Abstract:
The liquid coating method includes the step of ejecting droplets from nozzles of a recording head onto an imaging region of a surface of a substrate placed on a support plate, wherein a dot pitch φ that is an interval between landing positions of the droplets on the surface of the substrate satisfies a following condition: 
             ϕ   ≤     2   ⁢         3   ⁢     V   ⁡     (     1   +     cos   ⁢           ⁢     θ   a         )       ⁢   sin   ⁢           ⁢     θ   a           π   ⁡     (     1   -     cos   ⁢           ⁢     θ   a         )       ⁢     (     2   +     cos   ⁢           ⁢     θ   a         )         3             
where V stands for a volume of a droplet ejected from each of the nozzles and θ a  stands for an advancing contact angle of the droplet against the substrate.

Description:
CROSS-REFERENCE TO RELATED APPLICATION 
     This application claims priority under 35 USC 119 from Japanese Patent Application No. 2008-087673, filed Mar. 28, 2008, the disclosure of which is incorporated herein by reference. 
     BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The present invention relates to a liquid coating method, a liquid coating device, and a method of manufacturing a radiation detector, and more particularly to a liquid coating method and a liquid coating device in which a liquid is applied on a surface of a substrate by using an ink jet head. 
     2. Description of the Related Art 
     Japanese Patent Application Publication No. 2006-130436 discloses a liquid ejection device comprising an ejection head in which a plurality of nozzles are arranged in rows, wherein the ejection head and a substrate are arranged to form a predetermined angle within a plane substantially perpendicular to the direction in which the ejection head and the substrate are scanned (moved) relative to each other. 
     When liquid droplets are applied on the entire surface of an imaging region on a substrate serving as a medium by using an ink jet, all the droplets that have landed on the substrate have to be united so that no gap occurs therebetween. The distance (dot pitch) between the droplets landing on the imaging surface has to be optimized in order to unite the droplets so that no gap occurs in the imaging region and to prevent the liquid from protruding from the imaging region. 
     Japanese Patent Application Publication No. 2006-130436 describes optimizing the relationship between a nozzle pitch and a landing distance (dot pitch) of droplets by arranging the ejection head and substrate at a predetermined angle. However, Japanese Patent Application Publication No. 2006-130436 has absolutely no description relating to a method of determining a dot pitch necessary to unite all the droplets. 
     SUMMARY OF THE INVENTION 
     The present invention has been contrived to resolve this problem and it is an object of the present invention to provide a liquid coating method, a liquid coating device, and a method of manufacturing a radiation detector that make it possible to unite droplets within a predetermined imaging region on a substrate so that no gap occurs therebetween and prevent the liquid from protruding from the imaging region. 
     In order to attain an object described above, one aspect of the present invention is directed to a liquid coating method comprising the step of ejecting droplets from nozzles of a recording head onto an imaging region of a surface of a substrate placed on a support plate, wherein a dot pitch φ that is an interval between landing positions of the droplets on the surface of the substrate satisfies a following condition: 
             ϕ   ≤     2   ⁢         3   ⁢     V   ⁡     (     1   +     cos   ⁢           ⁢     θ   a         )       ⁢   sin   ⁢           ⁢     θ   a           π   ⁡     (     1   -     cos   ⁢           ⁢     θ   a         )       ⁢     (     2   +     cos   ⁢           ⁢     θ   a         )         3             
where V stands for a volume of a droplet ejected from each of the nozzles and θ a  stands for an advancing contact angle of the droplet against the substrate.
 
     Desirably, the advancing contact angle θ a  and a receding contact angle θ r  standing for a receding contact angle of the droplet ejected from each of the nozzles against the substrate satisfy a following condition: 
               θ   r     ≤     2   ⁢           ⁢   arc   ⁢           ⁢   tan   ⁢     {       π   3     ⁢         (     1   -     cos   ⁢           ⁢     θ   a         )     ⁢     (     2   +     cos   ⁢           ⁢     θ   a         )           (     1   +     cos   ⁢           ⁢     θ   a         )     ⁢   sin   ⁢           ⁢     θ   a         ⁢       r   2       ϕ   2         }       ≤     θ   a           
where r stands for a radius of one droplet with the volume V on the surface of the substrate when the one droplet has wetly spread under condition of the advancing contact angle θ a .
 
     Desirably, the advancing contact angle θ a  and the receding contact angle θ r  satisfy a following condition: 
     
       
         
           
             
               θ 
               r 
             
             ≤ 
             
               2 
               ⁢ 
               
                   
               
               ⁢ 
               arc 
               ⁢ 
               
                   
               
               ⁢ 
               tan 
               ⁢ 
               
                 { 
                 
                   
                     π 
                     12 
                   
                   ⁢ 
                   
                     
                       
                         ( 
                         
                           1 
                           - 
                           
                             cos 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               θ 
                               a 
                             
                           
                         
                         ) 
                       
                       ⁢ 
                       
                         ( 
                         
                           2 
                           + 
                           
                             cos 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               θ 
                               a 
                             
                           
                         
                         ) 
                       
                     
                     
                       
                         ( 
                         
                           1 
                           + 
                           
                             cos 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               θ 
                               a 
                             
                           
                         
                         ) 
                       
                       ⁢ 
                       sin 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       
                         θ 
                         a 
                       
                     
                   
                 
                 } 
               
             
             ≤ 
             
               
                 θ 
                 a 
               
               . 
             
           
         
       
     
     Desirably, the imaging region is a rectangular region having a size L a  in a first direction and a size L b  in a second direction perpendicular to the first direction, and the droplets are caused to land substantially equidistantly with an interval equal to or larger than L a /(2r) in the first direction and an interval equal to or larger than L b /(2r) in the second direction. 
     Desirably, wherein when the droplets are ejected onto the imaging region, only one scanning is performed over the imaging region. 
     In order to attain an object described above, another aspect of the present invention is directed to a liquid coating device comprising: a support plate onto which a substrate is placed; a recording head having a plurality of nozzles that eject droplets on an imaging region of a surface of the substrate placed on the support plate; and a control device controlling ejection from the recording head in such a manner that a volume V of a droplet ejected from each of the plurality of nozzles of the recording head onto the substrate satisfies the following condition: 
             V   ≥       π   24     ⁢         (     1   -     cos   ⁢           ⁢     θ   a         )     ⁢     (     2   +     cos   ⁢           ⁢     θ   a         )           (     1   +     cos   ⁢           ⁢     θ   a         )     ⁢   sin   ⁢           ⁢     θ   a         ⁢     ϕ   3             
where θ a  stands for an advancing contact angle of the droplet against the substrate and φ stands for a dot pitch that is an interval between landing positions of the droplets on the surface of the substrate.
 
     Desirably, the control device controls the ejection from the recording head in such a manner that a receding contact angle θ r  of a droplet ejected from each of the plurality of nozzles against the substrate satisfies a following condition: 
     
       
         
           
             
               θ 
               r 
             
             ≤ 
             
               2 
               ⁢ 
               
                   
               
               ⁢ 
               arc 
               ⁢ 
               
                   
               
               ⁢ 
               tan 
               ⁢ 
               
                 { 
                 
                   
                     
                       
                         π 
                         3 
                       
                       ⁢ 
                       
                         
                           
                             ( 
                             
                               1 
                               - 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                           ⁢ 
                           
                             ( 
                             
                               2 
                               + 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                         
                         
                           
                             ( 
                             
                               1 
                               + 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                           ⁢ 
                           sin 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           
                             θ 
                             a 
                           
                         
                       
                       ⁢ 
                       
                         V 
                         2 
                       
                     
                     3 
                   
                   ⁢ 
                   
                     1 
                     
                       ϕ 
                       2 
                     
                   
                 
                 } 
               
             
             ≤ 
             
               
                 θ 
                 a 
               
               . 
             
           
         
       
     
     Desirably, the control device controls the ejection from the recording head in such a manner that the advancing contact angle θ a  and the receding contact angle θ r  satisfy a following condition: 
               θ   r     ≤     2   ⁢           ⁢   arc   ⁢           ⁢   tan   ⁢     {           π   3     ⁢         (     1   -     cos   ⁢           ⁢     θ   a         )     ⁢     (     2   +     cos   ⁢           ⁢     θ   a         )           (     1   +     cos   ⁢           ⁢     θ   a         )     ⁢   sin   ⁢           ⁢     θ   a         ⁢     V   2       3     ⁢     1     4   ⁢           ⁢     r   2           }       ≤     θ   a           
where r stands for a radius of one droplet with the volume V on the surface of the substrate when the one droplet has wetly spread under condition of the advancing contact angle θ a .
 
