Abstract:
An optical sensor arrangement includes two sensors arranged one behind the other. The operational spectral ranges of the sensors match, and the first sensor forms an attenuation filter for the second sensor, which is arranged behind the first sensor.

Description:
BACKGROUND AND SUMMARY OF THE INVENTION 
       [0001]    Exemplary embodiments of the invention relate to an optical sensor arrangement. 
         [0002]    Optical sensor arrangements are, for example, used for the detection of pulsed laser sources that signal a threat. These lasers can be classified according to wavelength and radiation intensity:
       Beamrider weapon systems, near infrared region (NIR)region, a few mW/m2 to a few W/m2 and   Target designators and rangefinders, 1064 nm, beam intensity up to a few MW/cm2.       
 
         [0005]    A saturation requirement is placed on laser detectors (which are intended to detect a radiation intensity of a few mW up to a few MW), that the sensor (detector) may not saturate, so that the dynamic range comprises at least  6  orders of magnitude. At the same time the detection of pulsed laser radiation requires high time resolution of the sensor. These requirements cannot be fulfilled with a single sensor that is known from the prior art, but sensor arrangements are usually selected that comprise two sensors S 1 , S 2  disposed adjacent to each other with respectively associated entry windows F 1 , F 2 , wherein each individual sensor respectively detects only part of the desired dynamic range ( FIG. 1 ). 
         [0006]    If the sensor is also equipped with an optical arrangement in order to optimize the effective aperture of the sensor and the detected image angle, then each sensor is provided with a dedicated optical arrangement O 1 , O 2 . This increases the cost in terms of space and components for the design of a laser detector sensor. 
         [0007]    U.S. Pat. No. 5,428,215 discloses an arrangement comprising individual, parallel constructed channels for the detection of the dynamic range. The described sensor arrangement is known on the commercial market under the name HARLID®. 
         [0008]    Sandwich diodes, which utilize the principle of the “vertical color filter detector group”, are known from U.S. Pat. No. 6,632,701. These detectors are commercially available in the combination Si/InGaAs. They comprise a plurality of stacked semiconductor layers with n and p doping, wherein the resulting respective p-n junctions form photodiodes. The individual photodiodes operate wavelength-selectively in different wavelength ranges. A similar design principle is disclosed by U.S. Pat. No. 7,683,310 B1 in the form of photodetectors disposed in series, wherein the individual detectors are designed for different wavelengths. 
         [0009]    European patent document EP 0 236 035 A2 discloses a laser detector sensor, with which a plurality of linear detector arrays are disposed in the image plane of an imaging optical arrangement, which respectively monitor a strip section of the environment, wherein said strip sections are each at different distances from the sensor. 
         [0010]    These arrangements are undesirable due to the limited dynamic range. 
         [0011]    Exemplary embodiments of the invention are directed to a sensor arrangement with which the dynamic sensitivity is increased while maintaining the spectral wavelength range. 
         [0012]    The optical sensor arrangement according to the invention comprises a sensor for the detection of electromagnetic waves and an aperture associated with the sensor, wherein at least two sensors disposed in series are provided for the detection of the electromagnetic waves entering through the aperture. 
         [0013]    The at least two sensors disposed in series have matching spectral regions and cover the same region of the surroundings to be observed. The sensors are thus sensitive in coincident spectral regions. The sensors are exposed to radiation of the same wavelength but of different intensity. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWING FIGURES 
         [0014]    The invention and other advantages of the invention are explained in detail using figures. In the figures: 
           [0015]      FIG. 1  shows an exemplary sensor arrangement according to the prior art, 
           [0016]      FIG. 2  shows a schematic representation of two diodes disposed in series according to the invention together with the intensity profile within the diodes, 
           [0017]      FIG. 3  shows a sensor arrangement according to the invention. 
       
    
    
     DETAILED DESCRIPTION 
       [0018]    In the sensor arrangement according to the invention, at least two sensors disposed in series (upper part in  FIG. 2 ) use a common aperture and also a common optical arrangement (if an optical arrangement is necessary in an advantageous version of the invention). In the image plane of the optical arrangement there is a first diode D 1  that converts the incident radiation into an electrical photocurrent. This diode is designed such that the sensitive layer (p-n junction) is very thick. In this way the majority of the incident photons are absorbed in this layer and, according to the quantum efficiency, converted into electron-hole pairs. D 1  thus has high sensitivity, but at the same time is used as an effective attenuation filter for the second diode D 2  that is disposed downstream and that thus has low sensitivity. 
         [0019]    This will be illustrated by an example calculation, with which by way of example a dynamic range of  6  orders of magnitude is covered with two diodes, wherein each diode has a dynamic range of  3  orders of magnitude. As a result, in addition the ratio of the intensities absorbed in the respective p-n layers should be 1:1000. 
         [0020]    The absorption law I/(x)=I 0 ·e −a·x  applies, wherein I refers to the intensity at the depth x of the diode D 1  through whose surface the radiation I 0  is incident, and a is the coefficient of absorption of the diode D 1 . In the lower part of  FIG. 2  the intensity profile within diodes D 1 , D 2  is sketched with a solid line. 
         [0021]    As diode material, by way of example silicon with a coefficient of absorption in the near IR spectral region of 100 cm −1  is adopted. In order to absorb 99% of the intensity entering through the diode surface in the first diode D 1 , the thickness dl of the diode is selected as 0.46 mm: 
         [0000]        I   1   =I   0   ·e   −4.6 =0.01 ·I   0             S   D1   ∝I   0   −I   1 =0.99 ·I   0    
         [0022]    S D1  refers to the output signal of the diode D 1 , which is proportional to the absorbed intensity. In order to achieve the desired ratio of the absorbed intensities (I 0 −I 1 ):(I 1 −I 2 ), the thickness d 2  of the diode D 2  is specified as 0.01 mm, neglecting the absorption in the contact layers of the diodes D 1 , D 2 : 
         [0000]        I   2   =I   0   ·e   −4.7 =0.009 ·I   0             S   D2   ∝I   1   −I   2 =0.001 ·I   0             S   D1   :S   D2 ≈1000:1
 
