Patent Publication Number: US-2019187380-A1

Title: Photon generator

Description:
RELATIONSHIP TO OTHER PENDING APPLICATIONS 
     This patent application is a continuation of, cross references, and claims any and all priority benefit from U.S. patent application Ser. No. 15/833,274 filed on Dec. 6, 2017, now pending and incorporated by reference as if fully set forth herein. 
     U.S. patent application Ser. No. 15/833,274 cross references and claims the priority benefit under 35 USC § 119(e) of the filing date of provisional application Ser. No. 62/424,739 having been filed in the United States Patent and Trademark Office on Nov. 21, 2016 and now incorporated by reference as if fully set forth herein. 
    
    
     STATEMENT OF GOVERNMENT INTEREST 
     The invention described herein may be manufactured and used by or for the Government for governmental purposes without the payment of any royalty thereon. 
    
    
     TECHNICAL FIELD OF THE INVENTION 
     This invention relates generally to the field of quantum information processing and more specifically to integrated photonic devices that facilitate the same. 
     BACKGROUND OF THE INVENTION 
     Integrated photonics is proving to be a very promising platform for quantum information processing. Micro ring resonators are becoming a key component of such systems as they have been shown to be effective as photon-pair sources by means of exploiting a materials nonlinearity for spontaneous parametric downconversion (SPDC) or spontaneous four wave mixing (SFWM). 
     Often, it is desirable to have precisely one photon. While SPDC and SFWM sources generate pairs of photons, single photons can be achieved through heralding. Heralding is a technique in which the detection of a single photon from a pair is used to determine the existence of the other. One of the fundamental issues with ring resonators is their inherent 50% loss when critically coupled, regardless of operation in a single bus or double bus configuration. For single bus resonators (not shown), half of the generated photons are lost to scattering within the cavity. 
     Referring to  FIG. 1  depicts prior art double bus resonators which are slightly different as the photons are free to leave the ring  10  through either port—resulting in an effective loss of 50%. All of this assumes that the ring resonator is critically coupled to straight waveguides  20 ,  30 . 
     As with the two typical forms of ring resonators, they are denoted by the number of waveguides coupled to them giving them the titles of single bus and double bus, respectively. Both resonators work on the same principle. When light after a full round trip around the ring is of equal intensity and opposite phase to light that is reflecting into the ring, there is a destructive interference and no light can leave the resonator. Running time in reverse and seeing the light from the ring split at the directional coupler is an equivalent way to view this effect. In the case of the single bus resonator with no loss, resonance can only happen for a coupling ratio of 50/50 from the bus waveguide. When loss is present, this can happen for much lower splitting ratios. One form that loss can take is scattering. The double bus resonator can be seen as a special case of the single bus resonator where the scattering is captured into the second waveguide. 
     When the ring resonator is used for generation of single photons, two different processes can occur depending on the nonlinearity of the material of the waveguide. In the case of spontaneous parametric downconversion, a single pump photon produces a photon pair, called a signal and idler. The second case is spontaneous four wave mixing where two pump photons are absorbed and two single photons are created. Both of these cases must conserve energy and momentum. 
     Consequentially, the single photon light which is generated inside of the cavity has no input light to interfere with. Still referring to  FIG. 1 , therefore, in the case of the double bus resonator with the same coupler on input and output, the light that is generated inside the nonlinear optical material based mircroring resonator has an equal probability of exiting the first  20  and second  30  waveguide buses. This splitting is witnessed as intrinsic loss. In the case of single bus ring resonators, the light can either leave through the input port or be lost inside the ring. When the pump wavelengths are optimally coupled, the propagation losses around the ring balance with the coupling out of the ring. The generated single photons (like the pumps) will have this same balance in terms of loss and ability to couple out of the ring. In other words, the single photons leave the ring only 50% of the time. The odds of the single photons leaving the ring can be improved at the cost of how well the pump wavelengths are coupled. This is a compromise between loss and generation rate. 
     The underlying issue of single and double bus ring resonators is that they do not have wavelength discriminating couplers. It is well understood there doesn&#39;t exist dichroic mirrors on a chip presently. Moreover, in 1995, Barbarossa found that resonant wavelengths of a micro ring cavity could theoretically be suppressed by coupling the input waveguide to the ring at two points. However Barbarossa&#39;s design provided an optical filter for classical light without generating any photons in the resonator cavity. What is lacking in prior work and therefore still needed is a device that generates entangled pairs of photons and interferometric coupling as a filter for quantum states of light. 