     Desirably, when the imaging region is a rectangular region having a size L a  in a first direction and a size L b  in a second direction perpendicular to the first direction, the control device controls the ejection from the recording head in such a manner that the droplets are caused to land substantially equidistantly with an interval equal to or larger than L a /(2r) in the first direction and an interval equal to or larger than L b /(2r) in the second direction. 
     Desirably, the liquid coating device further comprises a scanning device which performs relative scanning of the recording head and the substrate relative, wherein when the droplets are ejected onto the imaging region, the scanning device performs the relative scanning in such a manner that only one scanning is performed over the imaging region. 
     Desirably, a nozzle pitch of the recording head corresponds to the dot pitch. 
     Desirably, a nozzle pitch of the recording head is integral multiple of the dot pitch. 
     In order to attain an object described above, one aspect of the present invention is directed to a method of manufacturing a radiation detector which has: a first electrode that transmits a radiation that carries image information; a photoconductive layer that generates an electric charge when irradiated with the radiation transmitted through the first electrode; a second electrode that is provided on a side opposite to a side where the first electrode is provided with respect to the photoconductive layer and that collects the electric charge generated by the photoconductive layer; and an organic polymer layer provided between the photoconductive layer and the first electrode, the method comprising the step of forming the organic polymer layer using one of the above-described liquid coating methods. 
     In accordance with the present invention, time required for applying the liquid can be shortened and the amount of liquid consumed when the liquid is applied on the entire surface of the imaging region on the surface of the substrate can be reduced. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       The nature of this invention, as well as other objects and benefits thereof, will be explained in the following with reference to the accompanying drawings, in which like reference characters designate the same or similar parts throughout the figures and wherein: 
         FIG. 1  is a perspective view illustrating a liquid coating device of a first embodiment of the present invention; 
         FIG. 2  is a plan view illustrating a plane formed by a nozzle of a recording head  12 ; 
         FIG. 3  is a cross-sectional view of an ejection element  20 ; 
         FIG. 4  is a block diagram illustrating a control system of the liquid coating device of the first embodiment of the present invention; 
         FIG. 5  schematically illustrates the variation with time of a droplet that has landed on the surface of a substrate  16 ; 
         FIG. 6  is a cross-sectional view illustrating a droplet that expanded due to wetting; 
         FIG. 7  is a cross-sectional view illustrating a receding contact angle of a droplet; 
         FIG. 8  is a perspective view illustrating a liquid coating device of a second embodiment of the present invention; 
         FIG. 9  is a plan view illustrating a plane formed by nozzles of the recording head  12  of the second embodiment of the present invention; 
         FIG. 10  is a block diagram illustrating a control system of the liquid coating device of the second embodiment of the present invention; 
         FIG. 11  is a perspective view illustrating another embodiment of the liquid coating device; 
         FIG. 12  is a perspective view illustrating another embodiment of the liquid coating device; 
         FIG. 13  is a perspective view illustrating another embodiment of the liquid coating device; 
         FIG. 14  is a perspective view illustrating another embodiment of the liquid coating device; 
         FIG. 15  is a perspective view illustrating another embodiment of the liquid coating device; 
         FIG. 16  is a perspective view illustrating another embodiment of the liquid coating device; 
         FIG. 17  is a perspective view illustrating another embodiment of the liquid coating device; 
         FIG. 18  is a perspective view illustrating another embodiment of the liquid coating device; 
         FIG. 19  is a perspective view illustrating another embodiment of the liquid coating device; 
         FIGS. 20A and 20B  are schematic diagrams illustrating the entire configuration of the radiation detector of a TFT system; 
         FIG. 21  is a schematic structural diagram illustrating main components of the radiation detector of a TFT system; 
         FIG. 22  is a cross-sectional view illustrating a structure of a one-pixel unit of the radiation detector of a TFT system; 
         FIG. 23  is a plan view illustrating a structure of a one-pixel unit of the radiation detector of a TFT system; 
         FIG. 24  is a graph illustrating the relationship between a shear rate and a shear viscosity of an ejection liquid used to form a hole injection blocking layer in the radiation detector of a TFT system; 
         FIGS. 25A and 25B  illustrate a schematic configuration of a radiation detection substrate serving as a radiation detector of an optical reading system; 
         FIGS. 26A and 26B  illustrate a schematic structure of a lower substrate for radiation detection of the radiation detection substrate illustrated in  FIG. 22 ; 
         FIG. 27  is a schematic diagram illustrating the configuration of the radiation detection substrate illustrated in  FIG. 22 ; 
         FIG. 28  illustrates a sealing structure that seals the upper electrode of the radiation detection substrate illustrated in  FIG. 22 ; 
         FIG. 29  is a block diagram illustrating the configuration of a charge take-out amplifier, and a connection mode between this configuration and an image processing device and other devices disposed outside the radiation detection substrate; 
         FIG. 30  is a schematic diagram illustrating a situation when the scanning is performed using line light as read-out light; and 
         FIGS. 31A and 31B  illustrate an example of applying the configuration of the hole injection blocking layer in the radiation detector of a TFT system illustrated in  FIGS. 20A and 20B , to the radiation detection substrate illustrated in  FIGS. 25A and 25B . 
     
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     Configuration of Liquid Coating Device 
       FIG. 1  is a perspective view illustrating a liquid coating device of a first embodiment of the present invention. 
     As illustrated in  FIG. 1 , the liquid coating device (ink jet recording device)  10  of the present embodiment includes an ink jet head (referred to hereinbelow as “recording head”)  12  and a support plate  14 . 
     A substrate  16  that is an object of applying a liquid with the recording head  12  is placed on the support plate  14 . 
     In the recording head  12 , nozzles  22  are arranged side by side over the entire width in the x direction and y direction of an object region (referred to hereinbelow as “imaging region”) of the substrate  16  that is to be coated with the liquid. 
     The recording head  12  is supported so that a constant clearance is maintained between the recording head and the support plate  14 , and the substrate  16  is placed on the support plate  14  so that the recording head  12  and the imaging region overlap. As a result, the liquid can be applied (deposited) on the entire surface of the imaging region of the substrate  16  by ejecting all the droplets at once from the nozzles  22  of the recording head  12 . 
       FIG. 2  is a plan view illustrating a surface where the nozzles of the recording head  12  are formed. 
     As illustrated in  FIG. 2 , the recording head  12  has a structure in which ejection elements  20 , each having a nozzle  20  and a pressure chamber  24 , are arranged substantially equidistantly along the sub-scanning direction (y direction) substantially perpendicular to the main scanning direction (x direction). 
     A nozzle diameter in the recording head  12  is, for example, 35 μm and a nozzle pitch is 254 μm (100 npi). The recording head  12  has a jet-out period of 1 kHz, and droplets can be continuously jetted out at a head scanning rate of 0.1 m/sec. 
     When the recording head  12  has a high-density configuration such that dots formed by the droplets jetted out from the adjacent nozzles overlap, an operation mode is preferred in which thinning control is conducted such that droplets are jetted out simultaneously from every other nozzle, rather than from the adjacent nozzles, and the jetting-out process is divided into two cycles. 
     As illustrated in  FIG. 2 , pressure chambers  24  provided correspondingly to nozzles  22  have a substantially square shape in a plan view thereof. An outflow port leading to the nozzle  20  is provided in one inner corner on a diagonal line of the pressure chamber  24 , and a liquid supply port  26  leading to the pressure chamber  24  is provided in the other corner. In addition to the aforementioned square shape, the pressure chamber  24  can have a polygonal shape such as tetragonal shape (rhomboidal shape, rectangular shape), pentagonal shape, or hexagonal shape, and also round shape or elliptical shape. 
       FIG. 3  is a cross-sectional view of the ejection element  20 . 
     As illustrated in  FIG. 3 , the pressure chamber  24  of the ejection element  20  is linked to a common channel  28  via the supply port  26 . The common channel  28  is linked to a tank (not illustrated in the figure) that serves as a liquid supply source, and the liquid supplied from the tank is distributed and supplied to the pressure chambers  24  via the common channel  28 . 
     A piezoelectric element  34  provided with an individual electrode  32  is bonded to a pressure plate (oscillation plate also serving as a common electrode)  30  constituting part of the surface (top surface in  FIG. 3 ) of the pressure chamber  24 . For example, a piezoelectric material such as lead zirconium titanate (PZT) or barium titanate can be used as a material for the piezoelectric element  34 . 
     Where a drive signal is applied between the individual electrode  32  and the common electrode, the piezoelectric element  34  is deformed and the volume of the pressure chamber  24  changes. As a result, the pressure inside the pressure chamber  24  changes, thereby ejecting a droplet from the nozzle  22 . After the droplet has been ejected, the displacement of the piezoelectric element  34  returns to the original state, and the pressure chamber  24  is refilled with new liquid from the common channel  28  via the supply port  26 . 
     In the present embodiment, a system is employed by which ink is pressurized by the deformation of the piezoelectric element  34 , but actuators of other systems (for example, a thermal system) may be also employed. 
     The liquid coating device  10  has a supply system for supplying liquid to the recording head  12  and a maintenance system for performing maintenance of the recording head  12  (these systems are not illustrated in the figure). 
       FIG. 4  illustrates a block diagram indicating a control system of the liquid coating device. 
     The liquid coating device  10  includes a communications interface  40 , a system controller  42 , a memory  46 , a heater driver  52 , an ejection control unit  56 , a buffer memory and a head driver  60 . 
     The communications interface  40  functions as an interface unit receiving ejection date sent from a host computer  80 . As the communications interface  40 , USB (Universal Serial Bus), IEEE 1394, Ethernet (registered trademark), wireless network, other serial networks, parallel interface such as Centronics may be used. Further, a buffer memory may be mounted on this portion in order to speed up the communications. 
     The system controller  42  includes a CPU (central processing unit) and the peripheral circuits, and functions as a control unit controlling each section of the liquid coating device  10 . This system controller  42  controls the communications with the host computer  80 , controls read-in and writing-in the memory  46 , generates control signals to control the motors of the conveyance drive system and the heater  54 , and performs other control. 
     Control programs of the liquid coating device  10  are stored in a program storage unit  44 . The system controller  42  reads out various sorts of control programs stored in the program storage unit  44  and performs the read-out programs in a proper manner. 
     The memory  46  is a memory device used as a temporary storage area of date and a working area when the system controller  42  carries out various sorts of calculations. As the memory  46 , a memory formed from a semiconductor element, or a magnetic medium such as a hard disk may be used. 
     The heater driver  52  drives the heater  54  in accordance with control signals from the system controller  42 . The heater  54  includes heaters for adjusting temperature provided on parts of the liquid coating device  10 . 
     The ejection date sent from the host computer  80  is sent into the liquid coating device  10  via the communications interface  40 , and is temporarily stored in the memory  46 . 
     The ejection control unit  56  has a signal processing function to carry out various processing and correction to generate signals for controlling the ejection from the ejection data stored in the memory  46  in accordance with the control by the system controller  42 , and supplies the generated print control signals (dot data) to the head driver  60 . Required signal processing is carried out in the ejection control unit  56 , and the ejection amount and the ejection timing of the liquid from the head  12  are controlled via the head driver  60 , on the basis of the ejection data. 
     The head driver  60  drives the piezoelectric elements  34  of the recording head  12  on the basis of the ejection data supplied from the ejection control unit  56 . The head driver  60  may include a feedback control system to maintain uniform drive conditions of the head. 
     The ejection control unit  56  is provided with a buffer memory  58 ; and ejection data, parameters, and other data are temporarily stored in the buffer memory  58  when the ejection data is processed in the ejection control unit  56 . 
     It is possible to use the buffer memory  58  as the memory  46 . It is also possible to integrate the ejection control unit  56  and the system controller  42  in such a manner that both the ejection control unit  56  and the system controller  42  are realized by one processor. 
     Droplet Coating Conditions 
     Conditions under which droplets are united on the surface of the substrate  16  will be explained below. 
       FIG. 5  illustrates schematically how the droplets that have landed on the surface of the substrate  16  change with time. The “a 1 ” part and “b 1 ” part of  FIG. 5  are cross-sectional views, and the “a 2 ” part and “b 2 ” part of  FIG. 5  are plan views. 
     As illustrated in the “a 1 ” part “a 2 ” of  FIG. 5 , each droplet L that has been ejected from the recording head  12  and landed on the surface of the substrate  16  has a substantially round shape at the initial stage of landing and is in contact with the adjacent droplets. Then, as illustrated in the “b 1 ” part and “b 2 ” part of  FIG. 5 , each droplet L spreads due to wetting (wetly spreads) and the entire surface of the rectangular region A 10  is coated with the liquid. 
     Where a radius of the droplet L that has spread on the surface of the substrate  16  due to wetting is denoted by r and an advancing contact angle is denoted by θ a , the volume V of the droplet L can be represented by Formula (1) below. In the explanation below, the substrate  16  is assumed to be from a medium that is impermeable to the droplet L (the droplet does not penetrate into the medium). 
     
