Abstract:
The invention is directed to an arrangement for the optoelectronic recording of large-area fingerprints, particularly for acquiring prints of the entire palm of the hand. The object of the invention is to find a novel possibility for recording the papillary ridge pattern of a hand which permits a complete optoelectronic image recording with one-time placement of large-area concave skin parts without the use of optical beam paths that are subject to contamination and without having to accept a loss of resolution. This object is met, according to the invention, in that the support body for supporting the skin parts has the basic shape of a cylinder providing a portion of the outer surface with a sufficient radian measure and radius as support surface, the end faces of the support body are each provided with a conical recess which is arranged coaxially around the cylinder axis in order to couple in an illumination beam path and an imaging beam path through the surface lines of the conical recesses, and the imaging beam path and a linearly extending image sensor are rotatable synchronously around the cylinder axis in order to record successive line-shaped strips of the frustrated total reflection at the illuminated outer surface of the support body with the supported skin part.

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
   This application claims priority of German Application No. 10 2005 004 640.1, filed Jan. 28, 2005, the complete disclosure of which is hereby incorporated by reference. 
   BACKGROUND OF THE INVENTION 
   a) Field of the Invention 
   The invention is directed to an arrangement for the optoelectronic recording of large-area fingerprints, particularly for acquiring prints of the entire palm of the hand. It is used for the recording of personal features for identification services and forensic identification. 
   b) Description of the Related Art 
   In law enforcement identification services, fingerprints and handprints of individuals are taken in order to be able to establish their identity. For more than one hundred years, the recording of the patterns of the papillary ridges on the finger and hand has conventionally been carried out by inking the surfaces of the finger or hand and subsequently printing them on paper. With the availability of high-performance electronic sensors and computers, arrangements have become known which are used for direct electronic acquisition of the patterns without the intermediary of ink, paper and scanning of the print image. In this way, the electronic acquisition can be carried out substantially faster and, above all, with higher quality. 
   While there have been many diverse publications concerned with the electronic acquisition of prints of individual fingers (more exactly, the upper two joints of the finger), only few solutions are known for acquiring the palm of the hand. These solutions are directed to arrangements which are either limited in format and allow only part of the palm to be acquired in one process or which can acquire the entire full-size hand but do not reliably achieve the quality necessary for applications of this kind. 
   The pre-published application US 2002/0090147 A1 describes an arrangement for optically recording the patterns of the palm of a hand in which the pattern of the papillary ridges lying on a plane recording surface of a prism is rendered visible as an image by means of frustrated total internal reflection (FTIR). For this purpose, the prism which is made of an optical solid material (e.g., glass) is supported in a stationary manner and incorporated in an optical imaging beam path for imaging the hand supporting surface on an image sensor. A mirror which can be tilted in two axes in a controlled manner is located in the beam path to increase the resolution of the two-dimensional image recording sensor through a special method with multiple recording of the images and subsequent combination of the image data. 
   In this arrangement, it works out disadvantageously that the palm of the hand is more or less curved inwardly and for this reason does not make direct contact in its entirety with the recording surface so that relatively large areas (usually in the center of the palm) are not imaged (i.e., appear white or empty). A practical remedy can be to apply pressure to the top of the hand resting upon the recording surface. However, given the concave surface of the hand, this improves the imaging only to a certain extent because the increased contact pressure on the parts of the hand that already had good contact before presses the papillary ridges together and the pressed areas in the resulting image appear very dark with poor contrast and are therefore more difficult to evaluate. 
   U.S. Pat. No. 6,038,332 describes an arrangement for the optical recording of patterns on the palm of a hand. The curved surface of a transparent half-tube (a glass tube that is split along its length) serves as a stationary support for the palm. In the interior, it is ensured by means of a light rod which extends linearly along the curved surface and which illuminates the curved surface obliquely that only light which is scattered at the outer surface of the hand resting on the support is coupled into an optical imaging beam path by a mirror. The imaging of the palm of the hand in its second dimension is generated by motor-actuated rotation of the mirror and by optics on an image sensor which is essentially one-dimensional, read out in the form of (overlapping) partial images and put together to form the output image. 
   It is disadvantageous that the papillary ridges are made visible and imaged using the principle of scattered light because residues from perspiration excreted by the hand must be meticulously removed in their entirety after every placement of the hand so that scattered light from old prints is not detected again. 
   U.S. Pat. No. 6,175,407 also discloses an arrangement for the optical recording of the papillary ridge patterns on the palm of a hand in which a cylinder of solid optical material (e.g., glass) is rotatably supported, prisms being arranged near the end faces of this cylinder in order to radiate illumination light at a flat angle to the outer surface of the solid cylinder and couple out illumination light on the opposite side in an optical imaging beam path. 
   The outer surface of the cylinder serves as a support for a portion of the palm that is placed thereon. By means of this arrangement, the image of the supported papillary ridges is made visible portion by portion using the principle of frustrated total internal reflection (FTIR) and imaged by optics on a one-dimensional image sensor. The second image dimension is scanned by rotating the solid cylinder by means of the hand and is assembled line by line to generate the output image. However, when the hand is moved too quickly over the cylindrical surface, i.e., when the angular velocity exceeds a maximum permissible velocity, the signal processing means of the image sensor are incapable of supplying image data so as to be synchronized with the rotating movement and, consequently, the output image is also not assembled correctly. For this reason, very complex additional arrangements are provided for measuring the angular velocity and for braking the cylinder when its given rotational speed is exceeded. 