     OBJECTS AND SUMMARY OF THE INVENTION 
     It is therefore a primary object of the present invention to provide an apparatus and method to generate and detect entangled pairs of photons for use in quantum information processing. 
     It is another object of the present invention to provide an integrated photonic apparatus and method that generates entangled pairs of photons. 
     A fundamental embodiment of the present invention, a quantum computation device, comprises a plurality of photon generators each have a second input and a second output; a first plurality of optical couplers, each corresponding to each of the plurality of photon generators couple the second input and the second output of the photon generator so as to produce entangled photon states; a second plurality of optical couplers, each corresponding to each of the first plurality of optical couplers; a reconfigurable optical switch network for matrixing connections between outputs of the first plurality of optical couplers and inputs of the second plurality of optical couplers; a third plurality of optical couplers, each connected to each of a corresponding second plurality of optical couplers so as to further entangle the photon states; and a plurality of photodetectors for indicating the entangled photon states output from the third plurality of optical couplers so as to facilitate computations therefrom. 
     Still in a fundamental embodiment of the present invention, a quantum computation device, comprises a photon generator having an annular optical channel, a first linear optical channel having a first input and a first output where the first linear optical channel is substantially tangential to the annular optical channel at a first point and a second point, a second linear optical channel having a second input and a second output, where the second linear optical channel is substantially tangential to the annular optical channel at a third point and a fourth point; and a predeterminable relative phase delay between the first and the second linear optical channels so as to cause a variance in an amount of light traversing the first and the second linear optical channels as a function of the frequency of the light. 
     In the preferred embodiment of the present invention, a quantum computation device, comprises a photon generator having an annular optical channel disposed in a chip, a first linear optical channel disposed in the chip, where the channel has a first input and a first output and where the first input and a first output are in common with each other and with an input to the chip, where the first linear optical channel is substantially tangential to the annular optical channel at a first point and a second point, and where a second linear optical channel is disposed in the chip with the second linear optical channel having a second input and a second output, where the second linear optical channel is substantially tangential to the annular optical channel at a third point and a fourth point, a first predeterminable relative phase delay between the first and the second linear optical channels so as to cause a variance in an amount of light traversing the first and the second linear optical channels as a function of the frequency of said light, and a second predeterminable relative phase delay between the second input and the second output, a photon detector sampling each of the second input and the second output, and a third output of the chip in common with the second input, a fourth output of the chip in common with the second output, and an electronic control subsystem in operative communication with the chip for facilitating the predeterminable relative phase delays and the photon detection. 
     Briefly stated, the invention provides an apparatus for quantum computing comprising optical integrated on-chip generation of photon pairs as a building block to create entangled photon states which are detected as necessary for quantum information processing. The invention provided a frequency selective optical coupling device which controls the transmission of light by varying the relative dimensions of otherwise symmetrical linear optical waveguides tangential to an annular optical waveguide, thereby controlling the coupling of light between the linear optical waveguides and the annular optical waveguide. Dimensional change of the optical waveguides is achieved by a heated medium in proximity of the optical waveguides and under electronic control. The device produces entangled photons in the nonlinear optical material based ring resonator, maximizing the coupling of the pump photons, and spectrally filtering the strong pump light from the generated photon pairs. The apparatus that generates the photon pairs, the dual mach-zehnder coupled ring resonator, is only a portion of the invention. A similar device was used in Popovic to modulate light, though there the device was for classical applications and the photons were input from outside the device. In this invention the photons that are input from outside the device only serve to add energy to produce the photon pairs that are inside the nonlinear optical material based ring resonator. These photons that are now generated inside the nonlinear optical material based ring resonator are photon pairs and can be used for quantum applications. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1  is a prior art double bus resonator showing the coupling coefficients to the two waveguides. 
         FIG. 2 a    is a Dual Mach-Zehnder device design of the present invention. 
         FIG. 2 b    is a microscope image of a fabricated Dual Mach-Zehnder device of the present invention. 
         FIG. 3 a    is a Dual Mach-Zehnder theoretical spectrum showing suppressed resonances at the input side and a single transmission dip. 
         FIG. 3 b    is a Dual Mach-Zehnder theoretical spectrum showing output side showing a suppressed single resonance and two resonance dips. 
         FIG. 4  is a Dual Mach-Zehnder experimentally generated spectrum showing suppressed resonances before and after tuning on both the input and output sides of the resonator. 