       
         
           
             
               
                 
                   V 
                   = 
                   
                     
                       π 
                       3 
                     
                     ⁢ 
                     
                       
                         
                           ( 
                           
                             1 
                             - 
                             
                               cos 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               
                                 θ 
                                 a 
                               
                             
                           
                           ) 
                         
                         ⁢ 
                         
                           ( 
                           
                             2 
                             + 
                             
                               cos 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               
                                 θ 
                                 a 
                               
                             
                           
                           ) 
                         
                       
                       
                         
                           ( 
                           
                             1 
                             + 
                             
                               cos 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               
                                 θ 
                                 a 
                               
                             
                           
                           ) 
                         
                         ⁢ 
                         sin 
                         ⁢ 
                         
                             
                         
                         ⁢ 
                         
                           θ 
                           a 
                         
                       
                     
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     1 
                     ) 
                   
                 
               
             
           
         
       
     
     By modifying Formula (1) above, it is possible to represent the radius r of the droplet L that has spread on the surface of the substrate  16  due to wetting by the following Formula (2). 
     
       
         
           
             
               
                 
                   r 
                   = 
                   
                     
                       
                         3 
                         π 
                       
                       ⁢ 
                       
                         
                           
                             ( 
                             
                               1 
                               + 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                           ⁢ 
                           sin 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           
                             θ 
                             a 
                           
                         
                         
                           
                             ( 
                             
                               1 
                               - 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                           ⁢ 
                           
                             ( 
                             
                               2 
                               + 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                         
                       
                       ⁢ 
                       V 
                     
                     3 
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     2 
                     ) 
                   
                 
               
             
           
         
       
     
     For the adjacent droplets L to abut and be united, the distance (referred to hereinbelow as “dot pitch”) φ between the centers of the adjacent droplets L has to be equal to or less than 2r. Where Formula (2) above is substituted in φ≦2r, the following Formula (3) is obtained. 
     
       
         
           
             
               
                 
                   ϕ 
                   ≤ 
                   
                     2 
                     ⁢ 
                     
                       
                         
                           3 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           
                             V 
                             ⁡ 
                             
                               ( 
                               
                                 1 
                                 + 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                           
                           ⁢ 
                           sin 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           
                             θ 
                             a 
                           
                         
                         
                           
                             
                               π 
                               ⁡ 
                               
                                 ( 
                                 
                                   1 
                                   - 
                                   
                                     cos 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     
                                       θ 
                                       a 
                                     
                                   
                                 
                                 ) 
                               
                             
                             ⁢ 
                             
                               ( 
                               
                                 2 
                                 + 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                           
                           ⁢ 
                           
                               
                           
                         
                       
                       3 
                     
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     3 
                     ) 
                   
                 
               
             
           
         
       
     
     By modifying Formula (3) above, it is possible to obtain Formula (3′) representing a condition relating to an injection volume V of a droplet from each nozzle. 
     
       
         
           
             
               
                 
                   V 
                   ≥ 
                   
                     
                       π 
                       24 
                     
                     ⁢ 
                     
                       
                         
                           ( 
                           
                             1 
                             - 
                             
                               cos 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               
                                 θ 
                                 a 
                               
                             
                           
                           ) 
                         
                         ⁢ 
                         
                           ( 
                           
                             2 
                             + 
                             
                               cos 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               
                                 θ 
                                 a 
                               
                             
                           
                           ) 
                         
                       
                       
                         
                           ( 
                           
                             1 
                             + 
                             
                               cos 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               
                                 θ 
                                 a 
                               
                             
                           
                           ) 
                         
                         ⁢ 
                         sin 
                         ⁢ 
                         
                             
                         
                         ⁢ 
                         
                           θ 
                           a 
                         
                       
                     
                     ⁢ 
                     
                       ϕ 
                       3 
                     
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     
                       3 
                       ′ 
                     
                     ) 
                   
                 
               
             
           
         
       
     
     As illustrated in  FIG. 6 , a thickness h of the droplet L after it has spread due to wetting can be represented by h=V/φ 2  if the droplet L is taken as a rectangular parallelepiped. The following Formula (4) can be obtained by substituting Formula (I) above into h=V/φ 2 . 
     
       
         
           
             
               
                 
                   h 
                   = 
                   
                     
                       V 
                       
                         ϕ 
                         2 
                       
                     
                     = 
                     
                       
                         π 
                         3 
                       
                       ⁢ 
                       
                         
                           
                             ( 
                             
                               1 
                               - 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                           ⁢ 
                           
                             ( 
                             
                               2 
                               + 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                         
                         
                           
                             ( 
                             
                               1 
                               + 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                           ⁢ 
                           sin 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           
                             θ 
                             a 
                           
                         
                       
                       ⁢ 
                       
                         
                           r 
                           3 
                         
                         
                           ϕ 
                           2 
                         
                       
                     
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     4 
                     ) 
                   
                 
               
             
           
         
       
     
     As illustrated in  FIG. 7 , where the receding contact angle of the droplet L is denoted by θ r , a condition of the droplet L not shrinking on the surface of the substrate  16  can be represented by θ r ≦2 arctan(h/r). By substituting Formula (4) above into θ r ≦2 arctan (h/r), the following Formula (5) can be obtained. 
     
       
         
           
             
               
                 
                   
                     
                       θ 
                       r 
                     
                     ≤ 
                     
                       2 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       arctan 
                       ⁢ 
                       
                         h 
                         r 
                       
                     
                   
                   = 
                   
                     2 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     arctan 
                     ⁢ 
                     
                       { 
                       
                         
                           π 
                           3 
                         
                         ⁢ 
                         
                           
                             
                               ( 
                               
                                 1 
                                 - 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                             ⁢ 
                             
                               ( 
                               
                                 2 
                                 + 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                           
                           
                             
                               ( 
                               
                                 1 
                                 + 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                             ⁢ 
                             sin 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               θ 
                               a 
                             
                           
                         
                         ⁢ 
                         
                           
                             r 
                             2 
                           
                           
                             ϕ 
                             2 
                           
                         
                       
                       } 
                     
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     5 
                     ) 
                   
                 
               
             
           
         
       
     
     Where φ=2r (that is, a maximum value of dot pitch φ satisfying the condition (Formula (3)) under which the adjacent droplets L abut) is substituted in Formulas (4) and (5) above, the following Formulas (6) and (7) can be obtained. 
     
