Abstract:
A cavity ring-down spectroscope includes a ring-down cavity. A trigger detector is optically coupled within the ring-down cavity to generate a signal to indicate a desired radiation level in the ring-down cavity. A controller is coupled to the trigger detector to control light provided to the ring-down cavity. A ring-down time may then be measured.

Description:
BACKGROUND 
       [0001]    Cavity ring-down spectroscopy (CRDS) systems include a cavity that reflects light within the cavity to provide a long path through a sample. The decay of light intensity from the cavity over time may be used to determine the strength of absorption of the sample. From a known absorption cross section at a probe wavelength, and the cavity loss from the sample measured by a ring-down time, a measurement of the sample, such as gas concentration, may be obtained. While achieving the input and output through a single mirror has significant benefits in terms of light intensity, some systems keep the cavity in resonance with a laser wavelength by tuning the path length using a piezoelectrically driven tuning mirror. Since a reflected portion of input light directly is coincident with ambient light, the former can perturb the measurement of cavity light and make it difficult to determine when light is coupled into the cavity or just reflected onto the detector without reaching the cavity. 
       SUMMARY 
       [0002]    A cavity ring-down spectroscope includes a ring-down cavity. A trigger detector is optically coupled within the ring-down cavity to generate a signal to indicate a desired radiation level in the ring-down cavity. A controller is coupled to the trigger detector to control light provided to the ring-down cavity. A ring-down time may then be measured. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0003]      FIG. 1  is a block diagram of a cavity ring-down spectroscope according to an example embodiment. 
           [0004]      FIG. 2  is a flow chart illustrating a method of operating the spectroscope according to an example embodiment. 
           [0005]      FIG. 3  is a block diagram of an alternative cavity ring-down spectroscope according to an example embodiment. 
           [0006]      FIG. 4  is a block diagram of an example system for performing methods according to an example embodiment. 
       
    
    
     DETAILED DESCRIPTION 
       [0007]    In the following description, reference is made to the accompanying drawings that form a part hereof, and in which is shown by way of illustration specific embodiments which may be practiced. These embodiments are described in sufficient detail to enable those skilled in the art to practice the invention, and it is to be understood that other embodiments may be utilized and that structural, logical and electrical changes may be made without departing from the scope of the present invention. The following description of example embodiments is, therefore, not to be taken in a limited sense, and the scope of the present invention is defined by the appended claims. 
         [0008]    The functions or algorithms described herein may be implemented in software or a combination of software and human implemented procedures in one embodiment. The software may consist of computer executable instructions stored on computer readable media such as memory or other type of storage devices. Further, such functions correspond to modules, which are software, hardware, firmware or any combination thereof. Multiple functions may be performed in one or more modules as desired, and the embodiments described are merely examples. The software may be executed on a digital signal processor, ASIC, microprocessor, or other type of processor operating on a computer system, such as a personal computer, server or other computer system. 
         [0009]      FIG. 1  is a block diagram of a cavity ring-down system (CRDS)  100  having a cavity  110  in which light is reflected between two or more mirrors through a sample containing molecules of interest. The cavity  110  may have several mirrors  115 ,  120 , and  125  in order to reflect the light, such as in a triangular path. Some of the mirrors, such as mirrors  120  and  125  may be totally reflective, such that no light transmits through them. Such mirrors improve the quality of the system  100 , since at least two of the mirrors do not contribute to a total transmission loss in system  100 . A high Q resonant structure is desired in one embodiment. Mirror  115  may be at least partially transmissive, allowing a portion of the reflected light to be detected by a ring-down detector  130 . 
         [0010]    In one embodiment, at least mirror  120  exhibits some light scattering, which is also a part of the total losses of the system  100 . An internal cavity intensity detector  135  is positioned proximate mirror  120  in order to detect the scatter loss. When the scatter loss reaches a predetermined threshold level, the pump light is stopped. In one embodiment, the light is provided by an input laser  140 , and is controlled by an acousto-optic (AO) modulator  145 . 