   Another basic problem consists in that the palm must be moved exactly without relative movement between the palm and the cylinder surface in order to avoid drastic errors in assembling the output image. With regard to practical realization further disadvantages consist in that there are considerable difficulties in sealing the optical light paths at both end faces of the rotatable cylinder in the transition to the prisms for preventing malfunction due to dust and moisture. 
   Further, another prior art arrangement for optical recording of the patterns of palms according to publication US 2004/0109245 uses a conical optical body. The principle of frustrated total internal reflection (FTIR) is again used in that a rod with line-shaped illumination is arranged in a bore hole along the axis of symmetry of the cone and the area of the conical outer surface which is accordingly illuminated virtually in a line-shaped manner is imaged downward on a line sensor through the planar base surface of the cone by imaging optics. The sensor and the optics are rigidly coupled to a rotatable plate which, further, is fixedly connected to the rod of the line-shaped illumination and all three components are moved jointly around the axis of symmetry of the cone. In this way, the outer surface is scanned line by line along the surface lines of the cone and an image of the palm that is placed thereupon one time is outputted as a quantity of individual lines corresponding to the outer surface of the cone that is unwound in a plane. However, in order to convert the image to a rectangular format, a coordinate transformation and resampling of the entire image must be carried out. While this operation is uniquely determined and is relatively simple to describe mathematically, it necessarily leads to contrast gradients in the effective optical modulation transfer function (MTF). Therefore, the MTF must deliver a substantially higher contrast in the raw image than is required (after transformation) in the output image according to relevant standards. Accordingly, the technical requirements for optics and sensor are appreciably higher than in an arrangement using the cylinder principle. This means that technical expenditure is considerably higher; otherwise, only a lower image quality (resolution in dpi) can be realized in the output image. 
   OBJECT AND SUMMARY OF THE INVENTION 
   It is the primary object of the invention to find a novel possibility for recording the papillary ridge pattern of a hand which permits a complete optoelectronic image recording with one-time placement of the print surfaces of a hand without the use of illumination beam paths or imaging beam paths that are inadequately sealed against environmental influences and without having to accept a loss of resolution or an appreciably increased expenditure on electronics for rectification of the image recordings and with a support surface that is curved in an ergonomically advantageous manner. 
   In an arrangement for optoelectronic image recording of prints of large-area concave skin parts, particularly whole handprints, with an optical support body with a convex support surface for supporting the skin parts with large-area contact with the support surface in order to realize an image recording based on frustrated total internal reflection, a light source for illuminating the support surface and a readout beam path for transmitting totally internally reflected illumination light to an image sensor, the above-stated object is met, according to the invention, in that the support body has the basic shape of a cylinder around a cylinder axis, which cylinder is not necessarily complete, the support body has a cylindrical outer surface with a radian measure and radius which are sufficient to provide at least one freely accessible portion of the outer surface as support surface for the large-area concave skin portion, in that the support body has a first end face and a second end face, each having a conical recess which is arranged coaxially around the cylinder axis, a light source extending at least parallel to a surface line of the conical recess is arranged in the conical recess of the first end face, and an imaging beam path is connected to the conical recess of the second end face, which imaging beam path images a strip of the support surface that extends in a line-shaped manner along a lateral line of the outer surface of the support body on a linearly extending image sensor at a total internal reflection angle in an axial plane given by the cylinder axis and the scanned strip, and in that the linearly extending image sensor and the imaging beam path are rotatable synchronously around the cylinder axis of the support body in order to record successive line-shaped strips of the frustrated total reflection at the illuminated outer surface due to the skin parts contacting the support surface and to combine them to form a two-dimensional image of the skin part resting on the support body. 
   A cylinder sector, preferably a quarter-cylinder to a half-cylinder, is advantageously used as a support body. 
   A tube which is supported so as to be rotatable around the cylinder axis is advisably provided for synchronous rotation of the image sensor and elements of the imaging beam path. The tube is arranged outside the conical recess of the support body or in a cylindrical recess of the cylindrical support body, which cylindrical recess extends coaxial to the cylinder axis. For the latter variant, the imaging beam path is advantageously folded into the tube and the cylindrical recess by means of a reflecting surface. 
   A stepper motor is advisably provided for the successive rotation of the tube around the cylinder axis to move the imaging beam path and the image sensor for scanning a series of strips of the support surface of the support body. 
   When a linear light source is used for illumination in an advantageous variant, this light source is fastened to the tube at the first front side of the cylindrical support body rigidly and parallel to the top of the conical recess and therefore so as to be movable around the cylinder axis synchronous with the imaging beam path. 
   The suitably shaped light source advantageously has a diffuser arranged downstream thereof in order to generate an intensive background illumination on the inner surface of the support body at least along a surface line of the support surface. A floodlight or plane projector that is arranged along the surface of the conical recess of the support body can be suitable for illuminating the inner cylindrical surface of the support body with an intensive background illumination along the entire support surface. 
