Patent Publication Number: US-8111970-B2

Title: Electromagnetic radiation frequency optimizing device and method with ambient heat conversion device

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS 
     This application is a continuation-in-part of U.S. application Ser. No. 12/566,966, filed Sep. 25, 2009. 
    
    
     FIELD OF TECHNOLOGY 
     The following relates to a device and method for optimizing and altering electromagnetic frequency using Doppler shifts of electromagnetic radiation, and, more specifically, to embodiments having a conversion device to convert ambient heat into electricity. 
     BACKGROUND 
     Photovoltaic (PV) devices operate optimally when incident electromagnetic radiation (EMR) has an energy that corresponds closely to the electron band gap of the PV material. Solar EMR is made up of a continuous spectrum of frequencies and wavelengths. When a photon with an energy less than the electron band gap of a given PV material, the photon lacks sufficient energy to move the electron from its valence band into the conductive band, and the PV material produces no electric current. When a photon has an energy greater than that of the PV material&#39;s electron band gap, the electron is moved to the conductive band, consuming the energy corresponding to the band gap, and the excess energy (i.e. the difference between the incoming photon and the PV electron band gap) is not utilized and otherwise lost, generally as heat. Using a radiation source having an energy optimized for the particular PV material used in a solar cell array increases the efficiency of the PV material because less EMR is lost or wasted as heat, and more electricity is produced. Because of the rising demand for alternative energy sources, the need for an efficient alternative energy exists. A major deficiency in alternative energy sources, such as solar energy, include low rate of conversion of EMR to electricity. 
     Therefore, a need exists for a device and method to increase efficiency of PV cells and avoid excess loss of EMR by altering and optimizing the frequency of incident EMR such that energy production in a PV cell is maximized. 
     Moreover, the frequency of the vibration and the frequency of the radiation are directly related to a temperature of a substance. Typically, the higher the temperature, the greater the speed of vibration and the higher the frequency of emitted radiation. Additionally, heat generally moves from a higher energy (temperature) location to a lower energy location. Thus, constant ambient heat from high temperature locations and low temperature locations is a renewable source of energy. However, the frequency of the radiation emitted by ambient temperature matter is generally below the threshold necessary to produce electricity using a photovoltaic cell. 
     Therefore, a need exists for a device and method to convert ambient heat into electricity. 
     SUMMARY OF THE INVENTION 
     A first general aspect relates to an electromagnetic radiation optimization device comprising a crystal undergoing a vibration, said crystal positioned in an opening having walls, wherein an interaction between an incoming electromagnetic radiation and said vibration of said crystal optimizes a frequency of said electromagnetic radiation. 
     A second general aspect relates to an electromagnetic radiation frequency optimizing device comprising a first end having a separator positioned proximate said first end, a second end having a focusing member positioned proximate said second end, at least two opposed walls having a reflective surface, wherein said at least two opposed walls connect said first end and said second end, and at least one absorption area located on said reflective surface. 
     A third general aspect relates to a method of optimizing electromagnetic radiation comprising providing a channel having a first end, a separator positioned proximate said first end, a second end, a focusing member positioned proximate said second end, at least two parallel walls having an reflective surface, wherein said at least two parallel side walls connect said first end and said second end, and at least one absorption area located on said reflective surface, determining an optimal frequency relative to a usable frequency of a target, separating an incoming electromagnetic radiation into component frequencies, vibrating said at least two parallel walls, wherein said parallel walls contain at least one crystal capable of vibration, directing said incoming electromagnetic radiation toward said at least two parallel walls, wherein contact between said incoming electromagnetic radiation and said vibration of said at least one crystal alters a frequency of said electromagnetic radiation toward said optimal frequency, and passing said optimal frequency through said second end. 
     A fourth general aspect relates to a method of providing a crystal undergoing a vibration, said crystal positioned in an opening having walls, wherein an interaction between an incoming electromagnetic radiation and said vibration of said crystal optimizes a frequency of said electromagnetic radiation, collecting said incoming electromagnetic radiation from a source through said first end, shifting the frequency of said electromagnetic radiation within said channel to achieve an optimal frequency of said electromagnetic radiation; and positioning a photovoltaic material a distance away from said channel. 
     A fifth general aspect relates to a device comprising a conversion channel including: a first end configured to accept ambient electromagnetic radiation, the ambient electromagnetic radiation having an initial frequency, a second end configured to allow the ambient electromagnetic radiation to exit, and at least two opposing walls connecting the first end and the second end, wherein the at least two opposing walls include one or more crystals, the at least two opposing walls being separated by at least one-half of a wave length; wherein when the ambient electromagnetic radiation interacts with the one or more crystals of the at least two opposing side walls, the initial frequency of the ambient electromagnetic radiation being repeatedly increased to an optimal frequency. 
     A sixth general aspect relates to a device comprising a first side wall and a second side wall connected forming a conversion channel, the conversion channel having a first end and a second end, wherein the first side wall is constructed out of one or more crystals and the second side wall is a reflective surface; wherein the conversion channel captures ambient infrared radiation having an initial frequency from an environment proximate the first end, and repeatedly increases the initial frequency to an optimal frequency through a plurality of interactions between the ambient infrared radiation and at least one atom of the one or more crystals making up the second wall, further wherein the at least one atom is moving toward the incoming infrared radiation during a single interaction. 
     A seventh aspect relates generally to a method of converting ambient heat to electricity comprising providing a conversion device including: a first end configured to accept ambient electromagnetic radiation, the ambient electromagnetic radiation having an initial frequency, a second end configured to allow the ambient electromagnetic radiation to exit, and at least two opposing walls connecting the first end and the second end, wherein the at least two opposing walls include one or more crystals, the at least two opposing walls being separated by at least one-half of a wave length, utilizing vibration of one or more crystals making up the at least two opposing walls, wherein the vibration causes atoms of one or more crystals to move in a direction towards the accepted ambient electromagnetic radiation, and repeatedly increasing the initial frequency of the ambient electromagnetic radiation through interactions with the at least two opposing walls until the ambient electromagnetic radiation reaches an optimal frequency. 
     The foregoing and other features of construction and operation will be more readily understood and fully appreciated from the following detailed disclosure, taken in conjunction with accompanying drawings. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       Some of the embodiments of this invention will be described in detail, with reference to the following figures, wherein like designations denote like members wherein: 
         FIG. 1  depicts a cross-section view of an embodiment of an optimization device while incident electromagnetic radiation enters the channel; 
         FIG. 2  depicts a numerical table of an embodiment of various calculations including the number of Doppler interactions for a given frequency; 
         FIG. 3  depicts an enlarged cross section view of an embodiment of a vibrating atom of the side walls of the channel; 
         FIG. 4  depicts a magnified cross section view of an embodiment of a vibrating atom moving in an identical direction as the electromagnetic radiation; 
         FIG. 5  depicts a magnified cross section view of an embodiment of a vibrating atom moving in the opposite direction as the electromagnetic radiation; 
         FIG. 6  depicts a top view of an embodiment of movement of the side walls when undergoing vibrations; 
         FIG. 7  depicts a cross-section view of an embodiment of an optimization device wherein no planar surface connects side walls; 
         FIG. 8A  depicts a cross-section view of an embodiment of an optimization device with a pair of minors placed between the side walls; 
         FIG. 8B  depicts a top view of an embodiment of an optimization device with a pair of minors placed between the side walls; 
         FIG. 9  depicts a cross section view of an embodiment of an optimization device, wherein a single crystal structure is used; 
         FIG. 10  depicts a cross section view of an embodiment of an optimization device wherein a dual use, single crystal is used; 
         FIG. 11  depicts a cross section view of an embodiment of a plurality of channels in series and parallel; and 
         FIG. 12  depicts a cross-section view of an embodiment of an ambient heat conversion device. 
     