       
         
           
             
               
                 
                   h 
                   = 
                   
                     
                       V 
                       
                         4 
                         ⁢ 
                         
                             
                         
                         ⁢ 
                         
                           r 
                           2 
                         
                       
                     
                     = 
                     
                       
                         π 
                         12 
                       
                       ⁢ 
                       
                         
                           
                             ( 
                             
                               1 
                               - 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                           ⁢ 
                           
                             ( 
                             
                               2 
                               + 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                         
                         
                           
                             ( 
                             
                               1 
                               + 
                               
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ) 
                           
                           ⁢ 
                           sin 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           
                             θ 
                             a 
                           
                         
                       
                       ⁢ 
                       r 
                     
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     6 
                     ) 
                   
                 
               
             
             
               
                 
                   
                     
                       θ 
                       r 
                     
                     ≤ 
                     
                       2 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       arctan 
                       ⁢ 
                       
                         h 
                         r 
                       
                     
                   
                   = 
                   
                     2 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     arctan 
                     ⁢ 
                     
                       { 
                       
                         
                           π 
                           12 
                         
                         ⁢ 
                         
                           
                             
                               ( 
                               
                                 1 
                                 - 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                             ⁢ 
                             
                               ( 
                               
                                 2 
                                 + 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                           
                           
                             
                               ( 
                               
                                 1 
                                 + 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                             ⁢ 
                             sin 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               θ 
                               a 
                             
                           
                         
                       
                       } 
                     
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     7 
                     ) 
                   
                 
               
             
           
         
       
     
     The range in which the droplet L spreads due to wetting can be then adequately controlled by making the advancing contact angle θ a  to satisfy the condition represented by the following Formula (8). 
     
       
         
           
             
               
                 
                   
                     θ 
                     r 
                   
                   ≤ 
                   
                     2 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     arctan 
                     ⁢ 
                     
                       { 
                       
                         
                           π 
                           3 
                         
                         ⁢ 
                         
                           
                             
                               ( 
                               
                                 1 
                                 - 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                             ⁢ 
                             
                               ( 
                               
                                 2 
                                 + 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                           
                           
                             
                               ( 
                               
                                 1 
                                 + 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                             ⁢ 
                             sin 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               θ 
                               a 
                             
                           
                         
                         ⁢ 
                         
                           
                             r 
                             2 
                           
                           
                             ϕ 
                             2 
                           
                         
                       
                       } 
                     
                   
                   ≤ 
                   
                     θ 
                     a 
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     8 
                     ) 
                   
                 
               
             
           
         
       
     
     Where Formula (8) above is modified, the following Formula (9) can be obtained. 
     
       
         
           
             
               
                 
                   
                     θ 
                     r 
                   
                   ≤ 
                   
                     2 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     arctan 
                     ⁢ 
                     
                       { 
                       
                         
                           
                             
                               π 
                               3 
                             
                             ⁢ 
                             
                               
                                 
                                   ( 
                                   
                                     1 
                                     - 
                                     
                                       cos 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       
                                         θ 
                                         a 
                                       
                                     
                                   
                                   ) 
                                 
                                 ⁢ 
                                 
                                   ( 
                                   
                                     2 
                                     + 
                                     
                                       cos 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       
                                         θ 
                                         a 
                                       
                                     
                                   
                                   ) 
                                 
                               
                               
                                 
                                   ( 
                                   
                                     1 
                                     + 
                                     
                                       cos 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       
                                         θ 
                                         a 
                                       
                                     
                                   
                                   ) 
                                 
                                 ⁢ 
                                 sin 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ⁢ 
                             
                               V 
                               2 
                             
                           
                           3 
                         
                         ⁢ 
                         
                           1 
                           
                             ϕ 
                             2 
                           
                         
                       
                       } 
                     
                   
                   ≤ 
                   
                     θ 
                     a 
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     9 
                     ) 
                   
                 
               
             
           
         
       
     
     By substituting φ=2r in Formulas (8) and (9) above, it is possible to obtain the following Formulas (8′) and (9′), respectively. 
     
       
         
           
             
               
                 
                   
                     θ 
                     r 
                   
                   ≤ 
                   
                     2 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     arctan 
                     ⁢ 
                     
                       { 
                       
                         
                           π 
                           12 
                         
                         ⁢ 
                         
                           
                             
                               ( 
                               
                                 1 
                                 - 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                             ⁢ 
                             
                               ( 
                               
                                 2 
                                 + 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                           
                           
                             
                               ( 
                               
                                 1 
                                 + 
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     θ 
                                     a 
                                   
                                 
                               
                               ) 
                             
                             ⁢ 
                             sin 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               θ 
                               a 
                             
                           
                         
                       
                       } 
                     
                   
                   ≤ 
                   
                     θ 
                     a 
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     
                       8 
                       ′ 
                     
                     ) 
                   
                 
               
             
             
               
                 
                   
                     θ 
                     r 
                   
                   ≤ 
                   
                     2 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     arctan 
                     ⁢ 
                     
                       { 
                       
                         
                           
                             
                               π 
                               3 
                             
                             ⁢ 
                             
                               
                                 
                                   ( 
                                   
                                     1 
                                     - 
                                     
                                       cos 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       
                                         θ 
                                         a 
                                       
                                     
                                   
                                   ) 
                                 
                                 ⁢ 
                                 
                                   ( 
                                   
                                     2 
                                     + 
                                     
                                       cos 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       
                                         θ 
                                         a 
                                       
                                     
                                   
                                   ) 
                                 
                               
                               
                                 
                                   ( 
                                   
                                     1 
                                     + 
                                     
                                       cos 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       
                                         θ 
                                         a 
                                       
                                     
                                   
                                   ) 
                                 
                                 ⁢ 
                                 sin 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   θ 
                                   a 
                                 
                               
                             
                             ⁢ 
                             
                               V 
                               2 
                             
                           
                           3 
                         
                         ⁢ 
                         
                           1 
                           
                             4 
                             ⁢ 
                             
                               r 
                               2 
                             
                           
                         
                       
                       } 
                     
                   
                   ≤ 
                   
                     θ 
                     a 
                   
                 
               
               
                 
                   Formula 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ( 
                     
                       9 
                       ′ 
                     
                     ) 
                   
                 
               
             
           
         
       
     
     As illustrated in  FIG. 1 , in the present embodiment, the liquid is applied in a state in which both the recording head  12  and the substrate  16  are stationary. Therefore, both nozzle pitches Δx and Δy in the directions x and y of the recording head  12  have to match the dot pitch φ satisfying the condition represented by Formula (3) above. For example, when the recording head  12  illustrated in  FIG. 1  ejects a very large droplet, ejects droplets on a substrate with very high lyophilicity, or ejects a droplet on a thin and long substrate, the recording head  12  such as illustrated in  FIG. 1  can be configured to apply a liquid, without scanning. 
     With the present embodiment, where the dot pitch φ and volume V are controlled based on the conditions (3) and (3′) for causing the droplets to come into contact with each other and be united on the surface of the substrate  16  on the basis of the advancing contact angle θ a  between the substrate  16  and the coating liquid and the droplet volume V and where the values of the advancing contact angle θ a  and receding contact angle θ r  of the substrate  16  and the coating liquid satisfy the conditions (8), (8′), (9) and (9′), the droplets can be reliably applied on the imaging region of the surface of the substrate  16 , without gaps and without oozing from the imaging region. Furthermore, with the liquid coating device  10  of the present embodiment where the above-described conditions are satisfied, the liquid coating rate can be increased and consumption of liquid in coating on the entire surface of the imaging region can be minimized. 
     Other Embodiments of Liquid Coating Device 
     Other embodiments of the liquid coating device  10  will be explained below. 
       FIG. 8  is a perspective view illustrating a liquid coating device of a second embodiment of the present invention.  FIG. 9  is a plan view illustrating a plane formed by nozzles of the recording head  12  of the present embodiment. 
     As illustrated in  FIG. 8 , the coating liquid device (ink jet recording device)  10  of the present embodiment includes an ink jet head (recording head)  12  and a support plate  14 . 
     The recording head  12  is a line-type recording head in which nozzles  20  are arranged side by side over the entire width in the y direction of a substrate  110 . 
     A substrate  16  that is an object of applying a liquid with the recording head  12  is placed on the support plate  14 . The support plate  14  is supported in such a manner that a constant clearance between the support plate  14  and the recording head  12  is maintained, and the scanning therebetween in the main scanning direction (x direction in  FIG. 1 ) can be carried out. 
     The support plate  14  is scanned in the x direction and droplets are ejected from the recording head  12  in each scanning position, thereby making it possible to apply the liquid on the entire surface of the imaging region of the substrate  16 . 
       FIG. 10  is a block diagram illustrating a control system of the liquid coating device of the present embodiment. 
     As illustrated in  FIG. 10 , the liquid coating device  10  of the present embodiment is further provided with a motor driver  48  and a motor  50 . 
     The motor  50  serves to ensure relative scanning of the recording head  12  and the support plate  14  illustrated in  FIG. 8 . The motor driver  48  drives the motor  50  according to a control signal from the system controller  42 . 
     In the example illustrated in  FIG. 8 , a droplet is ejected from the recording head  12  for each scanning position of the recording head  12 , thereby making it possible to apply the liquid on the entire surface of the imaging region of the substrate  16 . 
       FIGS. 11 to 19  are perspective views illustrating other embodiments of the liquid coating device. 
     The liquid coating device  10  illustrated in  FIG. 11  is configured so that the recording head  12  scans (moves) in the x direction and the support plate  14  scans in the y direction. 
     The liquid coating device  10  illustrated in  FIG. 12  is configured so that the recording head  12  scans in the y direction and the support plate  14  scans in the x direction. 
     The liquid coating device  10  illustrated in  FIG. 13  is configured so that the recording head  12  scans in the x direction and y direction. 
     The liquid coating device  10  illustrated in  FIG. 14  is configured so that the support plate  14  scans in the x direction and y direction. 
     The liquid coating device  10  illustrated in  FIG. 15  is configured so that the recording head  12  scans in the x direction and the support plate  14  scans in the x direction and y direction. 
     The liquid coating device  10  illustrated in  FIG. 16  is configured so that the recording head  12  scans in the y direction and the support plate  14  scans in the x direction and y direction. 
     The liquid coating device  10  illustrated in  FIG. 17  is configured so that the recording head  12  scans in the x direction and y direction and the support plate  14  scans in the x direction. 
     The liquid coating device  10  illustrated in  FIG. 18  is configured so that the recording head  12  scans in the x direction and y direction and the support plate  14  scans in the y direction. 
     The liquid coating device  10  illustrated in  FIG. 19  is configured so that the recording head  12  scans in the x direction and y direction and the support plate  14  scans in the x direction and y direction. 
     In the examples illustrated in  FIGS. 11 to 19 , at least one of the recording head  12  and the substrate  16  is driven and a droplet is ejected from the recording head  12  for each scanning position, thereby making it possible to apply the liquid on the entire surface of the imaging region of the substrate  16 . 
     As in the examples illustrated in  FIGS. 8 to 19 , when at least one of the recording head  12  and the substrate  16  is movable, it is desirable that the number of scans of the imaging region when the liquid is applied on the substrate  16  should be one. The entire substrate  16  may be also scanned a plurality of times. 
     It is also preferred that the nozzle pitches Δx and Δy of the recording head  12  satisfy any one of conditions [1] and [2] below.
     [1] A dot pitch in the main scanning direction (x direction) (dot pitch φ satisfying the condition represented by Formula (3) above) is equal to the nozzle pitch Δx in the main scanning direction of the recording head  12 .   [2] A dot pitch in the sub-scanning direction (y direction) (dot pitch φ satisfying the condition represented by Formula (3) above) is equal to the nozzle pitch Δy in the sub-scanning direction of the recording head  12 .   