   The light source is advisably a collimated linear light source which is arranged so as to be rotatable along the surface of the conical recess synchronous with the imaging beam path in order to generate a strip of intensive background illumination along the surface lines of the support surface on the inner surface of the support body. 
   The imaging beam path has at least one imaging optics arrangement for imaging a strip of the cylindrical surface of the support body on the linearly extending image sensor. 
   Further, the imaging beam path advantageously contains at least one optical element for correcting the perspective distortion of the strip of the support surface imaged on the image sensor. This optical element can advisably be at least one wedge-shaped prism for at least partial correction of the distortion. 
   In an advantageous variant, the imaging beam path has two prisms for correcting the perspective distortion and a reflecting surface for folding the beam path. The reflecting surface can be that of a separate plane mirror or the reflecting surface is arranged on one of the prisms as a reflecting back surface. Further, the reflecting surface is advisably a totally reflecting back surface of a prism of high-refractive index glass which corrects the image distortion. 
   In another variant for partial optical correction of the perspective distortion of the image, the first prism can be suitably integrated in the cylindrical support body in that the angle between the support surface and the conical recess as exit surface of the imaging beam path is appreciably larger than the angle of the total reflection and than the corresponding angle of the conical recess on the side of the illumination beam path. 
   Further, it is possible that the imaging beam path has a curved mirror for partial correction of the perspective distortion and for folding the beam path. 
   Heating elements are advisably arranged over a large area on the delimiting surfaces of the shaped support body that are formed as planar cut surfaces by cutting a cylinder sector or a cylinder segment, preferably in order to prevent condensation (but also to soften hard skin). 
   Further, calibrating devices are advisably arranged on the outer surface of the support body outside the support surface and are covered at least with hoods which protect against touching contact, contamination and external light in order to calibrate and check the imaging beam path. 
   The invention is based on the fundamental ideas of the use of the optical principle of frustrated total internal reflection (FTIR) in the interest of greater robustness in relation to hand perspiration and dust and of the need to prevent a relative movement of the hand (rolling) on a curved recording surface. Therefore, according to the invention, the outer surface of a stationary cylindrical base body serves as a hand support surface and conically beveled end faces are used for illuminating and reading out a strip along a surface line of the cylindrical support surface. For successive scanning of strips along a plurality of cylinder surface lines, the scanning beam path with the linear image sensor and—in case of a linear light source—also the illumination arrangement are rotated step by step around the cylinder axis of the base body by means of a rotating mechanism. The entire recording process is realized in a few seconds by suitable synchronization of the mechanical scanning movement around the cylinder axis and the rate of the data readout of the image sensor so that the hand can be held motionless without difficulty for this period of time. 
   A cylinder sector is sufficient for snugly fitting the palm against the cylindrical support surface in an ergonomically favorable manner. A housing which seals the interior space of the optical readout arrangement relative to the external environment so as to be tight against dust and water adjoins the edge of the outer surface of this cylinder sector. 
   The solution according to the invention makes it possible to record the papillary ridge pattern of a hand by means of a fixed, ergonomic cylindrical support surface which enables a complete optoelectronic image recording by placing the print surfaces of a hand once upon the cylindrical support surface which has an illumination beam path and an imaging beam path that are sealed off from environmental influences. The recording surface, which has a slight loss of resolution only in one dimension when rectifying the image recording, can unwind in a plane immediately without image transformation and accordingly provides a direct access from the optoelectronically acquired curved image to the digital planar papillary ridge pattern. 
   Further, by applying the principle of FTIR which was previously limited to plane recording surfaces or entailed serious disadvantages, there are hardly any problems with hand perspiration or contrast. Further, the known problems caused by rolling the hand as was conventional heretofore are prevented by the synchronized scanning in the interior of the optical arrangement below the stationary hand. 
   The invention will be described more fully in the following with reference to embodiment examples. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
     In the drawings: 
       FIG. 1  is a schematic view of a base body for frustrated total internal reflection with a cylindrical support surface with conical recesses concentric to the axis of the cylindrical support surface of the base body; 
       FIG. 2  shows a side view of the base body from  FIG. 1  with a cut out cylinder sector for defining a sufficient support surface for the palm of a hand and a central cylindrical recess along the cylinder axis; 
       FIG. 3  shows a schematic view of the arrangement according to the invention with a support body as is indicated in  FIG. 2  but with a cylinder sector shaped as a half-cylinder and with scanning along surface lines of the half-cylinder, the elements of the imaging beam path being rotated around the cylinder axis; 
       FIG. 4  shows an embodiment form of the invention using a scanning body (according to  FIG. 2 ) and a plane mirror for folding the readout beam path into a tube along the cylinder axis and optical wedges (prisms) for complete correction of the perspective error; 
       FIG. 5  shows a construction of the invention with a support body according to  FIG. 3  using a mirror prism and a transmission prism for complete correction of the perspective imaging error; 
       FIG. 6  shows a modified embodiment form according to  FIG. 5  with a high-refraction index prism in total reflection and an optical wedge for correcting the perspective imaging error; 
       FIG. 7  shows an embodiment form of the invention according to  FIG. 3  with a curved mirror for folding the readout beam path and partial correction of the perspective imaging error; 
       FIG. 8  shows a modified embodiment form according to  FIG. 4 , but with only partial correction of the perspective error by means of a cylinder sector which serves as support body and which has an adapted, flatter angle of inclination of the conical recess for the exit of the imaging beam path; 
       FIG. 9  shows a side view of  FIGS. 4 ,  6 ,  7  or  8  with a cylinder sector (e.g., a quarter-cylinder) as scanning body, with calibrating devices and heating elements; and 
       FIG. 10  shows a side view corresponding to  FIGS. 3 and 5  with a support body in the shape of a half-cylinder which is shortened by the radius of the cylindrical recess, with calibrating devices and heating elements and with a schematic depiction of a specific technique for supporting the hand. 