         [0023]    In this example the thickness d 1  of the first diode D 1  must be selected to be very large in order to absorb 99% of the intensity, because the coefficient of absorption of silicon in the near infrared is relatively small. 
         [0024]    In one advantageous form of the invention, a partly mirrored layer is therefore provided between the diodes D 1 , D 2 . This layer is advantageously applied to the rear side of the IR sensitive Si diode D 1 , so that the reflected radiation passes through the diode layer twice; the thickness of the diode can be reduced without changing the component of absorbed radiation. Part of the radiation incident on the beam splitter minor is thus reflected according to the reflection coefficients R (dotted line in  FIG. 2  lower part), and part is accordingly (1−R) transmitted, wherein the internal absorption within the beam splitter layer is negligible (dashed line in  FIG. 2  lower part). 
         [0025]    In this case the above example calculation can be represented as follows. In order to absorb about 99% of the intensity entering through the diode surface in the first diode D 1 , the thickness d 1  of the diode D 1  is selected to be d1=0.23 mm, and the reflectance of the beam splitter is selected to be R=0.90: 
         [0000]        I   1   =I   0   ·e   −α·d     1   =0.1 ·I   0    
         [0000]        S   D1   ∝I   0   −I   1   +R·I   1 ·(1 −e   −α·d     1   )= I   0   −I   1 ·( R ·(1 −e   −α d     1   )−1)= I   0 ·(1 −e   −α·d     1     +R·e   −α·d     1     −R·e   −2·α·d     1   )=0.98 ·I   0  
 
         [0026]    In order to achieve the desired ratio of absorbed intensities, the thickness d 2  of D 2  is again set to 0.01 mm: 
         [0000]        I   2   =I   1 ·(1 −R )· e   −α·d     2     =I   0 ·(1 −R )· e   −α·(d     1     +d     2     ) =0.009 ·I   0  
 
         [0000]        S   D2   ∝I   1 ·(1 −R )− I   1 ·(1 −R )· e   −α·d     2     =I   0 ·(1 −R )·( e   −α·d     1     −e   −α·(d     1     +d     2     ) )=0.001 I   0  
 
         [0000]        S   D1   :S   D2 ≈1000:1
 
         [0027]      FIG. 3  shows a sensor arrangement according to the invention. The sensor arrangement SA is disposed in a housing G with a window F. The electromagnetic waves can be incident on the sensor arrangement SA through the window F. The sensor arrangement SA is formed of a first diode D 1  and a second diode  2 , wherein the diode D 2  is disposed after the diode D 1  in relation to the X axis. Each diode D 1 , D 2  comprises contact connections K 11 , K 12 , K 21 , K 22 , with which they are each connected to a signal processing means SV 1 , SV 2 . 
         [0028]    Diode D 1  is used here as a detector for high sensitivity, diode D 2  as a detector for low sensitivity. Both diodes are designed for the same operational wavelength region. 
         [0029]    An optical arrangement O is advantageously provided perpendicular to the X axis and is disposed between the stack formed of diode D 1  and diode D 2  and the window F. The stack formed of diode D 1  and diode D 2  is advantageously disposed so that the diode D 1  is positioned in the image plane of the optical arrangement O. 
         [0030]    A partly mirrored layer (not illustrated) is provided between diode D 1  and diode D 2 . Such a partly transparent beam splitter minor can, if it is made of a metallic layer, be used for contacting the adjacent contact surfaces KF of the two diodes D 1 , D 2  at the same time. 
         [0031]    Of course, cascading of more than two stacked diodes to further increase the dynamic range is possible, likewise a transfer to other spectral regions. 
         [0032]    One advantage of the invention is that the output signals of both diodes D 1 , D 2  acting as detectors for the laser sources to be observed are of the same order of magnitude. Thus the output signals can be further processed with essentially the same circuits for signal processing SV 1 , SV 2 . The sensor arrangement according to the invention also saves space and reduces the number of required optical components. 
         [0033]    The foregoing disclosure has been set forth merely to illustrate the invention and is not intended to be limiting. Since modifications of the disclosed embodiments incorporating the spirit and substance of the invention may occur to persons skilled in the art, the invention should be construed to include everything within the scope of the appended claims and equivalents thereof.