         FIG. 5 a    is a Dual Mach-Zehnder measured photon pairs in the untuned configuration showing unwanted pairs on ports other than drop-drop, and therefore a long coincidence count rate. 
         FIG. 5 b    is a Dual Mach-Zehnder measured photon pairs in the tuned configuration showing the removal of the unwanted pairs exiting the other ports, and a noticeable increase in the drop-drop port coincidence rate. 
         FIG. 6 a    is an embodiment of the present invention employing a Dual Mach-Zehnder used to produce energy-time entangled photons pairs/squeezed beams. 
         FIG. 6 b    is an embodiment of the present invention employing a Dual Mach-Zehnder used to produce energy-time entangled photons pairs/squeezed beams, further depicting interconnections to the off chip electronics. 
         FIG. 7 a    is an embodiment of the present invention employing a Dual Mach-Zehnder used to produce NOON states or pairs/squeezed beams. 
         FIG. 7 b    is an embodiment of the present invention employing a Dual Mach-Zehnder used to produce NOON states or pairs/squeezed beams, further depicting interconnections to the off chip electronics. 
         FIG. 8 a    is an embodiment of the present invention employing a Dual Mach-Zehnder used to produce NOON states and pairs/squeezed beams simultaneously. 
         FIG. 8 b    is an embodiment of the present invention employing a Dual Mach-Zehnder used to produce NOON states and pairs/squeezed beams simultaneously, further depicting interconnections to the off chip electronics. 
         FIG. 9 a    is an embodiment of the present invention employing a Dual Mach-Zehnder used to produce NOON states, frequency combs, and pairs/squeezed beams simultaneously. 
         FIG. 9 b    is an embodiment of the present invention employing a Dual Mach-Zehnder used to produce NOON states, frequency combs, and pairs/squeezed beams simultaneously, further depicting interconnections to the off chip electronics. 
         FIG. 10  is an embodiment of the present invention providing a quantum computation device employing a Dual Mach-Zehnder used to produce NOON states, frequency combs, and pairs/squeezed beams simultaneously, capable of photo detection to facilitate computation. 
     
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT 
     An object of the present invention is to provide a quantum computation device that utilizes a wavelength dependent means to generate correlated photon pairs and separate those pairs which are generated in nonlinear optical material based ring resonator from the pump light used to generate them. The present invention employs a Dual Mach-Zehnder (MZI) device having legs that are grossly misbalanced, wherein the MZI will have a wavelength dependence to its ability to seperate the pump from the signal and idler photons. The present invention devises two unbalanced MZI, one which will perfectly transmit the pump wavelengths and partially reflect the signal/idler wavelength. The other MZI will do the opposite, reflecting the pump wavelengths but perfectly transmitting the signal/idler wavelength. The signal/idler are also generated inside the device via a nonlinear process, either spontaneous parametric downconversion or spontaneous four wave mixing. 
     Referring to  FIG. 2 a    and  FIG. 2 b   , the present invention essentially makes a a frequency selective optical coupling device having a nonlinear optical material based ring resonator in a double bus waveguide configuration where each bus waveguide connects the ring resonator at two independent points. Between these two connecting points a long waveguide section is placed to define a phase differential between the ring and the coupling arm. This creates an asymmetric Mach-Zehnder interferometer, a wavelength (frequency) selective device. Mach-Zehnder interferometer (MZI) out of the input waveguide  40  and the ring  50 . Being a cavity, the nonlinear optical material based ring  50  will only support specific wavelengths of light (where the resonance condition is satisfied) separated by the free spectral range (FSR). The spectrum of an unbalanced MZI is sinusoidal with the difference in optical path length between the two paths determining where in the spectrum the constructive and destructive interference will occur. For both the ring and the MZI, this is known as phase-matching. For the case of the ring this is phase-matching between consecutive round-trips while in the MZI it is phase-matching between the two different paths. The points of constructive interference in the spectra of these devices can be tuned by adjusting the relative phase between the different paths. In a fabricated device (see  FIG. 2 b   ) this can be accomplished by heaters or electro-optic phase shifters. The combination of these two elements results in a phase-matching condition that relies on both the resonance condition of the ring  50  and the interference pattern of the MZI. If the spectral width between two wavelengths of constructive interference in the MZI is twice the FSR of the ring  50 , it is possible to suppress every second resonance of the ring  50 . 