    
    
     DETAILED DESCRIPTION OF THE DRAWINGS 
     Although certain embodiments of the present invention will be shown and described in detail, it should be understood that various changes and modifications may be made without departing from the scope of the appended claims. The scope of the present invention will in no way be limited to the number of constituting components, the materials thereof, the shapes thereof, the relative arrangement thereof, etc., and are disclosed simply as an example of an embodiment. The features and advantages of the present invention are illustrated in detail in the accompanying drawings, wherein like reference numerals refer to like elements throughout the drawings. 
     Various embodiments of an electromagnetic radiation frequency altering and optimizing device of the present invention may optimize incident solar electromagnetic radiation  80  into an energy range that may be used in conjunction with a target, such as a photovoltaic material  70 . Incident electromagnetic radiation  80  may include radio waves, microwaves, terahertz radiation, infrared radiation, visible light, ultraviolet radiation, X-rays and gamma rays. Optimizing solar electromagnetic radiation  80  involves changing, altering, or shifting the frequency of the incident electromagnetic radiation  80  (and therefore wavelength and energy level) using Doppler shifts. A Doppler shift may either “blue shift” or “red shift” incident electromagnetic radiation to a desired optimal frequency. By performing multiple Doppler shifts, a desired optimal frequency may be attained. 
     A Doppler shift may change the frequency and wavelength of an incident electromagnetic radiation wave when the reflector is moving in relation to the incident wave. When incident electromagnetic radiation  80  is reflected off a surface that is moving generally in the opposite direction as an electromagnetic radiation wave, a “blue shift” occurs, and the resulting reflected electromagnetic radiation has a higher frequency than the initial electromagnetic radiation wave. Conversely, when an electromagnetic radiation wave is reflected of a surface which is moving in a direction generally the same direction of the electromagnetic radiation  80 , a “red shift” occurs, and the resulting reflected wave has a lower frequency. By coordinating or synchronizing the vibration of the plurality of crystals  17  comprising the inner reflective surface  15  and multiplying the effects of small Doppler shifts, an optimal electromagnetic radiation  85  may be obtained. Thus, the optimal electromagnetic radiation  85  has generally undergone blue or red shifts to achieve the desired optimal frequency before it is focused toward a target, such as a photovoltaic material  70 . 
       FIG. 1  depicts a single stage channel  5  designed to optimize and alter frequency of incident electromagnetic radiation  80 . The channel  5  may also be referred to as a Doppler channel, pathway, opening, conduit, duct, fluting, passage, pipe, tunnel, cavity or the like. The channel  5  may have a first end  10 , a second end  20 , a planar surface  7  connecting at least two side walls  25 ,  26 . Moreover, the channel  5  may have an inner reflective surface  15 , described in more detail infra. The shape of the channel  5  may vary. In an exemplary embodiment, the channel  5  will have two opposing, parallel side walls  25 ,  26 , forming a 90° angle with the planar surface  7 ; the at least two side walls  25 ,  26  may be separated by a distance, d, which may vary depending on the desired optimal frequency. A separator  12  is positioned within the channel  5 . In one embodiment, the separator  12  may be positioned proximate the first end  10 . Also located within the channel  5  is a focusing member  13 . In one embodiment, the focusing member  13  may be positioned proximate the second end  20 . Furthermore, at least one absorption area  14  is located on the inner reflective surface  15 . In many embodiments, the channel  5  may have multiple absorption areas  14 . 
     The channel  5  may receive, accept, capture, and/or collect incident electromagnetic radiation  80  at the first end  10 . When the incident electromagnetic radiation enters the channel  5  at the first end  10 , it may contact, pass through, reach, etc., the separator  12  which may be located proximate the first end  10 . The separator  12  may be any device capable of separating and directing incident electromagnetic radiation  80  into its component frequencies by refraction, diffraction, or filtering. In one embodiment, the separator  12  may be a prism. In another embodiment, the separator  12  may be a diffraction grating. In another embodiment, the separator  12  may be a system of filters. In yet another embodiment, the separator  12  may be concave and/or convex minors. The separator  12  may also be any combination of the aforementioned devices. 
     The separator  12  may separate incident electromagnetic radiation  80  into component frequencies and may direct the separated frequencies toward a side wall  25 ,  26  of the channel  5 , with each frequency or group of frequencies targeted to a particular location within the channel  5 . Furthermore, incident electromagnetic radiation  80  which may already be at or near the optimal and usable energy and frequency range for a particular target, such as a photovoltaic material  70 , may be separated and directed by the separator  12  to travel straight through the channel  5 , with minor incidental or no reflective interactions with the inner reflective surface  15 . As a result, the pre-optimal electromagnetic radiation  83  may be immediately directed toward the second end  20  and photovoltaic material  70 , free from any frequency modification or alteration. The determination of whether the incident electromagnetic radiation  80  is near or at optimal frequency may depend on the particular photovoltaic material  70 , and other variables known to those skilled in the art. 
     Other frequencies of incident electromagnetic radiation  80 , otherwise not useable by the photovoltaic material  70  may be separated and directed by the separator  12  to be reflected off the at least two side walls  25 ,  26  of channel  5 , where it may interact with the inner reflective surface  15 . The interaction between the inner reflective surface  15  and the incident electromagnetic radiation  80  performs a Doppler shift to the otherwise unusable frequency for the photovoltaic material  70 . The Doppler shift performed on the incident electromagnetic radiation  80  may shift, alter, change, etc., it to a frequency that may be usable by the photovoltaic material  70 . Because the otherwise unusable incident electromagnetic radiation  80  may undergo a change in frequency to a desired optimal frequency (or within the photovoltaic material&#39;s  70  usable energy range), the efficiency of a photovoltaic material  70  may be increased. In one exemplary embodiment, the separator  12  may separate and direct various frequencies of incident electromagnetic radiation  80  in different directions and may establish the reflection sequence which may result in the proper Doppler shifts according to the desired optimal frequency. 
     Furthermore, a focusing member  13  is located proximate the second end  20  of the channel  5 . The focusing member  13  may be any lens, grating, system of minors, a transparent medium, and the like. The focusing member  13  may direct and/or focus all electromagnetic radiation traveling through the channel  5  in a path not parallel to the side walls  25 ,  26  to exit the second end  20  such that the optimal electromagnetic radiation  85  exits the channel  5  and hits the target  70 . For example, the optimal electromagnetic radiation  85 , the pre-optimal electromagnetic radiation  83 , and incident electromagnetic radiation  80  may exit the second end  20  at a 90° angle to the channel  5 , or may exit the second end  20  at any angle and spread outward, and come into contact with a photovoltaic material  70 . In an alternate embodiment, the focusing member  13  may direct and/or focus exiting electromagnetic radiation at angle greater or less than 90°. Moreover, waste electromagnetic radiation  87  (discussed infra) may not reach the focusing member  13  because it is collected and/or absorbed by the absorption areas  14 ; thus, 100% of the incident electromagnetic radiation does not always pass through the focusing member  13 . 
     With continued reference to  FIG. 1 , incident electromagnetic radiation  80  that is not at an optimal frequency for the photovoltaic material  70  (target) may enter the channel  5  at the first end  10  and reach the separator  12 , and may be directed toward the sides walls  25 ,  26  at an angle, Ø, calculated to achieve desired optimal frequency shifts as the incident electromagnetic radiation  80  reflects within the channel  5 . For example, incident electromagnetic radiation  80  may enter the channel  5  and need to undergo a “blue shift” to change, alter, or shift its frequency to fall within the usable range of the photovoltaic material  70 . The separator  12  may direct the incident electromagnetic radiation  80  toward at least one of the two side walls  25 ,  26  at a calculated angle, Ø, to perform the Doppler shift required to achieve the necessary frequency alteration. The incident electromagnetic radiation  80  that is separated and directed by the separator  12  may be called directed electromagnetic radiation  81 . When the directed electromagnetic radiation  81  reaches the inner reflective surface  15  at an angle, Ø, a controlled, calculated Doppler shift may occur. A Doppler shift may occur when the directed electromagnetic radiation  81  interacts with the inner reflective surface  15  because of vibrating crystal atoms in the reflective surface  15 . Moreover, if the contact occurs at a point in the crystal&#39;s vibration where the crystal is moving generally in the opposite direction as the directed electromagnetic radiation  81 , the result of the interaction may be a “blue shift”, and the resulting frequency may be increased. 
     The inner reflective surface  15  may be made up of a plurality of crystals  17 , which may be suited for vibrating at high to ultra-high frequencies. Alternatively, the inner reflective surface  15  may comprise a single crystal suited to vibrate at high to ultra high frequencies. A crystal may be defined as a solid material whose atoms, molecules, or ions are arranged in a repeating pattern extending in all three spatial dimensions. The inner reflective surface  15  may contain ultra-high frequency vibrating atoms, which may or may not be made of crystals. Furthermore, the inner reflective surface  15 , crystal, or plurality of crystals  17  may be comprised of Silicon, SiO 2 , LiNbO 3 , GaAs, GeAsSe, BaF 2 , ZnSe, ZnS, Al 2 O 3 , ceramics, metals, carbon, diamond, beryllium, iron, brass, copper, tin, nickel, chromium, magnesium, barium titanate, zinc sulphide, tourmaline, hydrogen phosphate, magnesium oxide, silicon nitrate, silicon carbon, hafnium or any combinations or mixtures thereof. It is noted that reflective gasses and liquids may also be used, for example, enclosed in Plexiglas, which could be used as a substrate or other structural material. In the various embodiments of the Doppler channel  5 , the reflective crystal surface  15  may be attached, fastened, adhered, or otherwise affixed to the inner surfaces of the side walls  25 ,  26  of the channel  5 . The reflective crystal surface  15  may also be grown by using techniques that are well known in the art, (e.g. the vapor-liquid-gas method or the surface diffusion method, among other methods). The side walls  25 ,  26  may be made of any material that provides rigidity, structure, and allows for adherence or growth of crystals, and resists the moderate heat levels that may develop when the channel  5  may be continuously exposed to the heat of the sun, or other sources electromagnetic radiation. Furthermore, the side walls  25 ,  26  may be smooth or may be uneven and rough, and may also be circular, rectangular, or may be just any practical shape. Accordingly, the side walls  25 ,  26  may be made out of materials including, but not limited to, a metal, a plastic or thermal resistant polymer, a suitable substrate for growing crystals such as silicon, and the like. In an alternative embodiment, the crystals may form the side walls  25 ,  26 . 
