the substrate  400  surrounding the laser  401 . The photonic crystal fiber  403  is positioned within the indexing hole  408  such that the laser  401  extends into a selected air hole passage  402  contained within the fiber  403 . Using this configuration provides for several advantages. The nanowire laser  401  can be precisely positioned relative to the fiber  403 . Additionally, the coupling efficiency can be improved by means of mode-matching between the evanescent mode of the nanowire laser  401  and the evanescent mode of the fiber  403 , coupled with the fact that photonic crystal fiber typically has a larger numerical aperture than conventional single mode fiber, such as is commonly used in the telecommunications industry (e.g., single mode fiber typically has a numerical aperture ranging from approximately 0.2-0.5 while photonic crystal fiber typically has a numerical aperture ranging from approximately 0.7-0.9).  
         [0023]     Coupling between a nanowire laser and a fiber may also be achieved using evanescent mode coupling. The evanescent coupling between two adjacent waveguides is determined by the rate at which energy is transferred from one waveguide into the other, which in turn is proportional to the overlap of the electric fields of the two waveguides:
 
c(z)∝∫d 2 rE 1 *(r)·E 2 (r)  Equation (1)
 
 where c(z) is the mode overlap between two waveguides; z is the coordinate axis parallel to the axes of the waveguides; E 1 (r) is the electric field profile of the eigenmode in waveguide  1  at a point r={x, y, z}; E 2 (r) is the electric field profile of the eigenmode in waveguide  2  at the same point. The primary propagation axes of the waveguides are oriented in the z direction, and the two dimensional integral is performed over the transverse coordinates {x, y}, assuming a weak-coupling limit where the presence of one waveguide does not affect the modes of the other. The coupled wave equations are generally integrated over a distance z that is long compared to the wavelength, giving a substantial integrated mode overlap. In principle, the nanowire laser will be so short that the integrated mode overlap of the evanescent fields will be small, but in practice multiple passes of the electromagnetic field between the Bragg mirrors of a high-Q resonator will allow a substantial optical path length to be accumulated. 
 
         [0024]     An exemplary embodiment illustrating the evanescent coupling of a nanowire laser and a fiber is shown in  FIG. 5 . A tapered fiber  503  is positioned in a substrate  500  using an etched alignment fiducial  502 . The fiber  503  is positioned proximate to a nanowire laser  501 . The evanescent fields produced by the laser  503  are coupled to the fiber  501  in accordance with equation 1 set forth above.  
         [0025]     Other evanescent configurations may be constructed based on the configuration described above. For example, a collection of nanowire lasers can be arranged circumferentially around a tapered fiber.  FIG. 6  shows a fiber  603  positioned in a substrate  500  with two nanowire lasers  605 ,  607  positioned adjacent to the fiber  603 . While two nanowire lasers  605 ,  607  are shown for simplicity, any number of nanowire lasers could be used. If the nanowire lasers  605 ,  607  are identical and operated in tandem, the rate at which single photons of the same wavelength are generated can be increased. Alternatively, using nanowire lasers that differ in active material and/or structure allows for single photons of distinct wavelengths to be coupled into a single fiber, provided that the propagating modes at each distinct wavelength are supported by the fiber. Additionally, a region  608  that exists between the fiber and the waveguide could be filled with an index-matching material to enhance the coupling between the nanowire lasers and the fiber.  
         [0026]     A variety of modifications to the embodiments described will be apparent to those skilled in the art from the disclosure provided herein. Thus, the present invention may be embodied in other specific forms without departing from the spirit or essential attributes thereof and, accordingly, reference should be made to the appended claims, rather than to the foregoing specification, as indicating the scope of the invention.