   

   DESCRIPTION OF THE PREFERRED EMBODIMENTS 
   As regards its basic construction, the invention contains, as the core of the optoelectronic recording device, a specially constructed optically transparent support body as is shown in  FIG. 1  for recording large-area prints of skin parts of the fingers  21  or of the entire hand  2  (only in  FIG. 2 ). This cylindrical support body  1  is made of optical material (glass or plastic) in which at least a portion of the outer surface area  11  is provided as a support surface  12  for the hand  2  in such a way that the concave palm of the hand snugly contacts the outer surface  11  of the scanning body  1 . 
   Conical recesses  16  are arranged coaxial to the cylinder axis  15  in the two end faces  13  of the body  1  for coupling in the illumination beam path  3  on the one hand and for coupling out the imaging beam path  4  on the other hand so that the frustrated (because of the hand placed thereon) total reflection (FTIR) of a strip  41  (see  FIG. 9  or  FIG. 10 ) along a lateral line of the outer surface  11  can be recorded. 
   As is shown in  FIG. 2  in a side view of  FIG. 1 , another cylindrical recess  17  is preferably provided at the body  1  concentrically around the cylinder axis  15  in order to guide an imaging beam path  4  (shown only in  FIGS. 4 to 8 ) that is folded by reflecting elements to an image sensor unit  5  (shown only in  FIG. 3 ). Therefore, in order to realize a compact constructional form of the arrangement, as is shown in  FIGS. 4 to 8 , the folded recording beam path  4  and/or illumination beam path  3  can be rotated in a simple manner around the cylinder axis  15  in order to scan different strips  41  of the support surface  12  (as a portion of the outer surface  11 ) successively in progression in circular direction with any density and deliver a series of linear pixel rows from the image sensor unit  5 . A tube  42  (see  FIGS. 4 to 9 ) can be inserted in the additional recess  17  for oriented fastening and joint rotation of all optical components of the imaging beam path  4  around the cylinder axis  15 . 
   Since not more than the outer surface  11  of a half-cylinder  19 , or even less (see  FIG. 2 ,  9  or  10 ), is needed as a recording surface  12  for the entire palm of a hand  2 , the support body  1  is advantageously constructed only as a cylinder sector  18 . The cylinder sector  18  is produced by cutting a solid cylinder along its longitudinal axis, e.g., into halves, thirds or fourths, and so on. According to the axial sectional view in  FIG. 3 , the resulting cylinder section  18  appears as a prism with a cut off tip. 
   Accordingly, in  FIG. 3  (and all of the other subsequent figures) the light input and image readout are carried out in the same way as in a prism, but separately, substantially only in one dimension for every axial plane of the cylinder sector  18  because the entrance surface and exit surface, as outer surfaces of the conical recesses  16 , are conical. 
   The cylinder sector  18  is held in a device housing (not shown) in a stationary manner and the holders seal the outer surface  11  of the cylinder sector  18  relative to the interior space (below and to the side of the support surface  12 ) so as to be tight against dust and sprayed water. 
   On the one hand, for light input, a light source  31  for generating an intensive background illumination on the inner surface  11  of the cylinder sector  18  and, on the other hand, a linearly extending image sensor  51  of an image sensor unit  5  are arranged at the conical recesses  16  of the cylinder sector  18  parallel to the cone surface lines of the conical recesses  16 , which cone surface lines are visible in the axial section shown in the drawing. This light source  31  and linearly extending image sensor  51  make it possible to scan a strip  41  of the support surface  12  (portion of the outer surface  11  that is freely accessible for placement of the hand) within one and the same axial section of the cylinder sector  18  and are moved circularly in succession around the cylinder axis  15  in order to obtain an image of the skin parts of the hand  2  resting on the support surface  12 , which image is assembled from the individual strip scans. 
   The imaging beam path  4  of the strip  41  extending parallel to a surface line of the cylinder sector  18  to the linearly extending image sensor  51  contains at least one imaging optics arrangement  43  and, due to the fact that the image is considerably distorted optically, at least one optically correcting element (in this case, the prism  44 ) for at least partial optical rectification of the image. In the present example according to  FIG. 3 , there is a further (partial) correction of distortion by means of an inclined position of the image sensor  51  relative to the optical axis of the imaging optics  43  making use of the Scheimpflug condition. 