     In yet another embodiment, where a single crystal is used, the side walls  25 ,  26  may be comprised of a single crystal. In another embodiment, a plurality of crystals  17  may be placed on a structural material, such as a substrate. The optimization device  100  may only need a very thin shell to operate. For example, the thinnest material that possesses the desired characteristics and may be economical to machine manufacture might be the best material to act as a shell around the crystal or plurality of crystals  17 . The advantage of using a shell may be that less energy is required to achieve the vibrations of the crystalline atoms. However, if the optimization device  100  does not need to be synchronized, or is designed to operate without synchronized vibrations, than any construction material may be used to support the inner reflective surface  15 , the crystal, or the plurality of crystals  17 . In most embodiments, the crystals will be placed on a substrate to provide some support, which may be anything that does not adversely affect the performance of the crystals. In one exemplary embodiment, the crystals may be embedded in Plexiglas covers to provide support, and may allow the placement of the side walls  25 ,  26  and the separator  12  to be fixed. For example, the side walls  25 ,  26  and the separator  12  and focusing member  13  may be inserted in a panel of Plexiglas or they may be placed on a workboard which could be covered with Plexiglas. 
     Positioned somewhere inside the channel  5 , and located on the inner reflective surface  15  of the at least two side walls  25 ,  26  may be an absorption area  14 , or a plurality of absorption areas  14 . This absorption area  14  may be used to absorb incident electromagnetic radiation  80  which would otherwise be wasted as heat. For example, the absorption area  14  may collect or absorb unusable electromagnetic radiation. Unusable electromagnetic radiation may be electromagnetic radiation that may not be utilized by the photovoltaic material  70 , or any given target. This unusable electromagnetic radiation may be known as waste electromagnetic radiation  87 . As waste electromagnetic radiation  87  is absorbed by the absorption area  14 , the temperature of the absorption area  14  may be increased. The absorption area  14  may be in conductive communication with the inner reflective crystal surface  15 , thereby allowing heat generated by absorption of waste electromagnetic radiation  87  in the absorption areas  14  to be conducted to the reflective crystal surface  15 , and raise the temperature of the inner reflective crystal surface  15 . As the temperature of the inner reflective crystal surface  15  rises, the atoms of the crystals may vibrate with increasing frequency. The vibrations of the crystal caused by the absorption of waste electromagnetic radiation  87  may optimize (i.e. perform a Doppler shift) the incident electromagnetic radiation  80  when there is an interaction between the incident electromagnetic radiation  80  and the vibrations of the crystal. The absorption area  14  may be made of a non-reflective surface, any optically absorbing material, or any other material that may absorb electromagnetic energy and transform it to another form of energy, such as heat. 
     The presence of at least one absorption area  14  or more than one absorption area  14  located throughout the channel  5  may allow the optimization device  100  to be completely self-sustaining. No external power or energy need be used to power the vibrations of the crystals, although an external electric current may be applied to the channel  5  to heat the crystals and power the vibrations. For example, the incoming electromagnetic radiation  80  entering the first end  10  may be separated and directed and may come into contact with a spot on the surface of one of the side walls  25 ,  26  where an absorption area  14  is located. Thus, the absorption area  14  collects the waste electromagnetic radiation  87  which would normally be wasted as heat, or is unusable, and may use it to generate the vibrations of the crystals. Advantageously, the optimization device  100  may operate without requiring energy output from an external source. Accordingly, creating vibrations of the crystal atoms forming the side walls  25 ,  26  of the channel  5  by use of the energy contained in the ambient temperature and/or the energy contained in the waste electromagnetic radiation  87  may properly and solely power the optimization device  100 . 
     Moreover, the waste electromagnetic radiation  87  may be harvested and utilized to generate the vibrations in a number of other ways such as directing the waste electromagnetic radiation  87  to select areas of the side walls  25 ,  26  which are not reflective, in particular, towards absorption areas  14 , such that the waste electromagnetic radiation  87  energizes the crystals by the energy transferring by means of phonons throughout the crystal causing the desired vibrations. In addition, after the incident electromagnetic radiation  80  passes through the separator  12  and is separated into its component frequencies, waste electromagnetic radiation  87 , such as waste portions of the spectrum like infrared, may be directed towards the side walls  25 ,  26  at an angle, Ø, such that absorption occurs rather than reflection. Also, the waste electromagnetic radiation  87  may be directed by a series of minors to the edge of the side wall  25 ,  26  to induce vibrations. Furthermore, the side walls  25 ,  26  may be constructed out of a substance which may reflect the higher frequencies but absorb the infrared portions of the spectrum, and this absorption may be utilized as the energy source for the vibrations. 
     If a piezoelectric substance is utilized in comprising the side walls  25 ,  26 , such as quartz crystal, electricity and a feedback loop may be applied to cause the substance to vibrate in a desired fashion. A feedback loop may obtain a constant oscillation. Although, small amounts of energy may be needed to maintain the vibrations in a quartz crystal, the potential energy output, especially if sunlight is concentrated towards the optimization device  100  should exceed the energy needed to cause and maintain the harmonic vibrations in the crystals. For example, mirrors may be used to capture and/or concentrate the sunlight from a greater area and direct it towards the optimization device  100 . It is noted that the energy produced by the solar cells prior to the activation of the optimization device  100  may be more than sufficient to activate the constant oscillation which may energize the side walls  25 ,  26  (the crystal atoms). Likewise, reflected electromagnetic radiation  84  is being both upshifted and downshifted, the net effect of the incident electromagnetic radiation  80 , with respect to the channel  5 , may be neutral. 
     Referring again to  FIG. 1 , a distance, d, between the two side walls  25 ,  26 , the length, L, of the channel  5  may be carefully calculated to ensure that directed electromagnetic radiation  81  which undergoes a blue shift on its first interaction with the inner reflective surface  15  reaches an opposite side  26  (if the first interaction was with side wall  25 ) of the channel  5  and reflects off another crystal atom which is also moving generally in the same direction as the reflected electromagnetic radiation  84 , resulting in a further blue shift. Conversely, incident electromagnetic radiation  80  frequencies that need to undergo a red shift to become optimized may enter the channel  5  and follow the same procedure to perform a blue shift, except the contact between the directed electromagnetic radiation  81  and the vibrating crystal atoms in the inner reflective surface  15  may occur at a point in the crystal&#39;s vibration where the crystal is moving generally in the opposite direction as the directed electromagnetic radiation  81 , resulting in a red shift, and thus the frequency decreases. Moreover, the difference between the speed of light and the speed of a vibrating atom in the channel  5  is so great that minor errors in calculated distances, d and L, may be harmless with respect to the Doppler interactions. 
     The vibration speed of the atoms in the crystal surface  15  may vary depending on temperature. As the temperature rises, the atoms may tend to vibrate faster. As the speed of vibration changes, the amount of Doppler shift that occurs when the directed electromagnetic radiation  81  interacts with the moving atom may change accordingly. By changing the ambient temperature of the reflective material coating or comprising the side walls  25 ,  26 , the amount of Doppler shift and the number of reflections in a channel  5  may be changed. As incident electromagnetic radiation  80  interacts with the side wall  25 ,  26  of the channel  5 , there may be some waste electromagnetic radiation  87 , which may be lost as heat. The waste electromagnetic radiation  87  may be collected by the absorption areas  14  to use the resulting heat from the absorption to heat the surrounding reflective surfaces  15 , thereby increasing the frequency of vibration. Furthermore, this heat may be used to impart energy to the reflective surfaces  15  in order to provide energy to perform the Doppler shifts and vibrate the crystal atoms. 
     While it is understood that the directed electromagnetic radiation  81  undergoes a number of Doppler shifts, the specific number of Doppler shifts that a particular frequency must undergo to reach a desired or optimal electromagnetic radiation  85  may be calculated by observing certain mathematical formulas regarding Doppler effect in light. A number of variables may be determined to calculate ΔF, which is the change in frequency that occurs with each Doppler shift (i.e. each interaction between directed electromagnetic radiation  81  and inner reflective surface  15  undergoes a change in frequency equal to ΔF). Specifically, ΔF is the frequency of the source, Fs, minus the frequency of the listener, FL, (ΔF=Fs−FL). The frequency of the source, Fs, is the frequency of the particular incident electromagnetic radiation  80 , and may be known to those having skill in the art (See  FIG. 2  for a table of typical frequencies of various colors of the spectrum). The frequency of the listener, FL, may be calculated by observing an equation: 
     