     For the case of the photon-pair source function of the present invention, one side of the ring  50  can be used as the input  40  for the pump photons and the drop side  60  as the output for the photon pairs that are generated inside the nonlinear optical material based ring resonator. The MZI on the input side  40  (MZI 1 ) can be tuned to suppress every other resonance, while MZI 2  on the output of the ring  50  can be tuned to suppress the resonances allowed by MZI 1  (i.e. they are perfectly out of phase with each other). This configuration will ensure the pump laser is critically coupled into the ring  50  while not allowing it to exit out the drop port  60 , and ensures that any photons that are generated in the device at the resonances allowed by the drop port  60  will only exit the over-coupled drop port  60  (because MZI 1  is tuned to not be phased matched with those photons). This makes the device function as though it is two independent single bus ring resonators, one for the input side and one for the output side. The input side ring is characterized by the transmission from the input port  40  to the through port  70  while the output side ring is characterized by the transmission from the add port  80  to the drop port  60 . The photon pairs that are generated inside the ring according to energy and momentum conservation, with a strength corresponding to the pump intensity, nonlinear coefficient and the finesse of the ring resonator are the photons that leave on the exit port. It is crucial to note that the photons that are input to the device, the pump photons, are not the same photons that are exiting the device. The photons that exit the device are truly correlated photon pairs of which one can be detected to herald the presence of the second to produce true single photons. The theoretical spectral response for both the input and output sides are shown in  FIG. 3 a    and  FIG. 3 b   , respectively. This configuration has three key features: (i) The pump is critically coupled so the photon generation rate produced inside the device will be maximized; (ii) The pump is filtered from the photons pair generated inside the device and that exit the drop port minimizing noise and reducing the amount of off-chip filtering required; (iii) The photon pairs will always leave out the same over-coupled drop port, yielding 100% coincidence ratio, maximizing heralding efficiency. 
     The theory of operation of the present invention has been experimentally proven on a fabricated device as shown in  FIG. 4 . The invention exhibits all the cavity resonances when the thermal tuning has not been optimized. When the thermal tuning has been adjusted the undesirable resonances on both the input and output sides of the device are suppressed as shown in  FIG. 4 . This demonstrates the spectral filtering of the device (needed to remove the strong pump light from the single pairs of photons), along with the field enhancement from the ring cavity, and the directionality of the desired output for the photon pairs generated in the device shown in  FIG. 5 a    and  FIG. 5 b   . All aforesaid traits being useful for quantum information science applications. 
     With the confirmation of the dual Mach-Zehnder configuration as an optimal design for the generation of maximally bright, pump filtered, directionalized photon pairs, larger photon pair states, and higher squeezed states, the functional building block can be utilized to create entangled states when combined with other integrated waveguide circuits. 
     Detailed below are five different implementations of the present invention built with the dual mach-zehnder photon pairs generation source built into the circuit for use in quantum information science applications. These are not the only implementations that this device can be configured in for these applications. The invention as stated can be used to generate, photon pairs, entangled states, larger entangled states (cluster states, GHZ states, W states, etc.), and higher squeezed states (for continuous variable applications). All embodiments of the present invention described below can be utilized to generate any of these mentioned photon states. Lastly another benefit of the invention is that the source acts as filter for the pump light. This is an easy problem to deal with in bulk optics, but in integrated circuits, removing the pump is difficult since high rejection filters are required on chip to deal with ˜10 orders of magnitude difference in pump to signal/idler power. The present invention takes care of a large portion of this filtering. 
     Referring now to  FIG. 6 a    and  FIG. 6 b    concurrently depicts a dual Mach-Zehnder (DMZ) source being single or bi-directionally pumped from a continuous wave or pulsed laser source (not shown) via an optical waveguide  90 . The lower diagram in  FIG. 6 b   ,  FIG. 7 b   ,  FIG. 8 b    and  FIG. 9 b    depicts an overlay of the off chip electronics  160  and its associated control lines  170  (dashed lines) to detection  140  and phase shifting  150  elements. 