   The entire imaging beam path  4  is coupled to a rotatable tube  42  whose axis of rotation corresponds to the elongated cylinder axis  15  and which—as is shown in FIG.  3 —rotatably holds all of the components of the imaging beam path  4  for optical transmission of the image of the strip  41  from the support surface  12  to the image sensor unit  5  and receives them such that they are fixed relative to one another. The tube  42  is supported so as to be rotatable around the cylinder axis  15  and is moved in a defined manner by steps around the cylinder axis  15  by means of a stepper motor  6  at least in the angular area of the cylinder sector  18 . This movement may be a swiveling movement between two end points or a revolving rotational movement with intermittent scanning and/or illumination outside the cylinder sector  18 . 
   The background brightness that is conventional with frustrated total reflection is supplied by the light source  31  at a flat incident angle. The background illumination is reflected by the surface  11  of the cylinder sector  17  (that is, the support surface  12  for the hand  12 ) and recorded by the imaging beam path  4  in a line-shaped manner as a strip  41  insofar as no papillary ridges of the palm of the hand interfere with total reflection. The total reflection is partially frustrated by the papillary ridges of the skin so that no light from the light source  31  is imaged by the imaging beam path  4  on the image sensor  51  from these locations. 
   In this example, the light source  31  is suitably adapted to the shape of the conical recess  16  introduced in the first front side  12  and is oriented parallel to its surface lines. 
   When the illumination beam path  3  contains only a linear light source  33  (which is entirely sufficient because the imaging is only carried out strip by strip), this light source  33  would likewise have to communicate with the tube  42  so as to be rotatable around the cylinder axis  15  as is shown, e.g., in  FIG. 4 . When using a linear light source, directed illumination can also be advantageously used for more intensive illumination of the imaged strip  41 . 
   When a hand  2  or a finger  21  rests on the support surface  12 , the image of the strip  41  is imaged with frustrated total reflection by imaging optics  43  in the interior of the tube  42  on an image sensor  51 . The stepper motor  6  moves the tube  42  and all of the elements fastened thereto, such as imaging optics  43 , prism  44  and image sensor  51 , synchronously in small angular steps to discrete positions. The image of the newly adjusted strip  41  is recorded in the stationary position of the tube  42  and is subsequently read out from the image sensor  51 . During the readout, the stepper motor  6  moves the tube  42  into the next scanning position. The position of the scanned strip  41  in the object field, i.e., along the (inner) cylindrical surface  11  of the cylinder sector  18 , is moved laterally (circularly) by the positioning device. The step size is selected in such a way that the desired resolution (e.g., 1000 ppi) is achieved on the support surface  12 . 
   The size of the support surface  12  to be scanned for a hand  2  is given as height times width by 203.2 mm×139.7 mm (8″×5.5″). The width accordingly defines the length of the strip  41  to be scanned optically along the surface line  11  of the cylinder sector  18  and the height gives the scanning path of successive scans of strips  41  orthogonal to the direction of the surface lines of the cylinder surface  11 . Depending on the radius of the cylinder sector  18 , this gives the maximum angle around which the tube  42  must rotate in order to completely scan the prescribed “height” of the support surface  12 . Therefore, at 1000 ppi, images with a size of 5500 pixels (width) times 8000 pixels (height) are supplied by the scanner. With a radius of 200 mm, very good results are obtained because the palm of the hand can then rest snugly against the cylindrical outer surface  11  of the support body  1 . With smaller radii, the palm of the hand rests more snugly but there is increased deformation of skin parts. 
   In order not to make excessive demands on the imaging optics  43 , methods are employed to correct the geometric distortions (particularly the non-uniform imaging scale in the transverse direction of the hand  2 ) and the unevenness of illumination (intensity) and sensitivity distribution of the image sensor  51 . To this end, an image sensor  51  is used which has substantially more than the required 5500 pixels, e.g., 8000 pixels (e.g., Eastman Kodak Corp., USA), in direction of the imaged strip  41 . The correction can then be carried out in a real-time logic circuit which is arranged directly downstream of the image sensor  51  and an added analog-to-digital converter, and the prescribed row lengths of 5500 pixels are generated from the pixel data stream of 8000 pixel row lengths. 
   Operation is carried out in the rotating direction of the imaging beam path  4  without correction of geometric errors. The stepper motor  6  is selected in such a way that its positioning steps can be adjusted sufficiently closely and exactly (reproducibly). The perspective imaging error of the imaging beam path  4  causes an imaging of the image sensor  51  by means of the imaging optics  43  in the support surface  12  (that is, in the outer surface  11  of the cylinder sector  18 ) with broader pixels on the side facing the illumination beam path and narrower pixels on the opposite side. Therefore, the MTF in the support surface  12  depends on the location along the surface lines of the cylinder sector  18 . This dependency can be ignored when the MTF reaches the required minimum value even in the worst case, that is, on the side of the illumination beam path  3 . These minimum values of the MTF are set forth, for example, in the image quality standards of large police organizations (e.g., the FBI in the USA, the NPA in Japan) and must be achieved in a verifiable manner by the device within the framework of device certification. 