         [0011]    Scatter at ppm levels may be created in a mirror by a number of ways in various embodiments. In one embodiment, a film with an intentional controlled degree of crystallinity may be formed on a top surface of the mirror. Crystallinity can be generated by annealing to a sufficiently high temperature such that the thin film material generates scatter sites. Scatter may also be generated by roughing up the surface of the mirror. This can be done by gently milling the surface of the mirror with an ion beam to produce a controlled level of scatter in the ppm range which is generated by surface roughness. A desired amount of scatter can also be generated by having an index mismatch at a microscopic level by controllably adding impurities or scatter sites. In one embodiment, the level of scatter is small enough not to significantly adversely affect the power levels of laser light, yet large enough to be detected by internal cavity detector  135 . 
         [0012]    In further embodiments, the input laser and AO modulator may be combined in a single device, or a different device such as a mirror may be used to control whether light is pumped into the cavity  110  or not. The acousto-optic modulator (AOM), also referred to as a Bragg cell, uses the acousto-optic effect to diffract and shift the frequency of light using sound waves (usually at radio-frequency). 
         [0013]    At a predetermined light level, the trigger detector  135  signals the AO modulator  145  such as via a controller  150  to cause input radiation from laser  140  to be no longer provided to the cavity  110 . The ring-down detector  130  is positioned to measure the decay of light as transmitted through mirror  115 , without having to account for additional light being pumped into the cavity from the laser  140 . In one embodiment, the time it takes for the light within the cavity to decay, is representative of the amount or presence of an element within the cavity for which the light source and cavity are tuned to detect. 
         [0014]    The internal cavity intensity detector  135 , sometimes referred to as the trigger detector, may be mounted in a variety of different positions, such as near one of the mirrors within the cavity. The detector  135  may be positioned optimally where scatter occurs to efficiently detect the intensity of light being reflected within the cavity. In one embodiment, scatter off of one of the internal mirrors is observed. While the scattered light has low intensity since the mirror loss is low in the ppm range, the magnitude of the cavity light intensity provides a sufficiently strong signal for activating the AO modulator. In some prior approaches, a trigger detector is positioned outside the cavity and detects light transmitted through a mirror with a nominal 1 ppm or so transmission loss. The detector looks at the build up of light transmitted through this mirror. 
         [0015]    When the intensity in the internal detector  135  builds up to a high level, the detector triggers the AO modulator  145  via controller  150  which causes the input laser light to the cavity to extinguish. At this time, the only light reaching the decay detector is light from the cavity. The light may decay sufficiently within 10 μsec in one embodiment, allowing it to travel a long path length through the molecules, such as 3 kilometers in this embodiment. The light decays because of system losses, such as mirror transmission and scattering losses, and also because of absorption by a sample gas containing molecules of interest. In one embodiment, the loss due to the gas is comparable in magnitude to the system losses. 
         [0016]    For the period of time to charge the cavity with light and allow it to decay, on the order of a msec in one embodiment, the cavity is blind and can go out of resonance by thermal drifting. When the ring down is completed, normally within less than a msec, the input light may be redirected to the cavity via the AO modulator state change and a piezo mirror moves slightly and in conjunction with the trigger detector finds the new mirror position at which condition at which the internal cavity intensity is restored to begin another cycle. The piezo mirror may be any of mirrors  115 ,  120 . Mirror  125  usually does not have a piezoelectric element because it must transmit the laser light into the cavity and the exiting cavity light onto the detector. 
         [0017]    Controller  150  as shown receives sensed scatter information from detector  135  and controls the AO modulator  145  to extinguish light input into the cavity  110 . Controller  150 , or other separate controllers may be used to coordinate various other detectors, modulators and mirrors in various embodiments. 
         [0018]    In one embodiment, controller  150  or another controller assists in implementation of an algorithm as illustrated in a flowchart  200  in  FIG. 2 . At  210 , light is pumped into the cavity, and the cavity is optionally tuned to a desired frequency consistent with the light source and the molecules to be detected. The internal detector  135 , or ring-down detector  135  may be used to measure the light within the cavity  110  and assist in the tuning. 