     The pump photons interact in the nonlinear optical material based micro-ring resonator cavity  100  and produce signal/idler photons via the nonlinear process of spontaneous parametric downconversion or spontaneous four wave mixing, which exit via the optical waveguides  110  to the right of the micro-ring resonator  100 . The signal/idler photons pass through phase shifters  120  which can compensate for length and timing differences before hitting an optical tap  130  where a small portion may be sent to a photodetector  140  to monitor the photons. The other ports  180  allows the photon pairs/squeezed beams to pass to the rest of the circuit on the integrated chip or leave off chip. The device is controlled by off chip electronics  160 , with electrical control lines  170  being depicted as dashed lines in each of  FIG. 6  through  FIG. 9 . Part of what the off chip electronics  160  controls are the “heater” mechanisms  150 . Heater mechanisms  150  designated in  FIG. 6  through  FIG. 10  as wide, solid black sections comprise material that is placed alongside optical waveguide within the DMZ. When activated by the off chip electronics, the heater mechanisms  150  heat the adjacent optical waveguide, causing a dimensional change in the optical waveguide. The optical dimensional change insofar as the optical waveguide length is affected will cause a phase shift for any light therein. The net desired effect is to alter the relative optical lengths between the upper and lower waveguides and the optical length of the ring resonator  100  within the DMZ. The circuit that is shown in  FIG. 6  utilizes the DMZ to produce a frequency comb of entangled photon pairs or when operated in the bright pair regime will produce a comb of entangled squeezed light beams separated by a cavity free spectral range. This allows in both cases the quantum equivalent of a dense wavelength division photon source in a single device. 
     Referring now to  FIG. 7 a    and  FIG. 7 b    concurrently depicts DMZ source being pumped bi-directionally from a laser (continuous wave or pulsed) via an optical waveguide  90 . The pump photons interact in the ring resonator  100  and produce signal/idler photons via the nonlinear process of spontaneous parametric downconversion or spontaneous four wave mixing, in both clockwise and counter-clockwise directions, thus producing path indistinguishable photons created in the ring  100 . These photons then exit via the optical waveguides  110  to the right of the ring. The signal/idler photons pass through phase shifters  120  which can compensate for length and timing differences before simultaneously impinging on a directional coupler  190 . Directional coupler  190  is formed from one linear optical channel  220  connected between one of the phase shifters  120  and the corresponding optical tap  130 , and another linear optical channel  230  connected between one of the phase shifters  120  and the corresponding optical tap  130 . The two linear channels  220 ,  230  are substantially tangential at one point along their approximate mid-length. It is at this substantially tangential point that light is free to couple from one of the two linear optical channels to the other, thereby producing a coupling effect. The resultant coupler  190  mixes the photon states producing an entangled state called a NOON state, or N photon, Zero, Zero, N photon state. The state exits the coupler  190  and passes to an optical tap  130  where a small portion may be sent to a detector  140  to monitor the photons. The other ports  180  allows the photons to pass to the rest of the circuit on the integrated chip or leave off chip. The circuit can be utilized to produce not only NOON states but also qudit states for the other portions of the frequency comb that is produced. 
     Referring now to  FIG. 8 a    and  FIG. 8 b    concurrently depicts DMZ source being pumped bi-directionally from a laser (continuous wave or pulsed) via an optical waveguide  90 . The pump photons interact in the ring resonator cavity  100  and produce signal/idler photons via the nonlinear process of spontaneous parametric downconversion or spontaneous four wave mixing, in both clockwise and counter-clockwise directions, thus producing path indistinguishable photons created in the ring resonator  100 . These photons then exit via the optical waveguides  110  to the right of the ring resonator  100 . The spectrally degenerate photons are selected by an optical ring resonator filter  200  and pass through phase shifters  120  which can compensate for length and timing differences before impinging on a directional coupler  190 . This coupler  190  mixes the photon states producing an entangled state called a NOON state, or N photon, Zero, Zero, N photon state. The state exists the coupler  190  and passes to the rest of the circuit on the integrated chip or leave off chip. The photons that are not selected by the filter  200  travel on a different waveguide, passing through a phase shifter  120  and then hitting an optical tap  130 . This resonant comb of other wavelengths can be monitored with a photodetector  140  or passed to other circuitry to be utilized elsewhere. This source, shown in  FIG. 8 a    and  FIG. 8 b   , can then produce NOON states, entangled frequency combs, and or squeezed states simultaneously. 