   When a line sensor  52  is used as an image sensor unit  5 —as is shown in FIG.  4 —and is operated, e.g., at 30 MHz, a complete scan over the entire scanning surface  12  requires a period of 2.8 s (not including idle time). The time for the scanning of a strip  41  is about 0.5 ms. 
   With such short scan times for a strip  41 , the sensitivity of the line sensor  52  is very low compared with surface sensors (such as are used with flat scanners). This should be counteracted by means of an intensive linear (line-shaped) light source  33 . High-intensity LEDs or laser diodes whose light is collimated in the row direction in addition can be used for this purpose. 
   For users who place particular importance upon a uniform MTF in the entire object field, the perspective distortion of the imaging on the line sensor  51  can also be completely corrected by optical means. 
     FIG. 4  shows an arrangement which is suitably expanded for this purpose and which has a folded imaging beam path  4  with correction elements. A quarter-circle cylinder sector  18  is used as an optical support body  1 . The cylinder sector  18  is shown in the drawing plane as an axial section in which the linear image scanning is carried out. 
   In this example, the illumination beam path  3  has a linear light source  33  with a diffuser  32  which is placed in front of it and which is fixedly connected to the tube  42  and is therefore moved synchronously with the components of the imaging beam path  4  so that a narrow area of the outer surface  11  (the strip  41  to be imaged) is irradiated intensively through the illumination-side conical recess  16  always so as to revolve stepwise with the imaging. LED array arrangements or linearly expanded laser diodes can be used as linear light sources  33 . 
   The imaging beam path  4  is represented by the optical axis  49  (of the imaging optics  43 ) and by the marginal rays A 1  and A 2  of the imaged strip  41  of the hand  2 , where A 1  lies on the side of the illumination beam path  3  and A 2  lies on the opposite side. Geometric rectification seems advisable in view of the perspective distortion caused by the large angle of the total reflection. This geometric rectification can be carried out completely in the imaging beam path  4  by means of a first prism  44  and a second prism  45 . When the correction of distortion is not carried out completely optically, subsequent electronic correction can also be carried out (e.g., provided in embodiment variants according to  FIGS. 7 and 8 ). 
   In this case, the tube  42 , as the support member for the rotation of the illumination beam path  3  and the imaging beam path  4 , is arranged below the entire support body  1  so as to be rotatable concentric to the outer surface  11  in another recess  17  of the cylinder sector  18 , which recess  17  provides a free space for the tube  42  cylindrically around the cylinder axis  15 . 
   The strip-by-strip imaging of the supported hand  2  undergoes a partial correction of the perspective distortion by the first prism  44  before the imaging beam path  4  is folded into the tube  42  by a plane reflecting surface  46  and the second prism  45  takes over the rectification of the image which takes place completely optically in this case. The second prism  45  provides at the same time for the orientation of the imaging beam path  4  to the imaging optics  43  whose optical axis  49  lies parallel to the axis of symmetry of the tube  42  and to the cylinder axis  15  and which images the linear strip  41  on the line sensor  52 . Since the imaging is carried out on a line sensor  52 , the two prisms  44  and  45  can be constructed so as to be very narrow. This minimizes the dimensions, which is also advantageous with respect to the requirements for the rotary drive (stepper motor  6 ). 
   When fingers  21  or the entire hand  2  are resting on the support surface  12 , the total reflection—equivalent to the full-surface imaging with a planar supporting prism—is frustrated along the currently scanned surface line of the cylindrical outer surface  11  and the light-dark pattern is acquired in one dimension by the line sensor  52 . Since the two prisms  44  and  45  are fixedly connected to the tube  42 , they rotate synchronous with the line sensor  52  and objective  43  around the cylinder axis  15  so that images of strips  41  adjoining one another as tightly as desired can be recorded from the entire support surface  12  along the outer surface  11  of the cylinder sector  17  successively in time by means of step-by-step rotation of the tube  42 . 
   An alternative solution is also made possible by the arrangement in  FIG. 4 , wherein the prism  44  is arranged in a stationary manner as a circle segment with a radial thickness increase directly downstream of the conical recess  15  and does not move along with the tube  42 . Optically, this alternate variant with stationary prism  44  results in a completely geometrically corrected image exactly the same as the prism  44  (shown in  FIG. 4 ) that is rotated along by the tube  42 . 
     FIG. 5  shows a cylindrical body  1  in the form of a half-cylinder  19 . In this example, a linear light source  33  is again used. This linear light source  33  is fixedly connected to the tube  42  and is accordingly moved synchronously together with the components of the imaging beam path  4 . 
   In the imaging beam path  4 , the first prism  44  is provided directly with a reflecting surface  46  on its back. This reflecting surface  46  is preferably damped. The prism  44  accordingly serves for beam deflection and as a correction element. All the rest of the elements and functions are the same as described in  FIG. 4 . 
   The construction according to  FIG. 6  again starts with a cylinder sector  18 , for example, a quarter-cylinder with conical recesses  16  and a cylindrical recess  17 . In this variant of the invention, a totally reflecting prism  47  is made from a high-refractive index material and can carry out a (partial) rectification of the image as well as folding the imaging beam path  4 . 