     The recording head  12 , as referred to herein, means the entire configuration that ejects the liquid. The nozzle pitch, as referred to herein, means the nozzle spacing when ejection positions at which the nozzles eject the liquid are virtually arranged on a straight line that is drawn in the relative movement direction of the substrate  16  and the recording head  12 . 
     In a line-type recording head  12  in which the relative movement direction of the recording head  12  and the substrate  16  is one direction and the nozzles  20  are arranged side by side over the entire width in the y direction of the substrate  110 , as illustrated in  FIG. 8 , it is preferred that the nozzle pitch Δx in the main scanning direction of the recording head  12  and the nozzle pitch Δy in the sub-scanning direction be equal to the dot pitch φ satisfying the condition represented by Formula (3) above. 
     As illustrated in  FIGS. 11 to 19 , when there are two or more relative movement directions of the recording head  12  and the substrate  16 , it is preferred that the nozzle pitch Δx in the main scanning direction of the recording head  12  and the nozzle pitch Δy in the sub-scanning direction be integral multiples (positive integral multiples) of the dot pitch φ satisfying the condition represented by Formula (3) above. With the above-described configuration of nozzle pitches of the recording head  12 , the movement amount of the recording head  12  and the support plate  14  during driving becomes discrete and the drive system can be simplified. 
     When there are two or more relative movement directions of the recording head  12  and the substrate  16 , it is more preferred that the nozzle pitch Δx in the main scanning direction of the recording head  12  and the nozzle pitch Δy in the sub-scanning direction be equal to the dot pitch φ satisfying the condition represented by Formula (3) above. In this case, the movement amount during driving becomes constant and the drive system can be greatly simplified. 
     Instead of determining the nozzle pitches of the recording head  12  on the basis of the condition relating to the dot pitch φ, it is also possible, for example, to perform scanning with an inclined recording head  12  so that the nozzle pitch becomes a positive integral multiple of the dot pitch φ. 
     Embodiment of Radiation Detector 
     An embodiment of a radiation detector produced using the liquid coating device  10  of the present embodiment will be described below. 
     The radiation detector of the present embodiment is suitable for X ray pickup devices or the like, includes an electrostatic recording unit having a photoconductive layer that becomes conductive when irradiated with radiation, receives radiation carrying image information, records the image information, and outputs an image signal representing the recorded image information. 
     Examples of radiation detectors include a radiation detection substrate  500  of the so-called optical reading system in which reading is performed using a semiconductor material that generates an electric charge under light illumination and a radiation detector  400  of a system (referred to hereinbelow as “TFT system”) in which electric charges generated by irradiation with radiation are accumulated and the accumulated electric charges are read out by ON-OFF switching of an electric switch such as a thin-film transistor (TFT) by one pixel. 
     Configuration of Radiation Detector  400  of TFT System 
     A configuration of the radiation detector  400  of a TFT system will be explained below.  FIG. 20A  is a schematic diagram illustrating the entire configuration of the radiation detector  400  of a TFT system.  FIG. 21  illustrates principal configuration of the radiation detector  400  of a TFT system and illustrates components laminated on a glass substrate. 
     The radiation detector  400  of a TFT system of the present embodiment is provided with a photoconductive layer  404  that demonstrates an electromagnetic wave conductivity as a charge conversion layer generating electric charges under irradiation with X rays as an example of radiation carrying image information, as illustrated in  FIG. 20A  and  FIG. 21 . A noncrystalline (amorphous) material that has a high dark resistance, demonstrates good electromagnetic wave conductivity in response to X ray irradiation, and can be formed as a film of a large surface area at a low temperature by a vacuum vapor deposition method is preferred as the photoconductive layer  404 . 
     For example, an amorphous Se (a-Se) film is used as the noncrystalline (amorphous) material. Furthermore, materials obtained by doping amorphous Se with As, Sb, and Ge have excellent thermal stability and are preferred for the photoconductive layer  404 . 
     A bias electrode  401  that applies a bias voltage to the photoconductive layer  404  is formed as a first electrode that transmits radiation carrying image information on the photoconductive layer  404 . The bias electrode  401  is formed, for example, from gold (Au). The radiation transmitted by the bias electrode  401  falls on the photoconductive layer  404 . 
     A plurality of charge collecting electrodes  407   a  are formed as second electrodes collecting electric charges generated by the photoconductive layer  404  on the side opposite the side on which the bias electrode  401  is provided with respect to the photoconductive layer  404 , that is, below the photoconductive layer  404 . As illustrated in  FIG. 21 , the charge collecting electrodes  407   a  are connected to respective charge accumulating capacitors  407   c  and switch elements  407   b . The charge collecting electrodes  407   a  are also provided on the glass substrate  408 . 
     Furthermore, as illustrated in  FIG. 20A  and  FIG. 21 , a hole injection preventing layer  402  that has a hole blocking material is provided as an organic polymer layer between the photoconductive layer  404  and the bias electrode  401 . The organic polymer layer may also serve as a charge injection blocking layer having charge selectivity. The charge injection blocking layer having charge selectivity, as referred to herein, is a layer that has a property of blocking electric charges (holes when the bias electrode  401  has a positive bias and electrons when it has a negative bias) flowing out of the bias electrode  401 , which is in contact with the charge injection blocking layer, and transmitting electric charges flowing to the bias electrode  401 . 
     Thus, a hole injection blocking layer that blocks the injection of holes, while serving as a conductor with respect to electrons, or an electron injection blocking layer that blocks the injection of electrons, while being a conductor with respect to holes, can be used as the charge injection blocking layer. In the present embodiment, because the bias electrode  401  is a positive electrode, the hole injection blocking layer  402  is provided as the organic polymer layer. 
     A film in which a hole blocking material is mixed with an insulating polymer such as a polycarbonate, polystyrene, a polyimide, and a polycycloolefin can be advantageously used as the hole injection blocking layer  402 . 
     At least one kind of a hole blocking material contained in the hole injection blocking layer  402  is desirably of at least one kind selected from carbon clusters and derivatives thereof. The carbon cluster is desirably of at least one kind selected from fullerene C60, fullerene C70, fullerene oxide, and derivatives thereof. 
     As illustrated in  FIG. 21 , an electron injection blocking layer  406  is provided between the photoconductive layer  404  and the charge collecting electrode  407   a.    
     Crystallization blocking layers  403  and  405  are provided between the hole injection blocking layer  402  and the photoconductive layer  404  and between the electron injection blocking layer  406  and the photoconductive layer  404 , respectively. GeSe, GeSe 2 , Sb 2 Se 3 , a-As 2 Se 3 , Se—As, Se—Ge, and Se—Sb compounds can be used for the crystallization blocking layers  403  and  405 . 
     An active matrix layer  407  is configured by the charge collecting electrodes  407   a,  switch elements  407   b , and charge accumulation capacitors  407   c . An active matrix substrate  450  is configured by the glass substrate  408  and active matrix layer  407 . 
       FIG. 22  is a cross-sectional view illustrating the structure of a one-pixel unit of the radiation detector  400 .  FIG. 23  is a plan view thereof. One pixel illustrated in  FIG. 22  and  FIG. 23  has a size of about 0.1 mm×0.1 mm to 0.3 mm×0.3 mm. In the entire radiation detector, the pixels are arranged as a matrix including about 500×500 to 3000×3000 pixels. 
     As illustrated in  FIG. 22 , the active matrix substrate  450  has the glass substrate  408 , gate electrodes  411 , charge accumulating capacitor electrodes (referred to hereinbelow as Cs electrodes)  418 , a gate insulating film  413 , drain electrodes  412 , a channel layer  415 , collector electrodes  416 , source electrodes  410 , an insulating protective film  417 , an interlayer insulating film  420 , and charge collecting electrodes  407   a.    
     The switch element  407   b  composed of a thin-film transistor (TFT) is configured by the gate electrode  411 , gate insulating film  413 , source electrode  410 , drain electrode  412 , channel layer  415 , and contact electrode  416 . The charge accumulation capacitor  407   c  is configured by the Cs electrode  418 , gate insulating film  413 , and drain electrode  412 . 
     The glass substrate  408  is a support substrate. For example, an alkali-free glass substrate (for example, #1737 manufactured by Corning Co.) can be used as the glass substrate  408 . The gate electrodes  411  and source electrodes  410  are electrode wirings arranged in a grid-like configuration, as illustrated in  FIG. 23 , and the switch element  407   b  composed of a thin-film transistor is formed in the intersection points of the electrodes. 
     A source and a drain of the switch element  407   b  are connected to the source electrode  410  and drain electrode  412 , respectively. The source electrode  410  is provided with a linear portion as a signal line and an extending portion for configuring the switch element  407   b.  The drain electrode  412  is provided so as to link the switch element  407   b  and the charge accumulating capacitor  407   c.    
     A take-out electrode  470  that takes out the electric charge collected at the charge collecting electrode  407   a  is connected to the source electrode  410  for acquiring image information. The take-out electrode  470  is provided at the glass substrate  408  and disposed outside the photoconductive layer  404 . 
     The gate insulating film  413  is composed of SiNx or SiOx. The gate insulating film  413  is provided to cover the gate electrode  411  and Cs electrode  418 . A zone of the gate insulating film positioned above the gate electrode  411  acts as a gate insulating film in the switch element  407   b , and the zone positioned above the Cs electrode  418  acts as a dielectric layer in the charge accumulating capacitor  407   c . In other words, the charge accumulating capacitor  407   c  is formed by a superposition region of the drain electrode  412  and the Cs electrode  418  formed in the same layer as the gate electrode  411 . Not only SiNx and SiOx, but also an anodization film obtained by anodization of the gate electrode  411  and Cs electrode  418  can be used as the gate insulating film  413 . 
     Furthermore, the channel layer (i layer)  415  is a channel portion of the switch element  407   b  and serves as a current channel linking the source electrode  410  and the drain electrode  412 . The contact electrode (n+ layer)  416  serves as a contact of the source electrode  410  and the drain electrode  412 . 
     The insulating protective film  417  is formed on the source electrode  410  and the drain electrode  412 , that is, on the glass substrate  408  over almost the entire surface (almost the entire region). As a result, the drain electrode  412  and source electrode  410  are protected and also electrically insulated and separated. Furthermore, the insulating protective film  417  has a contact hole  421  in a predetermined position thereof, that is, in a zone positioned on a portion facing the Cs electrode  418  in the drain electrode  412 . 
     The charge collecting electrode  407   a  is configured by an amorphous transparent conductive oxide film. The charge collecting electrode  407   a  is formed to fill the contact hole  421  and laminated on the source electrode  410  and the drain electrode  412 . The charge collecting electrode  407   a  and the photoconductive layer  404  are electrically connected so that the electric charges generated in the photoconductive layer  404  can be collected at the charge collecting electrode  407   a.    