       
         
           
             
               F 
               ⁢ 
               
                   
               
               ⁢ 
               L 
             
             = 
             
               
                 
                   
                     ( 
                     
                       c 
                       - 
                       v 
                     
                     ) 
                   
                   
                     ( 
                     
                       c 
                       + 
                       v 
                     
                     ) 
                   
                 
               
               × 
               F 
               ⁢ 
               
                   
               
               ⁢ 
               s 
             
           
         
       
         
         
           
             wherein c=speed of light (299,792,458 meters per second) and v=velocity of the light source moving towards the listener
 
It should be understood that other formulas may be used to determine the frequency of the listener, and one having skill in the art may calculate a weighted average from each formula to determine the frequency of the listener. The velocity of the light source moving toward the listener, v, may be also be considered the speed of a vibrating atom. A typical atom vibrates at a speed of 1,117 meters per second (2500 miles per hour), but may vary considerably depending on, for example, temperature. Thus, in one embodiment, ν may be plugged into the FL formula as 1,117 meters per second. Once all variables are known, ΔF may be calculated, and in many embodiments, ΔF=2.4×10 9 .
 
           
         
       
    
     Next, calculating the number of Doppler shifts to be performed to reach the optimal (target) electromagnetic radiation  85  may be achieved by subtracting the source frequency, Fs, by the optimal (target) frequency, Fopt, and dividing the difference (Fs−Fopt) by ΔF (2.4×10 9 ). For example, green light may have a source frequency, Fs, of 6.0×10 14  Hertz (or cycles per second), and assume the optimal (target) frequency, Fopt, is 4.5×10 14 . Subtracting Fs (6.0×10 14 ) by Fopt (4.5×10 14 ), yields a difference of 1.5×10 14 , which may be understood as the required amount of Doppler shift (as a frequency). The required amount of Doppler shifts may then be divided by ΔF (2.4×10 9 ) to calculate the number of Doppler interactions/shifts. In the instant example, the number of Doppler shifts needed to reach the optimal (target) frequency, Fopt, is 66,964.  FIG. 2  includes a table calculating the number of Doppler shifts for multiple frequencies on the visible electromagnetic spectrum, but it should be understood that the number of Doppler shifts may be calculated for frequencies other than visible light in accordance with the principles of the present invention. 
     Furthermore, the maximum speed in the vibration may occur when the atom is closest to equilibrium and stops at each end. The vibrating object must stop in each end of its vibration and reverse its direction. Thus, the meaningful useful portion of the vibration for a Doppler interaction may only occur during a center phase (high velocity) of the vibration. The center phase may also be split in half to reflect the fact that during one part of the cycle the atom is traveling in one direction, and during the second half of the cycle the atom may be traveling in the opposite direction. For example, to shift the frequency of directed electromagnetic radiation  81  in one direction, only approximately one-quarter of each vibration cycle may supply the useful velocity in the appropriate direction for the desired Doppler interaction. However, if there are at least two different optimal (target) frequencies, Fopt, and the source frequency, Fs, is between the optimal (target) frequencies, both halves of the center phase (high velocity) of the vibration cycle may be used. Moreover, when the vibration is in one direction, the Doppler shift may occur towards one desired frequency (i.e. a red shift) and when the atom vibrates in the opposite direction, the useful portion of the vibration cycle in the opposite direction may result in a converse Doppler shift (i.e. blue shift). However, if all of the optimal (target) frequencies, Fopt, are either below the source frequency, Fs, only one-quarter of the vibration cycle which supplies the useful velocity in the appropriate direction for the desired Doppler interaction may be used. In an alternate embodiment, both high velocity phases of the vibration may be utilized. 
       FIG. 3  depicts a portion of the channel  5 , wherein a vibrating atom  50  of side wall  25 ,  26  has a vibrating range, r. The atoms of the plurality of crystals  17 , or a single crystal, vibrate in directions  55 ,  56 . When the reflected electromagnetic radiation  84  contacts the vibrating atom  50  moving in the same direction  56 , a red shift occurs, and the frequency of the reflected electromagnetic radiation  84  is decreased (See  FIG. 4 ). Conversely, if the reflected electromagnetic radiation  84  contacts the vibrating atom  50  moving in the opposite direction  55 , a blue shift occurs, and the frequency of the reflected electromagnetic radiation  84  is increased (See  FIG. 5 ). In one embodiment, the vibrations of multiple vibrating atoms  50  are synchronized. 
     Referring now to  FIG. 6 , the channel  205  may be constructed such that side walls  225 ,  226  vibrate in an opposite phase of each other. For example, if the inside edge of side wall  225  is vibrating in one direction (e.g. to the right), then the opposite side wall  226  may vibrate in the opposite direction (e.g. to the left). This principle may be referred to as “synchronized-vibration” for the purposes of illustration and explanation of the following embodiments of the present invention. 
     In one embodiment, depicted in  FIG. 6 , the channel  205  may have two side walls  225 ,  226  constructed out of separate but identical crystal, which is capable of vibrating at high to ultrahigh frequencies to perform desired Doppler shifts. The crystal need not be exactly identical, but near as practicable to each other. The side walls  225 ,  226  may move toward each other, and simultaneously may move away from each other; the side walls  225 ,  226  vibrate in opposite phase to achieve “synchronized-vibration.” The side walls  225 ,  226  may be constructed out of a rigid crystal, such as quartz, and rigid crystals may vibrate at certain resonant frequencies and harmonics. Placing two like-manufactured crystals, which comprise side walls  225 ,  226 , in close proximity to each other, but not so close as to interfere with each other, when synchronized may vibrate in the same manner. Without any significant changes to the local environment surrounding side walls  225 ,  226 , “synchronized-vibration” may occur. Once “synchronized-vibration” has been started, a harmonic may continue its harmonic motion indefinitely. Thus, to achieve a desired Doppler shift, each side wall  225 ,  226  may be placed a certain distance, d, apart from each other. In another embodiment, there may be an array of side walls  225 ,  226  placed in a series, as depicted in  FIG. 11 . Furthermore, the system  200  or array may be coated with a coating material  45  such as Plexiglas to strengthen or reinforce the system  200  or array. The coating material  45  may slow down the speed the speed of light through the channel  205 , but the net effect may be negligible in terms of the construction of the device  200  and may strengthen the device  200 , thereby increasing its durability and may lessen variations in the counter-phase synchronicity of the side walls  225 ,  226  caused by external influences. 
     Referring now to  FIG. 7 , side walls  325 ,  326  may not be connected to each by a planar surface  7 , thus having two independent side walls  325 ,  326 . Once the channel  305  is constructed, the crystals  315  may be tuned such that each crystal  315  may be vibrating in an opposite phase to the adjacent crystal. For example, the crystals  315  of side wall  325  may be configured and tuned to vibrate in one direction, and the crystals  315  of side wall  326  may be configured and tuned to vibrate in the opposite direction. In this manner, the two side walls  325 ,  326  may be both vibrating towards each other at the same time and opposite each other at the same time (“synchronized-vibration”). Initially starting the crystals  315  to vibrate in a given pattern may be done by methods known to those skilled in the art. Because the adjacent crystals of side walls  325 ,  326  may be in the same environment, subject to the same temperature variations, shocks, and like trauma, the net effect may be that the crystals  315  continue with their harmonic vibrations in the same out of phase manner as initially set relative to each other. For example, if one crystal  315  changes in frequency, all of the adjoining crystals may suffer the same trauma, and may change in the same manner. The harmonic properties of the crystals  315  will lessen the possibility of gradual degradation of the counter-synchronicity of the adjoining crystals once set. Moreover, it is understood that the crystals  315  may be reset, and during this time maintenance may be performed on the system  300 , including but not limited to repair and cleaning. 