   In contrast to  FIG. 5 , no separate reflective coating  46  is needed in  FIG. 6  because the high-refractive index optical material (e.g., heavy flint glass, where n=1.8) enables total reflection at the back surface of the prism  44 . Since the folding of the imaging beam path  4  is carried out at a substantially flatter angle in this case, the tube  42  is designed with a larger diameter and has an eccentrically arranged axis of rotation along the cylinder axis  15 . As in the previous examples, the stepper motor  6  carries out the rotating movement of the imaging beam path  4  (including the line sensor  52 ), in this case together with the linear light source  33 , around the cylinder axis  15 . 
   The construction of the arrangement in  FIG. 7  differs from the previous arrangements above all in that there is no complete rectification of the image within the optical beam path  4 . In this example, the tube  42  is again rotatable concentric to the cylinder axis  15  and has, in addition to the line sensor  52  and imaging optics  43 , only a curved mirror  48  for folding the beam path  4  and for partial correction of the distortion of the image. The rest of the rectification of the image can be carried out electronically in a simple manner. 
   Further, in contrast to  FIGS. 4 to 6 , the illumination beam path  3  has a plane projector  34  which, although it contains a diffuser  32 , intensively irradiates the entire area of the illumination-side conical recess  16  in a stationary manner. 
     FIG. 8  shows another variant of the invention in which the image distortion is only partially optically corrected in the imaging beam path  4 . In this case, the partial correction is achieved in that the angle φ of the conical recess  16  at the readout side of the support body  1  relative to the outer surface  11  is selected so as to be appreciably larger than the corresponding angle γ at the side of the illumination beam path  3  so that the occurring path length differences and the resulting perspective distortion—depending upon the refractive index of the glass that is used—are partially compensated. Optically, the change in the angle φ of the conical recess  14  means a first prism  44  which is added directly to the support body  1  (although its effect is diminished) and whose deficient correction cannot be sufficiently compensated by the second prism  45 . Therefore, a complete correction cannot be achieved. For this purpose it would be necessary to use additional optical elements such as additional prisms or a curved mirror  48  (as in  FIG. 7 ) instead of the plane reflecting surface  46 . The rest of the rectification of the image can then also be carried out electronically in a simple manner as was already mentioned above. 
   In order to assist in the correct placement of the hand on the support surface  12 , a special operating mode can be provided for all of the variants of the invention described above in which the tube  42  makes larger angular steps (for example, eight times larger than in a “normal” scan) and, further, eight pixels in the longitudinal dimension of the image sensor  51  are combined to form a pixel signal. The resulting image is accordingly eight times smaller in both dimensions: (W)×(H)=687×1000 pixels, that is, comprises only 1/64 of the amount of data. This reduced image can be read out eight times faster and is accordingly available after only 0.35 s. In a repeating scan operation in which the stepper motor  6  permanently rotates the tube  42  back and forth similar to the movement of a windshield wiper, about three images of this type with reduced resolution can be recorded per second. Therefore, by immediately displaying these images on a connected image screen (not shown), the user has a kind of quasi-live image for monitoring the correct complete placement of the palm of a human hand  2  on the support surface  12 . 
     FIGS. 9 and 10  show further embodiments in a side view and cross section, respectively, of arrangements described above which make the application of the invention reproducible and more reliable. 
   First, the cylindrical optical support body  1  is brought into contact at its “longitudinal sectional surfaces” (when a cylinder section  18  is generated from a solid cylinder) with heating elements  7  and is accordingly heated in a deliberate manner. The heat from the heating elements  7  propagates in the optical support body and after a certain heating period leads to the uniform heating of the outer surface  11 . This serves to prevent condensation in cold environments and, by softening hard skin and stimulating a spontaneous excretion of perspiration by the supported hand  2 , supports high-contrast image recording. The heating elements  7  which can preferably be adjustable electric heating elements (resistors, transistors, or the like) are shown schematically in  FIG. 9  as area heaters which are arranged over the full surface of the radially oriented surfaces of the support body  1  which is a quarter-circle cylinder sector  18  in this example. 
     FIG. 9  further shows calibrating units  8  by means of which the image quality parameters can be tested and monitored by arranging calibrating marks  81  and  82  on both sides outside the support surface  12  at different locations on the outer surface  11  of the cylinder sector  18 . These calibrating marks  81  and  82  can contain MTF test structures and geometry test fields. To protect against environmental influences, each of these areas is covered by a hood  83  and possibly also by the device housing (not designated by a reference number). The hood  83  can be very flat and only ensures that the test structures cannot be touched and can be imaged accurately on the linearly extending image sensor  51  by the imaging beam path  4 . 
     FIG. 9  further shows an advantageous variant of the arrangement according to one of the preceding  FIGS. 4 ,  6 ,  7  or  8  in cross section, The optical support body  1  is constructed as a quarter-circle cylinder sector  18 . At a predetermined length of 203.2 mm (8″) for the support surface  12  of the hand  2 , the outer surface  11  extends around the cylinder axis  15  in corresponding manner. This dimension of the support surface  12  is scanned in the area delimited by dashes by a back-and-forth rotation of the image sensor  51  (and of the imaging beam path  4  which is visible here only as a tube  42 ). 