     The charge collecting electrode  407   a  will be described below in greater detail. The charge collecting electrode  407   a  used in the present embodiment is configured by an amorphous transparent conductive oxide film. Materials having an oxide of indium and tin (ITO: Indium-Tin-Oxide), an oxide of indium and zinc (IZO: Indium-Zinc-Oxide), or an oxide of indium and germanium (IGO Indium-Germanium-Oxide) as a basis composition can be used as the amorphous transparent conductive oxide film. 
     A variety of metal films and conductive oxide films have been used as the charge collecting electrode  407   a , but transparent conductive oxide films such as ITO (Indium-Tin-Oxide) are used most often for the following reasons. When an incident X ray dose in the radiation detector  400  is high, unnecessary electric charges are sometimes trapped in a semiconductor film (or close to an interface of the semiconductor film and an adjacent layer). 
     These residual charges are stored for a long time or transferred over a long time. The resultant problem is that an X ray detection characteristic during subsequent image detection is degraded or a residual image (latent image) is developed. Accordingly, Japanese Patent Application Publication No. 9-9153 (corresponding U.S. Pat. No. 5,563,421) discloses a method by which when residual charges are generated in the photoconductive layer  404 , the residual charges are excited and removed by light irradiation from the outside of the photoconductive layer  404 . In this case, in order to perform light irradiation with good efficiency from below the photoconductive layer  404  (side of the charge collecting electrode  407   a ), it is necessary that the charge collecting electrode  407   a  be transparent to the irradiation light. 
     It is desirable that the charge collecting electrode  407   a  be formed so as to cover the switch element  407   b  in order to increase a surface area filling ratio (filling factor) of the charge collecting electrode  407   a  or shield the switch element  407   b . However, if the charge collecting electrode  407   a  is not transparent, the switch element  407   b  cannot be observed after the charge collecting electrode  407   a  has been formed. 
     For example, in the case the characteristics of the switch element  407   b  are inspected after the charge collecting electrode  407   a  has been formed, where the switch element  407   b  is covered with the charge collecting electrode  407   a  that is not transparent, when property deterioration of the switch element  407   b  is found, observations under an optical microscope or the like cannot be performed to clarify the reasons for such property deterioration. Therefore, it is desirable that the charge collecting electrode  407   a  be transparent, thereby making it possible to observe easily the switch element  407   b  even after the charge collecting electrode  407   a  has been formed. 
     The interlayer insulating film  420  is composed of a photosensitive acrylic resin and serves for electric insulation and separation of the switch element  407   b . A through contact hole  421  is formed in the interlayer insulating film  420 , and the charge collecting electrode  407   a  is connected to the drain electrode  412 . As illustrated in  FIG. 22 , the contact hole  421  is formed to have an inverse tapered shape. A high-voltage power source (not illustrated in the figure) is connected between the bias electrode  401  and the Cs electrode  418 . 
     The configuration covering the photoconductive layer  404  will be explained below. As illustrated in  FIG. 20A , a cover glass  440  as an example of a cover member that covers the bias electrode  401  is provided above the bias electrode  401 . 
     A protective member  442  to which the cover glass  440  is bonded is provided on the glass substrate  408 . 
     The protective member  442  is formed to have a box-like shape that surrounds the photoconductive layer  404  and is open as a whole at the top and bottom. 
     The protective member  442  is formed to have an L-like cross section and has a side wall  442   a  provided in a vertical condition on the outer circumferential portion of the glass substrate  408  and a flange portion  442   b  that protrudes from the upper portion of the side wall  442   a  toward the upper side of the central portion of the glass substrate  408 . 
     An upper surface of the outer circumferential portion of the cover glass  440  is joined to a lower surface (inner wall) of the flange portion  442   b  and supported by the protective member  442 . 
     The joint portion of the protective member  442  and the cover glass  440  is disposed outside the photoconductive layer  404 . Thus, the protective member  442  and the cover glass  440  are joined in a region where the photoconductive layer  404  located on the glass substrate  408  is not present, rather than above the photoconductive layer  404 . 
     An insulating member having insulating properties is used for the protective member  442 . For example, a polycarbonate, polyethylene terephthalate (PET), polymethyl(acryl)methacrylate, and polyvinyl chloride can be used as the insulating member. 
     The lower opening of the protective member  442  is closed by the glass substrate  408 , and the upper opening is closed with the cover glass  440 , thereby forming a closed space of a predetermined volume inside the protective member  442 . The photoconductive layer  404  is accommodated in this closed space, and the photoconductive layer  404  is covered by the cover glass  440 , glass substrate  408 , and protective member  442 . 
     The space surrounded by the cover glass  440 , protective member  442 , and glass substrate  408  is filled with a curable resin  444  serving as a filling member. For example, a resin curable at normal temperature, such as epoxy resin or silicone can be used as the curable resin  444 . 
     Formation Range of Hole Injection Blocking Layer  402   
     A formation range of the hole injection blocking layer  402  will be explained below. 
     An outer edge portion of the hole injection blocking layer  402  serving as an organic polymer layer, that is, a circumferential edge serving as a boundary with other layers is located in a predetermined position. As a result, the hole injection blocking layer  402  is formed within a predetermined range and has a configuration covering the predetermined range. 
     In the configuration of the present embodiment, the outer edge portion of the hole injection blocking layer  402  is positioned between a region end G 1  of an image information acquisition region G where image information is acquired and the take-out electrode  470 , within a region irradiated with radiation carrying the image information. A range represented by arrow A in  FIG. 20A  is between the region end G 1  of an image information acquisition region G and the take-out electrode  470 . 
     In the preferred configuration, the outer edge portion of the hole injection blocking layer  402  of the present embodiment is located outside the image information acquisition region G and within a region having a film thickness equal to or greater than 10% the average film thickness of the flat portion of the photoconductive layer  404 . The average film thickness of the flat portion of the photoconductive layer  404  is determined by measuring a film thickness in any nine points within a region of the image information acquisition region G of the photoconductive layer  404  and finding an average film thickness for these nine points. The film thickness is measured by observing the cross section of the film under a microscope with a magnification factor of 100. 
     A range represented by arrow B in  FIG. 20A  is outside the image information acquisition region G and within a region having a film thickness equal to or greater than 10% the average film thickness of the flat portion of the photoconductive layer  404 . 
     In even more preferred configuration, the outer edge portion of the hole injection blocking layer  402  of the present embodiment is located outside the bias electrode  401  and within a region having a film thickness equal to or greater than 10% the average film thickness of the flat portion of the photoconductive layer  404 . 
     A range represented by arrow C in  FIG. 20A  is outside the bias electrode  401  and within a region having a film thickness equal to or greater than 10% the average film thickness of the flat portion of the photoconductive layer  404 . 
     In even more preferred configuration, the outer edge portion of the hole injection blocking layer  402  of the present embodiment is located outside the bias electrode  401  and within a region in which a gradient of an end portion bevel of the photoconductive layer  404  is equal to or less than 50%. 
     The outer edge portion of the hole injection blocking layer  402  is positioned within a region with a gradient of equal to or less than 50% in the end portion bevel of the photoconductive layer  404  in which the gradient gradually increases from the flat portion to the outer edge, that is, within a range in which the gradient is more gradual than a gradient of 50%. The gradient of 50% is a gradient formed by an inclined side in a rectangular triangle configured by a side along the film thickness direction of the photoconductive layer  404 , a side perpendicular to this side, and the inclined side, as illustrated in  FIG. 20B , in which where the length of the side along the film thickness direction of the photoconductive layer  404  is taken as 1, the length of the side perpendicular to this side is 2. The gradient is measured by observing the cross section under a microscope with a magnification of 100. 
     A range represented by arrow D in  FIG. 20A  is outside the bias electrode  401  and within a region in which the gradient of the end portion bevel of the photoconductive layer  404  is equal to or less than 50%. 
     The photoconductive layer  404  is formed in a region wider than the bias electrode  401 . Furthermore, the charge collecting electrode  407   a  is formed in a region wider than the image information acquisition region G. 
     The outer edge portion of the hole injection blocking layer  402  of the present embodiment may be positioned outside the image information acquisition region G and in the region of the photoconductive layer  404 . 
     Operation Principle of Radiation Detector of TFT System 
     The operation principle of the radiation detector  400  of a TFT system will be described below. Where the photoconductive layer  404  is irradiated with X rays, electric charges (electron-hole pairs) are generated inside the photoconductive layer  404 . In a state in which a voltage is applied between the bias electrode  401  and the Cs electrode  418 , that is, in a state in which a voltage is applied to the photoconductive layer  404  via the bias electrode  401  and the Cs electrode  418 , a structure is produced in which the photoconductive layer  404  and the charge accumulating capacitor  407   c  are electrically connected in serial. Therefore, the electrons generated in the photoconductive layer  404  move to the + electrode side and holes move to the − electrode side. As a result, electric charges are accumulated in the charge accumulating capacitor  407   c.    
     The electric charges accumulated in the charge accumulating capacitor  407   c  can be taken out from the source electrode  410  to the outside via the take-out electrode  470  by setting the switch element  407   b  into an ON state by an input signal to the gate electrode  411 . Furthermore, because the electrode wirings composed of gate electrodes  411  and source electrodes  410 , switch element  407   b , and charge accumulating capacitor  407   c  are all provided in a matrix-like configuration, image information of X rays can be obtained two dimensionally by successively scanning the signals inputted to the gate electrode  411  and detecting the signal from the source electrode  410  for each source electrode  410 . 
     EXAMPLE 1 
     In Example 1, an electron injection blocking layer  406  composed of antimony sulfide and having a thickness of 2 μm was formed on an active matrix substrate  450 . Then, a crystallization blocking layer  405  with a thickness of 0.15 μm was formed by vapor depositing a Se starting material containing 3% As. A photoconductive layer  404  composed of amorphous Se and having a thickness of 1000 μm was formed by vapor depositing a Se starting material containing 10 ppm Na. 
     A hole injection blocking layer  402  was formed as an organic polymer layer by using an ejection liquid including a hole blocking material of at least one kind selected from carbon clusters and derivatives thereof and at least one from aromatic solvents represented by General Chemical Formulas (1) and (2). 
     