     Returning to the previous example calculating the number of Doppler shifts required to reach the optimal (target) frequency, Fopt, for green light, the number of Doppler shifts required is approximately 66,964. In an embodiment of device  300 , the 66,964 Doppler shifts may be accomplished in 1/10 th  of ¼ of a cycle. More particularly, if the atoms vibrate at 30,000 hertz, the time frame to perform a Doppler shift may be one-quarter of one vibrating cycle. Based on the useful one-quarter cycle, there is approximately 120 thousandths or 0.00000833 seconds (8.33×10 −6 ) of useful time. In this amount of useful time, light traveling at 299,792,458 meters per second may travel 2,498 meters. During the useful phase of a single cycle there may be a total distance of 249,827 centimeters distance for light to travel during which the useful cycle occurs. Therefore, if side walls  325 ,  326  are placed apart from each other a distance, d, of 0.373 centimeters, 66,964 Doppler shifts may occur in 1/10 th  of the ¼ th  of the useful cycle, and the incident green light has been optimized to reach the optimal (target) electromagnetic radiation 85. 
     With continued reference to  FIG. 7 , the height of the side walls  325 ,  326  may be set to varying heights, and no particular height may be required. It is understood that a channel  305  may be on a nanoscale, and may be configured to operate with various nanotechnology and the like. The only limiting criteria of the channel  305  may be the distance, d, between side walls  325 ,  326  to eliminate any interference with the vibrations of each side wall  325 ,  326 . 
       FIGS. 8A and 8B . depict an embodiment of an optimization device  400  having a time/distance extender  450  located proximate to side walls  425 ,  426 . Because the channel  405  may only utilize one-quarter of the incident electromagnetic radiation  80 , it may be desirable to recycle the incident electromagnetic radiation  80  that is not used. The unused electromagnetic radiation may be called waste electromagnetic radiation  87 . One possible way to recycle waste electromagnetic radiation  87  may be to construct a time/distance extender (TDE)  450 . More than one TDE  450  may be used in a given channel  405 , and may face each other to facilitate repeated reflection. The TDE  450  may be a gap with mirrors or a reflective material at each end of the gap with a lens  455  at each end of the reflective material that may allow light which has not been directed to the target, to be reflected between the minors for a sufficient amount of time approximately equal to the amount necessary so that the side walls  425 ,  426  have passed through a partial phase of a vibration cycle. After a delay, the otherwise waste electromagnetic radiation  87  may be redirected to the first end  410  of optimization device  400  or towards the side walls  425  and  426  the lenses  455  may direct the waste electromagnetic radiation  87  in the TDE  450  to the side wall where the Doppler shift occurs and the waste electromagnetic radiation  87  may then be reflected back through the TDE  450  to the opposite side wall. After sufficient Doppler interactions, the TDE  450  may be bypassed and the waste electromagnetic radiation  87  may be directed to either the target  70  or thereafter recycled to the first end  410 , or directed through another channel  405  in series or succession. Thus, the waste electromagnetic radiation  87  may be repeatedly recycled until it passes through the channel  405  at an optimal phase such that a desired frequency may be obtained. In this manner, the waste electromagnetic radiation  87  which may not be otherwise be utilized because it did not pass through the channel  405  during a useful velocity vibration phase, may be time delayed until it passes through the channel  405  during a useful velocity vibration phase. With the use of a TDE  450 , up to half of the available light may be utilized. For example, if a lower frequency is sought, then in such case, the light which is Doppler shifted to a lower frequency and the light which pass through the channel  405  during the low velocity vibration phase which was just prior to the downward conversion Doppler shift phase may be utilized. 
     Although waste electromagnetic radiation  87  may be recycled with the use of the TDE  450 , incident electromagnetic radiation  80  may also enter the channel  405  and reflect through the TDE  450  as shown by  FIGS. 8A and 8B . The incident electromagnetic radiation  80  may enter the channel  405  and reflect off one of the side walls  425 ,  426  and contact one of the minors of the TDE 450. Once the incident electromagnetic radiation  80  enters the channel  405  and interacts with side wall  425  or side wall  426 , it may be referred to as reflected electromagnetic radiation  84 . The reflected electromagnetic radiation  84  may reflect back and forth within the TDE  450  moving in both a horizontal and vertical direction through the channel  405 . While moving horizontally, the reflected electromagnetic radiation  84  may pass through one of the lens  455 . In many embodiments, there may be four lens  455 , but there may also be only two lens  455 . Lens  455  may change the angle of reflection and direct the reflected electromagnetic radiation  84  at approximately a 90° towards a side wall  425 ,  426 . The side wall  425 ,  426  may then reflect the reflected electromagnetic radiation  84  perpendicularly back through lens  455 , which may again change the angle of reflection, angling the reflected electromagnetic radiation  84  back towards the minors of the TDE  450 . Thus, the electromagnetic radiation  84  moves horizontally to one edge of the TDE  450  until it contacts the lens  455 , wherein it may reverse its course and move horizontally towards the opposite edge of the TDE  450  until it contacts the opposing lens  455 . Simultaneously, the reflected electromagnetic radiation  84  may be moving vertically down the channel  405  towards the second end  420 . This process may continue until the reflected electromagnetic radiation  84  has moved vertically down the channel  405  a sufficient distance where the TDE  450  mirror substrate no longer extend. In other words, the TDE  450  may be dimensioned to have a shorter height, h, than the height, L, of the side walls  425 ,  426 , as depicted in  FIG. 8A . 
       FIG. 9  depicts a channel  505  whereby a single crystal is implemented. The single crystal comprising both side walls  525 ,  526 , may act as a standing wave, and the entire crystal may vibrate consistently. For example a single crystal may be in the shape of a tuning fork, whereby each prong of the tuning fork may comprise a side wall  525 ,  526 ; the vibrating relationship between two points on the inside of the tuning fork design may be consistent. For example, all points on the single crystal may move at the same time. Based on this consistent movement of the single crystal in the shape of a tuning fork, when the right inside edge of the left fork moves to the left, the left inside edge of the right fork also moves to the left. In accordance with the calculations discussed supra, to obtain a Doppler shift, the inside edge of the opposite side of the fork to be out of phase by one-half cycle. Furthermore, to obtain the desired Doppler shift as the directed incident electromagnetic radiation  82  reflects off each of the inside edges of the channel  505 , it may be necessary to cause the space between the two inside edges of the channel  505  to be such that when the directed incident electromagnetic radiation  82  travels from one inside edge to the opposite inside edge, the opposite inside edge is one-half of a cycle out of phase to the prior edge. 
     To shorten the distance, d, between each of the side walls  525 ,  526 , a time/distance extender (TDE)  550  may be inserted between the side walls  525 ,  526  of the channel  505 . TDE  550  may be a device that, in effect, holds the light for a given period of time. The TDE  550  may be a gap with opposing planar surfaces covered by a reflective surface such as a mirror and lenses  555  at each end so as to direct the waste electromagnetic radiation  87  and/or reflected electromagnetic radiation  84  in the TDE  550  to the side wall  525  where the Doppler shift occurs and the waste electromagnetic radiation  87  and/or reflected electromagnetic radiation  84  may then be reflected back through the TDE  550 . More than one TDE  550  may be used in a given channel  505 , and may face each other to facilitate repeated reflection. The TDE  550  may also cause the directed electromagnetic radiation  81  to reflect between its minors numerous times so as to create a delay in time. However, after the light has traveled a considerable distance (back and forth in the TDE), the light may be directed back towards the first end  510  of the channel  505 , or may be directed to an inside edge of the channel  505  to undergo a Doppler shift. In an exemplary embodiment, there is no TDE medium  560  between the more than one TDE  550 . In another embodiment, a TDE medium  560  with a high index of refraction may be positioned between the more than one TDE  550  to add structural support and to lessen the need to execute many reflections. For example, a TDE medium  560  with a high index of refraction may slow the speed of light which may lessen the distance the light needs to travel. 
     To determine the distance, d 1 , between each TDE  550 , consider that the atoms vibrate at 30,000 hertz, and the time frame to perform a Doppler shift may be one-quarter of one vibrating cycle. If a TDE medium  560  made out of Plexiglas, which has an index of refraction of 1.51, is placed between two TDE  550 , and the distance, d 1 , between the TDEs  550  is 3.3 centimeters, the light may reflect 100,000 times in the TDE  550  before it hits one of the side walls  525 ,  526 . The number of reflections may be calculated as follows: refraction index (e.g. 1.51 for Plexiglas) divided into the speed of light (i.e. 299,792,458 meters per second) equals a net speed (i.e. 198,538.51 meters per second). 