   The calibrating marks  81  and  82  are arranged on the outer surface  11  immediately outside of this portion of the cylinder sector  18  and are covered by the hood  83  for protection. In addition, there are calibrating marks  85  under additional hoods  84  which differ from calibrating marks  81  and  82  in that there are no calibration patterns under the hoods  84  but rather only an empty partial surface of the outer surface  11 . These hoods  84  protect the calibrating surfaces  85  from touching, soiling and external light. 
   The empty calibrating surfaces  85  under the hoods  84  are used to determine the intensity distribution of the line-shaped background illumination. For this purpose, when the tube  42  is rotated in such a way that the image sensor  51  “sees” exactly this area the calibrating data are read out and stored in order to be used for determining correction values. An existing non-uniformity of the light source  31 , or one occurring in the course of operation, shading of the imaging optics  43  by edges or a non-uniform pixel sensitivity of the image sensor  51  can be corrected with the correction values. 
   In order to detect the calibrating marks  81  and  82 , the tube  42  is moved by means of the stepper motor  6  (not visible in  FIG. 9 ) in such a way that not only the portion located below the hoods  83  and  84  is recorded, but a scan is carried out from the covered areas of the hoods  83  and  84  on one side over the support surface  12  to the covered areas of the hoods  83  and  84  on the other side. This separate calibrating scan results in a two-dimensional image of the calibrating marks  81  and  82 . With correspondingly formed marks  81  and  82  at other locations along the outer surface  11  (extending orthogonal to the drawing plane) a number of important parameters for the image quality can then be calculated automatically from the calibrating image data. Similar advantageous solutions are described in EP 11 01 187 and are incorporated herein by reference. 
   The construction according to  FIG. 10  can be interpreted as a side view of  FIG. 3  and  FIG. 5  in that a half-cylinder  19  is used as a support body  1  in this embodiment example. The available “height” of the support surface  12  is accordingly enlarged or this same surface area, e.g., H×W=203.2 mm×139.67 mm (8″×5.5″), can be produced with a smaller radius of the half-cylinder  19  and accordingly with a greater curvature of the support surface  12 . In the latter case, there is the added possibility of improved acquisition of the thumbprint of a hand  2  in the gripping position. A corresponding attitude of the hand is shown schematically in  FIG. 10 . 
   But a special feature in this example consists in that the cylinder sector  18  (in this case a half-cylinder  19 ) was shortened to economize on the cylindrical recess  17 . This possibility is also offered for all of the preceding examples (also in the smaller cylinder sectors) in that, instead of the cylindrical recess  17 , it is possible simply to provide a straight section S (parallel to the two straight edges of the outer surface  11 ) to create the required space for the tube  42  (or differently shaped holders) for the imaging beam path  4  which is rotatable around the cylinder axis  15 . However, the straight section S may only shorten the height of the half-cylinder  19  (or of the cylinder sector  18 ) to the extent that the imaging beam path  4  can still always exit from the conical recess  16  during its rotating scanning movement. In particular, this condition must also be met outside the support surface  12  for the scan of the calibrating units  8 ; however, these calibrating units  8  can be made accessible to complete imaging in a simple manner by means of suitable spatial arrangement along the cylinder length. 
   All of the rest of the details in  FIG. 10  such as the heating elements  7  and calibrating units  8  are provided in the same way as was described with reference to  FIG. 9 , the only difference being the enlarged scan angle between the two dashed lines which delimit the freely accessible support surface  12  and therefore create an elongated support surface  12  which is particularly suited to the special manner of supporting the hand  2 . 
   The optical body  1  (cylinder sector  18  and half-cylinder  19 ) can be made of glass or optical plastic. In order to protect against scratching—particularly on plastic material—a coating is applied or the support surface, when not in use, can be completely protected by a correspondingly curved cover. 
   While the foregoing description and drawings represent the present invention, it will be obvious to those skilled in the art that various changes may be made therein without departing from the true spirit and scope of the present invention. 
   Reference Numbers 
   
       
         1  support body 
         11  surface 
         12  support surface 
         13  first end face 
         14  second end face 
         15  cylinder axis 
         16  conical recesses 
         17  additional (cylindrical) recess 
         18  cylinder sector 
         19  half-cylinder 
         2  hand 
         21  finger 
         3  illumination beam path 
         31  light source 
         32  diffuser 
         33  linear light source 
         34  plane projector 
         4  imaging beam path 
         41  strip 
         42  tube 
         43  imaging optics 
         44  first prism 
         45  second prism 
         46  reflecting surface 
         47  prism (of high-refractive index glass) 
         48  curved mirror 
         49  optical axis 
         5  image sensor unit 
         51  (linearly extending) image sensor 
         52  line sensor 
         6  stepper motor 
         7  heating element 
         8  calibrating devices 
         81 ,  82  calibrating marks 
         83 ,  84  hood 
         85  calibrating surface 
       A 1 , A 2  marginal ray 
       S section plane