       
                 
         
             
             
         
      
     
     (In the General Chemical Formulas (1) and (2), R 1 -R 8  represent hydrogen, a halogen, or an alkyl group). 
     In the present example, fullerene C60 was used as the carbon cluster. Fullerene C60 was nanom purple (C60) manufactured by Frontier Carbon Corp. 
     Furthermore, in the present example, the coating liquid was prepared by dissolving 1.05 wt. % polycarbonate resin (PCz) (lupilon PCz-400, manufactured by Mitsubishi Gas Chemical Co., Ltd.) and 30 wt. % (based on the PCz) fullerene C60 in o-dichlorobenzene serving as the aforementioned aromatic solvent. 
     The ejection liquid had a dilatancy property. The dilatancy property is an ability of a liquid to increase in viscosity in response to increase in a shear rate. The relationship between shear rate and shear viscosity of the ejection liquid was measured with a rheometer. The shear rate was measured twice within a range of 10 to 1000 s −1 . The average value is illustrated in  FIG. 24 . Because the shear viscosity increased with the increase in shear rate, it can be said that the ejection liquid has a dilatancy property. 
     The exponential approximate equation of the graph illustrated in  FIG. 24  is y=2.2331e 1E-05x . A shear rate applied to the ejection liquid during ejection from an ink jet head is generally considered to be about 10 5  s −1 , and a shear viscosity in this case is estimated at 6.07 mPa·s. Meanwhile, because the shear rate after landing can be taken as 0 s −1 , the shear viscosity at this time can be estimated as 2.23 mPa·s. Because viscosity decreases after landing, the liquid spreads easily and is clearly suitable for forming a uniform film. 
     Furthermore, a contact angle of the ejection liquid with the photoconductive layer  404  is taken to be equal to or less than 45°. In the present example, an ejection liquid was used that had a contact angle of 5° with the photoconductive layer  404 . 
     The ejection liquid was loaded in an ink jet head SE-128 manufactured by FUJIFILM Dimatix, Inc., and ejection was carried out into a range that was wider than the image information acquisition region G and did not cover the take-out electrode  470 . A solvent was evaporated in a vacuum drier and a hole injection blocking layer  402  with a thickness of 0.2 μm was obtained. Finally, an Au film was formed by vapor deposition on the inside of the end of the hole injection blocking layer  402  and the bias electrode  401  with a thickness of 0.1 μm was obtained. 
     In the configuration of the present example, the outer edge portion of the hole injection blocking layer  402  is positioned at a distance of 1 mm from the take-out electrode  470  on the side of the image information acquisition region G and between the take-out electrode  470  and the region end G 1  of the image information acquisition region G where image information is acquired. 
     As a result, the image information acquisition region G of the photoconductive layer  404  is covered with the hole injection blocking layer  402 , degradation of the photoconductive layer  404  such as crystallization in the image information acquisition region G can be inhibited, and endurance of the radiation detector  400  is increased. Because the hole injection blocking layer  402  does not cover the take-out electrode  470 , adverse effect on conduction of the take-out electrode  470  can be prevented. 
     EXAMPLE 2 
     In the configuration of Example 2, the outer edge portion of the hole injection blocking layer  402  is positioned within 1 mm from the end of the bias electrode  401  and within a region that is outside the image information acquisition region G and has a thickness of equal to or more than 10% the average thickness of the flat portion of the photoconductive layer  404 . 
     With the configuration of the present example, the hole injection blocking layer  402  having charge selectivity does not cover a region having a thickness less than 10% the average thickness of the flat portion of the photoconductive layer  404 , that is, a region of small thickness, thereby inhibiting the occurrence of a surface discharge generated along the hole injection blocking layer  402 . 
     EXAMPLE 3 
     In the configuration of Example 3, the outer edge portion of the hole injection blocking layer  402  is positioned in a location with 50% the average thickness of the flat portion of the photoconductive layer  404  and within a region that is outside the bias electrode  401  and has a thickness of equal to or more than 10% the average thickness of the flat portion of the photoconductive layer  404 . 
     With the configuration of the present example, the hole injection blocking layer  402  covers the end portion of the bias electrode  401 , thereby inhibiting a discharge breakdown caused by electric field concentration at the end portion of the bias electrode  401 . 
     EXAMPLE 4 
     In the configuration of Example 4, the outer edge portion of the hole injection blocking layer  402  is positioned 2 mm outside the end of the bias electrode  401  and within a region that is outside the bias electrode  401  and in which the gradient of the end portion bevel of the photoconductive layer  404  is equal to or less than 50%. 
     With the configuration of the present example, because the hole injection blocking layer  402  is formed in the region in which the gradient of the end portion bevel of the photoconductive layer  404  is equal to or less than 50%, no liquid sagging occurs even when the hole injection blocking layer  402  is formed from a liquid material. Where a liquid pool is produced by sagging, crystallization of C60 occurs and a surface discharge is easily induced, but in the present example, no sagging occurs and, therefore, the surface discharge can be inhibited. 
     Furthermore, the hole injection blocking layer  402  may have a two-layer structure, and antimony sulfide may be laminated to a film thickness of 0.6 μm on the organic polymer layer including a fullerene. Such a configuration increases hole blocking ability. 
     Configuration of Radiation Detector of Optical Reading System 
     The present invention is also applicable to a radiation detector of an optical reading system and can be applied correspondingly to the configuration of the hole injection blocking layer  402  in the above-described radiation detector  400 . Here, a radiation detection substrate  500  serving as a radiation detector of an optical reading system will be described. 
       FIGS. 25A and 25B  are schematic drawings of the radiation detection substrate  500 . As illustrated in  FIGS. 25A and 25B , TCP  510  and a read device  512  and a high-voltage wire  514  for applying a high voltage, which are connected via the TCP  510 , are connected to the radiation detection substrate  500 . 
     The TCP (Tape Carrier Package)  510  is a flexible wiring board carrying IC (charge amplifying IC)  511  for signal detection. The TCP  510  are connected by thermal press bonding by using an ACF (Anisotropic Conductive Film). 
     An extending electrode portion  519  that extends from an upper electrode  518  located in the upper portion of a detection area  516  is formed, and the high-voltage wire  514  is connected to the extending electrode portion  519 . The detection area  516  that detects radiation is configured by a lower electrode  520  for signal reading and high voltage application, a radiation detection layer  522  that converts radiation into electric charges, and the upper electrode  518  that applies a high voltage. 
     The lower electrode  520  is provided on a glass substrate  536 , and a lower substrate  524  for radiation detection is configured by the glass substrate  536  provided with the lower electrode  520 . 
     The process for manufacturing the radiation detection substrate  500  can be generally divided into production of the lower substrate  524  for radiation detection that includes the lower electrode  520 , formation of the radiation detection layer  522  and upper electrode  518 , and connection of the high-voltage wire  514 . 