     However, other materials may be used as a TDE medium  560 . For example, a TDE medium  560  made of silicon may be used, which has a refraction index of 4.0. The higher the index of refraction of the TDE medium  560 , the lower the effective speed of light. For example, if silicon is used as the TDE medium  560 , the net effective speed of light may be reduced to approximately 74,948,114 meters per second. The net effective speed may be multiplied by the length of time which passes in one-half cycle; the light would then need to travel only 1,249 meters to result in a delay of one-half cycle. Thus, if 100,000 reflections between the TDEs  550  were desired, the distance, d 1 , may be approximately 1.25 centimeters. However, if the distance, d 1 , remained at 3.33 centimeters, then the amount of reflections may only be approximately 37,357 in the TDE  550 . In yet another non-limiting example, if incident green light needed to be shifted to red light (target frequency), and the number of required Doppler shifts may be 66,964, the total amount of time to create the shift may be 1.116 seconds. 
       FIG. 10  depicts a Dual Use Single Crystal Solution (DUSCS). DUSCS may utilize both sides of a single independent crystal as the inside of side walls  625 ,  626  of the channel  605 . In this manner, a single, vibrating crystal may create all the vibrations necessary for the Doppler interactions. The DUSCS may eliminate the need to synchronize the vibrations of an independent crystal, and may eliminate the need to implement a large crystal. The DUSCS may function by having incident electromagnetic radiation  80  vibrate off one side of a vibrating crystal, and then subsequently direct the directed electromagnetic radiation  81  towards a time distance extender  650 . After the requisite delay, the time distance extender  650  directs the directed electromagnetic radiation  81  towards the opposite side of the single, vibrating crystal. This may occur after one-half of the vibration cycle has passed. Accordingly, the Doppler interactions may always be synchronized because the DUSCS uses the same, vibrating crystal; there also may not be any phase issues. 
     Furthermore, the time distance extender  650  may not have to be placed between the “forks” of a single crystal because DUSCS employs a single, solid crystal. Thus, the TDE  650  may be constructed having opposing mirrors separated by a distance, d 1 , approximately equal to the length or width of the optimization device  600 . In one embodiment, the optimization device may be created using one-half meter panels, and the distance, d 1 , between the mirrors attached to the TDEs  650  may be approximately 50 centimeters. Moreover, if a TDE medium  660 , such as Plexiglas is placed between the TDEs  660 , only 6,618 reflections may be necessary to result in a one-half cycle time delay if the crystal is vibrating at 30,000 hertz. A further advantage of DUSCS may be that DUSCS greatly simplifies the needed accuracy in setting the reflection angles in the TDE  660 , and it may also lessen the losses which may occur upon each reflection. In addition, another TDE  660  may be utilized as a delay so as to recycle the incident electromagnetic radiation  80  which passes through one-quarter of the channel  605  when the vibration speed is insufficient to provide a beneficial Doppler interaction and achieve the optimal frequency. 
     With continued reference to  FIG. 10 , the crystal may be any size which is optimal for manufacturing purposes, and the channel  605  may be constructed in accordance with the dimensions of the crystal. For example, the crystal may be 0.01 cm in height, 0.001 cm in width, and 1.0 cm in length. 
       FIG. 11  depicts a plurality of channels  705  used in series and/or parallel order to form an array of Doppler channels  705  to achieve optimal Doppler shifting capability. The array of channels  705  may be the same approximate structure as channel  5  having a first end  710  and a second end  720 , but not all channels  5  may have a focusing member  13 . Instead, the directed electromagnetic radiation  81  may travel directly through a transparent structural member  790  and into a successive separating member  712  of another, proximately located, Doppler Channel  5 . Therefore, in an array of Doppler channels  705  array, each channel  5  and subsequent Doppler channel(s) to which it may be connected may be calculated or tuned to receive and perform a Doppler shift to a particular range of frequencies. For example, when a channel  5  is tuned to either red shift or blue shift to a particular range of frequencies, incident electromagnetic radiation  80  entering the separating member  712  are separated according to the frequencies for which each channel  5  is intended. The separating member  712  may direct the directed electromagnetic radiation  81  to the series or array of Doppler channels  705  tuned specifically to shift and optimize those particular frequencies. Finally, optimized electromagnetic radiation  85  is produced and may be focused onto a target, wherein the target may operate more efficiently as a result of the increased amount of optimal electromagnetic radiation  85  contacting the target. In one exemplary embodiment, the target may be a photovoltaic material. 
     Referring now to  FIG. 12 , with general reference to  FIGS. 1-11 , an embodiment of a ambient heat conversion device  800  is described. Components such as a planar surface  807 , a crystal(s)  817 , reflective surface  815 , and at least two opposing walls  825 ,  826  may share the same or substantially the same structure and functions as planar surface  7 , crystals (and atoms  50 ), and the side walls  25 ,  26  described supra with respect to other embodiments. However, embodiments of ambient heat conversion device  800  may have a conversion channel  805 , the conversion channel  805  may include a first end  810 , a second end  820 , at least two side walls 825, 826. Other embodiments of ambient heat conversion device  800  may include a conversion channel  805  including: a first end  810  configured to accept ambient electromagnetic radiation  880 , the ambient electromagnetic radiation  880  having an initial frequency, F I , a second end  820  configured to allow the ambient electromagnetic radiation  880  to exit, and at least two opposing walls  825 ,  826  connecting the first end  810  and the second end  820 , wherein the at least two opposing walls  825 ,  826  include one or more crystals, the at least two opposing walls  825 ,  826  being separated by at least one-half of a wave length; wherein when the ambient electromagnetic radiation  880  interacts with the one or more crystals of the at least two opposing side walls  825 ,  826 , the initial frequency, F I , of the ambient electromagnetic radiation  880  being repeatedly increased to an optimal frequency, F OPT . Further embodiments of conversion device  800  may include a first side wall  825  and a second side wall  826  forming a conversion channel  805 , the conversion channel  805  having a first end  810  and a second end  820 , wherein the first side wall  825  is constructed out of one or more crystals and the second side wall  826  is a reflective surface; wherein the conversion channel  805  captures ambient infrared radiation  880  having an initial frequency, F I , from an environment proximate the first end  810 , and repeatedly increases the initial frequency, F I , to an optimal frequency, F opt , through a plurality of interactions between the ambient infrared radiation  880  and at least one atom  50  of one or more crystals making up the first side wall  825 , further wherein the at least one atom  50  is moving toward the incoming infrared radiation  880  during a single interaction. 
     The ambient heat conversion device  800  follows the scientific principle that when electromagnetic radiation reflects off a moving object, the frequency of the reflected radiation becomes wither high (i.e. blue shifted) or lower (i.e. red shifted), depending on the relative speed of the object towards the light source. If an object, such as an atom  50  of a crystal in a side wall  825 ,  826 , is moving toward the light source, such as ambient electromagnetic radiation  880 , the frequency may become higher (i.e. blue shifted). The one or more crystals used in conversion device  800  may include Silicon, SiO 2 , LiNbO 3 , GaAs, GeAsSe, BaF 2 , ZnSe, ZnS, Al 2 O 3 , ceramics, metals, carbon, diamond, beryllium, iron, brass, copper, tin, nickel, chromium, magnesium, barium titanate, zinc sulphide, tourmaline, hydrogen phosphate, magnesium oxide, silicon nitrate, silicon carbon, hafnium, reflective gas, reflective liquid, or any combinations or mixtures thereof. 
     Ambient heat, ambient electromagnetic radiation, ambient infrared radiation, and the like, may not always have an initial frequency, F I , high enough to meet a threshold to produce, or be converted into electricity. Thus, conversion device  800  may repeatedly upshift, or blueshift, the ambient electromagnetic radiation  880  through repeated Doppler interactions within the conversion device  800  until the resulting frequency is high enough so that electricity will be produced when the blueshifted radiation interacts with a target  70 , such as a photovoltaic device. For example, the initial frequency, F I , of ambient electromagnetic radiation  880  may need to be increased to 4.1×10 14  Hz. The resultant radiation, or the blueshifted radiation that interacts with a target  70  may be referred to as optimal radiation  885 , and may have an optimal frequency, F OPT . Generally, the difficulty in producing/causing the required blue shift is that the energy required to achieve the speeds/velocity necessary to obtain such a Doppler shift (e.g. blue shift) may greatly exceed any useful energy which might thereby be produced. Thus, the conversion device  800  can solve this problem by harnessing the movements or vibrations of matter (e.g. movements and/or vibrations of the crystal atoms  50  in a side wall  825 ,  826 ) which may naturally occur in a non-zero temperature environment. For instance, the conversion device  800  may utilize the vibration movement which already exists or takes place in various environments. To the extent heat energy is converted into electricity, the ambient heat energy replaces the loss; accordingly, the conversion device  800  may utilize an unlimited source of “free” energy anywhere on the planet. 