         [0019]    At  220 , following the optional tuning, light intensity is detected within the cavity by internal detector  135 . The pumping is stopped at  230  when light in the cavity is detected at a predetermined threshold level. After the pumping is stopped, the ring-down detector  130  is used to detect the amount of time that it takes light to decay to a desired level at  240 . The process is repeated as indicated at  250 , again optionally including tuning to compensate at least for thermal drift. Multiple ring down measurements may be performed, and a statistical computation, such as average ring-down time, may be performed at  260  and associated with whether or not the desired molecule is present. The statistical analysis in some embodiments may allow detection of molecules in the range of parts per trillion. 
         [0020]    By using an internal intensity detector, the mirrors used to reflect light may have lower transmission losses, allowing a system to have a high Q. The only loss may be through a mirror allowing light to reach the ring-down detector. By detecting scatter using an internal detector, the direct laser light does not adversely affect the detection that triggers shutting off the laser. The use of a three mirror, triangular configuration preserves polarization of the laser light, further allowing for a resonator cavity having an increased quality factor, Q. It also allows the ring-down detector to not receive direct laser light. 
         [0021]    An alternative two mirror system is illustrated at  300  in block diagram format in  FIG. 3 . A laser  310  and AO modulator  315  provide light to a cavity  320  via a first mirror  325 . Light is reflected back and forth in cavity  320  between first mirror  325  and a second mirror  330 . An internal light detector  335  is positioned proximate second mirror  330  to detect light scattering representative of overall light intensity within the cavity  320 . A third mirror  340  is positioned such that the laser light passes through it to enter the cavity  320 , but also reflect light transmitted out of the cavity  320  through first mirror  325 . The light is reflected onto a ring-down detector  345 . This system  300  operates in a manner similar to that illustrated in  FIG. 2 , but utilizes only two mirrors to provide a long light path length through the molecules to be detected within the cavity. 
         [0022]    In one embodiment, a gas input  350  and output  355  may be provided. The gas containing molecules to be detected may be provided via the input  350  and removed from the cavity via output  355 . In one embodiment, the gas is provided and held within the cavity while detection occurs. In further embodiments, the gas may be flowing during detection so as not to interrupt an industrial process flow. The input and output may be smaller in cross section than the cavity, or may be the same size or even larger if desired. The ring shaped detector in  FIG. 1  may be used in a similar manner. In further embodiments, the ring shaped detector may be disposed within a larger pipe carrying molecules of potential interest. The ring shaped detector may be the same size as the pipe, and positioned similar to a washer between sections of pipe. 
         [0023]    A block diagram of a computer system that executes programming for performing the above algorithm is shown in  FIG. 4 . A general computing device in the form of a computer  410 , may include a processing unit  402 , memory  404 , removable storage  412 , and non-removable storage  414 . Memory  404  may include volatile memory  406  and non-volatile memory  408 . Computer  410  may include—or have access to a computing environment that includes—a variety of computer-readable media, such as volatile memory  406  and non-volatile memory  408 , removable storage  412  and non-removable storage  414 . Computer storage includes random access memory (RAM), read only memory (ROM), erasable programmable read-only memory (EPROM) &amp; electrically erasable programmable read-only memory (EEPROM), flash memory or other memory technologies, compact disc read-only memory (CD ROM), Digital Versatile Disks (DVD) or other optical disk storage, magnetic cassettes, magnetic tape, magnetic disk storage or other magnetic storage devices, or any other medium capable of storing computer-readable instructions. Computer  410  may include or have access to a computing environment that includes input  416 , output  418 , and a communication connection  420 . The computer may operate in a networked environment using a communication connection to connect to one or more remote computers. The remote computer may include a personal computer (PC), server, router, network PC, a peer device or other common network node, or the like. The communication connection may include a Local Area Network (LAN), a Wide Area Network (WAN) or other networks. 
         [0024]    Computer-readable instructions to execute methods and algorithms described above may be stored on a computer-readable medium such as illustrated at a program storage device  425  are executable by the processing unit  402  of the computer  410 . A hard drive, CD-ROM, and RAM are some examples of articles including a computer-readable medium. 
         [0025]    The Abstract is provided to comply with 37 C.F.R. §1.72(b) is submitted with the understanding that it will not be used to interpret or limit the scope or meaning of the claims.