     Referring to  FIG. 9 a    and  FIG. 9 b    concurrently depicts The DMZ source is pumped bi-directionally from a laser (continuous wave or pulsed) via an optical waveguide  90 . The pump photons interact in the ring resonator cavity  100  and produce signal/idler photons via the nonlinear process of spontaneous parametric downconversion or spontaneous four wave mixing, in both clockwise and counter-clockwise directions, thus producing path indistinguishable photons created in the ring resonator  100 . These photons then exit via the optical waveguides  110  to the right of the ring resonator  100 . The spectrally degenerate photons are selected by an optical ring resonator filter  200  and pass through phase shifters  120  which can compensate for length and timing differences before impinging on a directional coupler  190 . This coupler  190  mixes the photon states producing an entangled state called a NOON state, or N photon, Zero, Zero, N photon state. The state exits the coupler  190  and passes to the rest of the circuit on the integrated chip or leave off chip to other circuits. The photons that are not selected by the ring resonator filter  200  travel on a different waveguide, passing through a phase shifter  120  followed by two additional filters  210 . These two secondary filters  210  can serve a number of functions. They can further filter the pump wavelength to allow for a filtered set of photons to leave on the original waveguide. They can each filter out a different set of wavelengths to produce more correlated outputs, one on each set of filter outputs and letting the rest of the comb exit on the original waveguide when multiple correlated photon pair outputs are required. This source can then produce NOON states, multiple energy-time correlated pairs/squeezed beams, entangled combs, and squeezed states simultaneously. 
     Referring to  FIG. 10  depicts the DMZ source being pumped bi-directionally from a laser (continuous wave or pulsed) via an optical waveguide  90 . The pump photons interact in the ring resonator cavity  100  producing signal/idler photons via the nonlinear process of spontaneous parametric downconversion or spontaneous four wave mixing, in both clockwise and counter-clockwise directions, thus producing path indistinguishable photons created in the ring resonator  100 . These photons then exit via the optical waveguides to the right of the ring resonator  100 . The signal/idler photons pass through phase shifters  120  which can compensate for length and timing differences before simultaneously impinging on a directional coupler  190 . These partially spectrally filtered (pump not fully rejected) signal/idler photons enter coupler  190  which mixes the photon states producing an entangled state called a NOON state, or N photon, Zero, Zero, N photon state. The state exits the coupler  190  and passes to a switching network which in one implementation could consist of Mach-Zehnder interferometers (MZI). These MZI&#39;s mix the photon states in a reconfigurable manner that allows the creation of entangled states. These can range from two photon (Bell states) to larger entangled states (Cluster and Greene-Horne-Zeilinger (GHZ) states). The circuit can be used to produce states important for small scale quantum information processing, specifically quantum computation. The optical waveguides can terminate with photodetectors  140  allowing the entire computation to be completed on chip. 
     Still referring to  FIG. 10 , the invention produces larger entangled photon states. The invention would be the quantum equivalent of an FPGA (field programmable gate array) in classical computing, thus one advantage is the reconfigurability. The invention functions in the following way, a pump laser is input to optical waveguide  90 , and travels to ring  100 . Inside ring  100 , the pump laser&#39;s photons are converted into pairs of photons which are correlated, or twin photons. Due to the design of the optical waveguide  90 , connecting to the ring  100 , only the twin photons enter the two phase shifters  120 , while the pump laser light remains in ring  100 . These twin photons traveling through  120  experience a phase shift and interfere at directional coupler  190 . These correlated photons are entangled and can be used as quantum bits for computation. All this occurs in only one section of the invention from  90 , to  100 , to  120 , to  190 . Ideally for real computations more than two quantum bits are required, so the necessary components  90 ,  100 ,  120 , and  190  are repeated in an array from  1  to n. To allow all of these different sources to become entangled, through interference, and function together a large array of these interferometers are required, made of components  190 ,  120 , and  190 . The required grid of interferometers is n×n, where n is number of waveguides exiting all the rings  100 . Encoding via interference and phase shifts via  120 , are imprinted on the channels to create larger quantum states or enact a calculation. The result of these changes can be measured via a photodetector  140 , and the results are recorded via electronics. This invention would be one incarnation of a photonic processor for quantum computation. This device allows for the generation of large entangled states in a reconfigurable fashion due to the mesh network of interferometers. 
     The dual mach zehnder photon source,  90  &amp;  100 , allows for on chip filtering of the pump laser, something not done before in a source. This source also allows for the use of a single integrated chip as most systems would need to filter the pump light off chip before going to the interferometric mesh network. 
     The dual mach zehnder design allows for controlled directionality of the twin photons, which are the required quantity needed for computation (these are the quantum bits). Traditional sources lose 50% of these twins just from their source design. Therefore the dual mach zehnder source allows for a reduction in the required pump laser power compared to other sources. This makes the overall device more efficient. 
     Having described preferred embodiments of the invention with reference to the accompanying drawings, it is to be understood that the invention is not limited to those precise embodiments, and that various changes and modifications may be effected therein by one skilled in the art without departing from the scope or spirit of the invention as defined in the appended claims.