     Moreover, the conversion device  800  may be designed to obtain numerous Doppler shifts during a single favorable vibration phase of an atom, such as a crystal atom  50 . If the initial frequency, F I , of ambient electromagnetic radiation  880  are high enough and if vibration speeds/velocity are fast enough, it may be possible that all Doppler interactions can occur during a single vibration phase of an atom, and may eliminate a need for a time distance extender, such as TDE  450 ,  550 ,  650 . Examples of this situation may be co-generation environments wherein “waste” heat is generated, such as in nuclear and fossil fuel power plants, in high temperature industrial processes, or engine compartments. Thus, embodiments of conversion device  800  may harvest electricity from waste, or unused emitted heat/energy. 
     Referring still to  FIG. 12 , the ambient, or background, electromagnetic radiation  880 , such as infrared radiation, may be captured, collected, accepted, etc., proximate the first end  810  of the device  800 . The first end  810  of the device may also be referred to as an input end. At the input end, or first end  810 , of the device, the ambient electromagnetic radiation  880  may also be focused and directed into the channel  805 . However, in many embodiments, the conversion device  800  need not direct the radiation  880  through a frequency splitter proximate the first end  810  because the ambient temperature and the frequency may be relatively consistent. The conversion device  800  may be designed or customized to a temperature range of a particular location or environment to increase the consistency of the radiation  880 . Furthermore, in environments or locations which emit more heat, and thus emit higher frequency radiation, the conversion device  800  need not optimize the frequency proximate the first end  810 . 
     As the ambient radiation  880  enters the first end  810  of the device  800 , the radiation, having an initial frequency, F I , can contact or be directed to contact one of the side walls  825 ,  826  of the channel  805 . The angle at which the ambient radiation entering the channel  805  contacts one of the side walls  825 ,  826 , may be at any angle; however, in many embodiments the angle of interaction is close to perpendicular. Embodiments of conversion device  800  mat include a lens, prism, minor, and the like to direct the incoming ambient electromagnetic radiation at specific angles depending on the desired Doppler interaction with the side walls  825 ,  826 , and crystals therein. Upon reflecting off one of the side walls  825 , the ambient radiation  880  is blue shifted (i.e. increase frequency), and continues towards the opposing side wall  826  for another Doppler interaction (i.e. another blue shift). The side walls  825 ,  826  of channel  805  of conversion device  800  may be separated by only a very small distance to obtain numerous Doppler shifts (i.e. blue shifts) during a single favorable vibration phase of an atom. For example, the distance between a first side wall  825  and a second side wall  826  may be at least one half of a wave length, wherein the wave length is determined by the initial frequency, F I , of the ambient radiation  880 . In other words, the opposing side walls  825 ,  826  may be separated by at least 5,000 nanometers. Further embodiments of the conversion device  800  may construct the side walls  825 ,  826  some multiple of half wave lengths apart from each other to promote uniformity on construction of the device  800 . In addition to the uniformity in construction, increased efficiencies due to harmonics can be obtained if the side walls  825 ,  826  are separated by a multiple of half wave lengths. Furthermore, at least one of the opposing side walls  825 ,  826  may include or be made of a single or a plurality of crystals. If only one side wall  825  includes or is made of a plurality of crystals, the opposing side wall  826  may be a reflective surface. In many embodiments, both of the side walls  825 ,  826  include a plurality of crystals, wherein the crystals may vibrate, setting the atoms  50  in motion either toward or away any incoming ambient or reflected radiation. If one of the side walls  826  utilizes a mirrored substance, the reflections from the mirrored substance may be random; therefore, most (potentially all) useful Doppler interactions may occur from the interaction between the radiation (ambient or reflected) and the vibrating atoms  50  of the side wall  825  containing, or made of crystal(s). It is contemplated that if only one side wall  825  includes a plurality of crystals, no synchronization may be needed, thereby simplifying construction. 
     Alternatively, if both opposing side walls  825 ,  826  utilize, include, are constructed of, etc., one or more crystals, then useful interactions may occur from the interaction between the radiation (ambient or reflected) and the vibrating atoms  50  of both of the opposing side walls  825 ,  826 . In embodiments where both of the side walls  825 ,  826  utilize crystals, there may be a need for synchronization. Synchronization involves synchronizing the crystals in the opposing side walls  825 ,  826  so that the atoms  50  of the crystals in the first side wall  825  vibrate/move towards the atoms  50  of the crystals in the second side wall  826  at the same time so that the ambient radiation  880  being reflected off of the opposing side walls  825 ,  826  during a favorable vibration phase shall Doppler shift in the same manner (i.e. both blue shift). However, the need for synchronization may depend on the different between the initial frequency, F I , of the ambient radiation  880  and the desired or optimal frequency, F opt . For example, if the desired frequency shift (e.g. change in frequency (Hz), or desired increase in frequency) is small, then non-synchronized Doppler side walls  825 ,  826  may be used as, statistically, favorable interactions may occur sufficiently often so as to result in a favorable net increase in frequency. In contrast, if a greater frequency shift is needed, the side walls  825 ,  826  may be synchronized for optimum results. One method of synchronization may include applying an electrical charge to the conversion device  800 , in particular, to the side walls  825 ,  826 . Those having skill in the art should appreciate that different means may be used to apply an electrical charge, for example, a regulator may provide or apply the electrical charge sufficient to cause synchronization of the crystal atoms  50  in the side walls  825 ,  826 . Furthermore, the resonance frequency (i.e. frequency of the vibrating crystals) may be selected so that it is slightly above the resonance frequency that would occur near the ambient temperature level. In this manner, the bulk of the energy causing the Doppler interaction may be that supplied by the ambient heat as opposed to the electrical charge causing the resonance. One purpose of the resonance may be to synchronize the timing such that favorable Doppler interactions occur. For instance, higher resonance frequencies can be applied, but may result in a need for a greater input energy (i.e. other than from the ambient area). Therefore, once a desired frequency is obtained, the emitted radiation  885  may be directed to target  70 , such as a PV cell, wherein the target  70  may generate electricity. 
     Moreover, approximately 3650 Doppler interactions can occur during a single positive vibration phase of an atom. Accordingly, the Doppler shift/change in frequency during a single positive vibration phase of an atom may be 3.24×10 11  Hz. By determining the initial frequency, F I , or input frequency, and calculating, determining, utilizing, and/or providing the required/desired optimal frequency, F opt , or output frequency, the conversion device  800  may be constructed, dimensioned, structured, etc., to achieve the necessary number of Doppler interactions. For example, if the amount of the required blueshift (frequency shift—increase) is greater than what can be achieved during a single favorable phase of a vibration of an atom (e.g. 3.24×10 11 ), then the reflected radiation may be directed through a time distance extender  450 ,  550 ,  650  after each favorable vibration phase and then redirected to one of the side walls  825 ,  826  to achieve repeated favorable Doppler blue shifts until the optimal frequency, F opt , is reached. 
     Furthermore, the frequency of the radiation passing through the channel  805  may be split proximate the second end  820 , or output end, such that the radiation having a frequency equal to the optimal frequency, F opt , may be directed towards the target  70 , and the radiation having a lower frequency than the optimal frequency, F opt , may be redirected to same device  800  or another device  800  placed in series or parallel. However, radiation having a frequency lower than the optimal frequency, F opt , (e.g. waste energy) may not be a concern because it will be converted into ambient heat that may increase the ambient temperature, thereby increasing the vibration speed of the crystal atoms and the initial frequency, F I , of the ambient radiation  880 . If the device  800  is placed in a higher ambient temperature environment, such as the cooling towers in an industrial or traditional power generation facility, the device  800  may be designed so that all or most of the Doppler interactions may occur during a useful phase of one vibration of an atom  50 . 
     Referring still to  FIG. 12 , an embodiment of a ambient heat conversion device  800  may be described in the following example: If the device  800  is placed in an environment where the ambient temperature is 55° F. (286 K), such as an average basement environment, the ambient radiation  880  has an average wave length of 10,133 nanometers and an initial frequency, F I , of 2.958575×10 13  Hz, and the desired optimal frequency, F opt , is 4.1×10 14  Hz, then a frequency shift (i.e. blue shift—increase in frequency) of 3.804×10 14  Hz is needed. Because the ambient temperature is 55° F. (286K), this example assumes that the average speed of the atom  50  is 900 meters per second (m/s). Therefore, the average Doppler shift (i.e. change in frequency) per interaction (i.e. radiation contacting vibrating crystal of side walls  825 ,  826 ) is approximately 8.9×10 7  Hz. Further, if the average favorable distance of the vibration during a favorable vibration phase is 111 nanometers (i.e. width of the atom  50 , for example, a silicone atom) at 900 meters per seconds for 1.233×10 −10  seconds, during which time radiation would travel 0.0369744 meters, then 3650 favorable Doppler interactions (e.g. of 10,132 nanometers) may occur during a single favorable vibration phase of an atom  50 . The 3650 Doppler interactions may result in a frequency shift/increase of 3.24×10 11  Hz, which depending on the initial frequency, F I , and the optimal frequency, F opt , may result in a favorable frequency change after a single favorable interaction. To achieve the optimal frequency, F opt , of 4.1×10 14  in this example, a total of 4,274,382 Doppler interactions would be required. Because 3650 Doppler interactions occur during a single favorable vibration phase, the optimal frequency, F opt , may be achieved with 1,171 favorable atom  50  vibration phase interactions. Because the distance between each interaction is on the micron level, the duration of all of the interactions may be 4.5×10 −7  seconds. One having skill in the art should understand that thousands, hundreds of thousands, millions, etc., of Doppler interactions may occur each second to constantly convert ambient heat and radiation to an optimal frequency, F opt , which is directed to a target  70  to generate electricity. A lens, prism, minor, and the like may be used to direct the emitted radiation  885  toward the target  70 . Those skilled in the art should also appreciate that the variables used in the above example may change, and may vary based on the environment and target  70  requirements. For instance, the distance of vibration may be more than or less than the width of an atom  50 . 
     Some of the advantages of conversion device  800  include low cost for producing energy, especially considering the alternative methods of producing energy may be costly, unfeasible, unsustainable, and the like. Conversion device  800  may not be dependent on wind, tides, sunlight, or any of the ephemeral needs which are generally associated with green/clean energy. Additionally, device  800  operates continuously once placed in its environment, and may not need/require backup generators. For example, the ambient heat in an environment may be recharged by the ambient heat from an adjacent area. The conversion device  800  may also be placed/installed in numerous environments, including basements, foundations, tunnels, caves, inside of electrical device, engine compartments. This flexibility in placement may eliminate the need for transmission lines, which are costly and a source for energy loss. Furthermore, device  800  may consistently and continuously produce renewable energy at night in hostile environments, such as a battlefield, lessening or possibly eliminating the need for logistical supplies. 
     Moreover, the device  800  is lightweight and small which may ease transport and handling of the same. Due to the compact nature of the device  800 , it may be used/utilized as a charger or a power cell battery source. For instance, it could be built into cellular phones or other electronic devices to provide a primary or back power source. In addition, the device could be constructed to provide an efficient infrared radiation collector. It is further contemplated that hundred, thousand, even millions of devices  800  may be placed on a single chip, even if each device  800  only produces a small amount of electricity the aggregate effect may be sufficient. Embodiments of the device  800  may be used for other applications in addition to those expressly disclosed herein. 
     Referring to  FIGS. 1-12 , embodiments of a method of optimizing electromagnetic radiation is also disclosed. The method of optimizing electromagnetic radiation may comprise the following steps: providing a channel having a first end, a separator positioned proximate the first end, a second end, a focusing member positioned proximate the second end, at least two parallel walls having an reflective surface, wherein the at least two parallel side walls connect the first end and the second end, and at least one absorption area located on the reflective surface, vibrating the at least two parallel walls, wherein the parallel walls contain at least one crystal capable of vibration, directing the incoming electromagnetic radiation toward the at least two parallel walls, wherein contact between the incoming electromagnetic radiation and the vibration of the at least one crystal alters a frequency of the electromagnetic radiation toward the optimal frequency. 
     The method may also comprise the steps of: determining an optimal frequency relative to a usable frequency of a target, separating an incoming electromagnetic radiation into component frequencies, passing the optimal frequency through the second end, capturing a portion of the incoming electromagnetic radiation in the absorption area to cause the vibration, inserting a pair of minors between the at least two side walls, and positioning the target near the second end. 
     Another embodiment of a method of optimizing electromagnetic radiation frequency to increase the efficiency of a photovoltaic cell may include the steps of providing a crystal positioned in a channel undergoing a vibration, wherein an interaction between an incoming electromagnetic radiation and the vibration of the crystal optimizes a frequency of the electromagnetic radiation, accepting the incoming electromagnetic radiation from a source through the first end, shifting the frequency of the electromagnetic radiation within the channel to achieve an optimal frequency of the electromagnetic radiation, and positioning a photovoltaic material a distance away from the channel. 
     Referring still to  FIGS. 1-12 , an embodiment of a method of converting ambient heat to electricity may include the steps of providing a conversion device  800  including: a first end  810  configured to accept ambient electromagnetic radiation  880 , the ambient electromagnetic radiation  880  having an initial frequency, F I , a second end  820  configured to allow the ambient electromagnetic radiation  880  to exit; and at least two opposing walls  825 ,  826  connecting the first end  810  and the second end  820 , wherein the at least two opposing walls  825 ,  826  include at least one crystal, the at least two opposing walls  825 ,  826  being separated by at least one-half of a wave length, utilizing vibration of the at least one crystal least two opposing walls  825 ,  826 , wherein the vibration causes atoms of one or more crystals to move in a direction towards the accepted ambient electromagnetic radiation  880 , and repeatedly increasing the initial frequency, F I , of the ambient electromagnetic radiation  880  through interactions with the at least two opposing walls  825 ,  826  until the ambient electromagnetic radiation  880  reaches an optimal frequency, F opt . Embodiments of this may further include the steps of obtaining an optimal frequency, F opt  relative to a usable frequency of a target  70 , dividing the incoming ambient electromagnetic radiation into component frequencies, passing the ambient electromagnetic radiation  880  through the second end  820 , providing a pair of reflective surfaces between said at least two side walls  825 ,  826 , extending a time and a distance in which the ambient electromagnetic radiation  880  travels within the conversion device  800 , and placing a target  700  proximate or otherwise near the second end  820 . In one embodiment, the target may be a semiconductor. In another embodiment, the target may be a photovoltaic cell. Furthermore, the conversion device  800  may be placed in at least one of a high temperature environment and a low temperature environment. 
     Various modifications and variations of the described apparatus and method will be apparent to those skilled in the art without departing from the scope and spirit of the invention. Although this invention has been described in connection with specific embodiments, outlined above, it should be understood that the invention should not be unduly limited to such specific embodiments. Various changes may be made without departing from the spirit and scope of the invention.