     The structure of the lower substrate  524  for radiation detection will be explained below.  FIGS. 26A and 26B  illustrate a schematic structure of the lower substrate  524  for radiation detection. In the simplified structure illustrated in  FIGS. 26A and 26B , The TCP  510  are provided by one on the left and right sides, the number of channels is three on each side, and the total number of channels is six. As illustrated in  FIGS. 26A and 26B , the lower substrate  524  for radiation detection is configured by a radiation detection portion  526 , a pitch conversion portion  528 , and a TCP connection portion  530  serving as a take-out electrode. 
     In a radiation detection portion  526 , the lower electrode  520  for taking out the signals is arranged in a stripe-like (linear) shape. Furthermore, a color filter layer  534  that partially transmits light of a random wavelength is formed on the lower layer via a transparent organic insulating layer  532 . 
     A layer present above the color filter layer  534  is called a common B line  520 B, and a portion where the color filter layer  534  is not present is called a signal S line  520 S. The B line  520 B is shared outside the radiation detection portion and has a comb-shaped electrode structure. The S line  520 S is used as a signal line. The width of the B line  520 B is, for example, 20 μm, the width of the S line  520 S is, for example, 10 μm, and the distance between the B line  520 B and the S line  520 S is, for example, 10 μm. 
     The width of the color filter layer  534  is, for example, 30 μm. The lower electrode  520  has to be transparent to enable light irradiation from the back surface and has to be flat to avoid breakdown of the like caused by electric field concentration during application of a high voltage and, for example, IZO or ITO is used therefor. When IZO is used, the thickness is 0.2 μm and the flatness is about Ra=1 nm. 
     The color filter layer  534  is from a photosensitive resist having a pigment dispersed therein, for example, a red resist used for a color filter of a LCD. A transparent insulating layer  532  of a photosensitive organic material such as PMMA is used to eliminate steps in the color filter layer  534 . 
     The glass substrate  536  serving as a support member is desirably a transparent and rigid substrate. Furthermore, it is desirable that the glass be soda-lime glass. Examples of thickness of each layer are as follows: lower electrode 520: 0.2 μm, color filter layer  534 : 1.2 μm, organic transparent insulating layer  532 : 1.8 μm, and glass substrate  536 : 1.8 μm. The color filter layer  534  and organic insulating layer  532  are present only in the radiation detection portion  526 , and the boundaries thereof are present in the radiation detection portion  526  and a pitch conversion portion  528 . For this purpose, the IZO wiring is formed on the glass substrate  536  in the TCP connection portion  530  via a boundary step portion of the organic insulating layer  532 . 
     In the radiation detection portion  526 , a wiring is taken out to the left and right TCP  510 , wherein several packages are considered as a unit. In  FIG. 23 , three lines are taken as a unit. The number of lines is, for example,  256 . The line width in the radiation detection portion  526  is different from the line width in the TCP connection portion  530 , and the line width is adjusted in the pitch conversion portion  528  to adjust the line width in the radiation detection portion and pull the wiring around to the predetermined TCP connection position. The B line  520 B is shared and similarly pulled out to the TCP connection portion  530 . 
     The signal S line  520 S and the common B line  520 B shared on the outside of the radiation detection portion are disposed in the TCP connection portion  530 . The common B line  520 B is disposed outside the signal S line  520 S. For example, there are 256 signal lines and they are connected to the TCP by using five upper and five lower common lines. The electrode line-to-space ratio is 40 to 40 μm. 
     Furthermore, a TCP alignment mark is necessary for connecting the TCP in the TCP connection portion  530 . It is desirable that the mark be formed of a transparent electrode, but because the mark is transparent, it is difficult to recognize. For this reason, the alignment mark is formed using a non-transparent material, for example, the color filter layer  534  serving as a constituent member of the substrate. 
     The radiation detection layer  522  will be explained below.  FIG. 27  is a schematic diagram illustrating the configuration of the radiation detection substrate  500 . The radiation detection layer is configured by providing a photoconductive layer  542  for recording, a charge accumulating layer  544 , a photoconductive layer  546  for reading, an electrode interface layer  548 , an underlayer  550 , and an overlayer  552 , as illustrated in  FIG. 27 . 
     Photoconductive Layer for Recording 
     The photoconductive layer  542  for recording is configured by a compound containing as a main component at least one from among amorphous selenium compounds, Bi 12 MO 20  (M: Ti, Si, or Ge), Bi 4 M 3 O 12  (M: Ti, Si, or Ge), Bi 2 O 3 , BiMO 4  (M: Nb, Ta, or V), Bi 2 WO 6 , Bi 24 B 2 O 39 , ZnO, ZnS, ZnSe, ZnTe, MNbO 3  (M: Lie, Na, or K), PbO, HgI 2 , PbI 2 , CdS, CdSe, CdTe, BiI 3 , and GaAs, which are photoconductive substances generating electric charges upon absorption of electromagnetic waves. Among them, amorphous selenium compounds are especially preferred. 
     In the case of amorphous selenium compounds, those can be used for the layer that are microdoped with 0.001 ppm to 1 ppm an alkali metal such as Li, Na, K, Cs, and Rb, those microdoped with 10 ppm to 10,000 ppm a fluoride such as LiF, NaF, KF, CsF, and RbF, those doped with 50 ppm to 0.5% P, As, Sb, or Ge, those doped with 10 ppm to 0.5% As, and those microdoped with 1 ppm to 100 ppm Cl, Br, or I. 
     In particular, amorphous selenium containing about 10 ppm to 200 ppm As, amorphous selenium containing about 0.2% to 1% As and also 5 ppm to 100 ppm Cl, and amorphous selenium containing about 0.001 ppm to 1 ppm alkali metal can be advantageously used. 
     Furthermore, compositions containing fine particles of a photoconductive substance such as Bi 12 MO 20  (M: Ti, Si, or Ge), Bi 4 M 3 O 12  (M: Ti, Si, or Ge), Bi 2 O 3 , BiMO 4  (M: Nb, Ta, or V), Bi 2 WO 6 , Bi 24 B 2 O 39 , ZnO, ZnS, ZnSe, ZnTe, MNbO 3  (M: Li, Na, or K), PbO, HgI 2 , PbI 2 , CdS, CdSe, CdTe, BiI 3 , and GaAs with a particle size of from several nanometers to several microns can be used. 
     In the case of amorphous selenium, the thickness of the photoconductive layer  542  for recording is desirably equal to or greater than 100 μm and equal to or less than 2000 μm. In particular, in applications for mammography, a range of thickness equal to or greater than 150 μm and equal to or less than 250 μm is especially preferred, and in applications for general imaging, a range of thickness equal to or greater than 500 μm and equal to or less than 1200 μm is especially preferred. 
     Charge Accumulating Layer 
     The charge accumulating layer  544  may be any film, provided it has insulating properties with respect to charges of a polarity that is wished to be accumulated, and can be configured by a polymer such as an acrylic organic resin, a polyimide, BCB, PVA, acryl, polyethylene, a polycarbonate, and a polyetherimide, a sulfide such as As 2 S 3 , Sb 2 S 3 , and ZnS, and also by an oxide and a fluoride. Furthermore, a substance that has insulating properties with respect to charges of a polarity that is wished to be accumulated and has conductive properties with respect to charges of opposite polarity is more preferred, and also a substance is preferred in which a difference in a product of mobility×life between the charges of different polarity is equal to or greater than three orders of magnitude. 
     Examples of preferred substances include As 2 Se 3 , As 2 Se 3  doped with 500 ppm to 20,000 ppm Cl, Br, and I, As 2 (Se x Te 1-x ) 3  (0.5&lt;x&lt;1) obtained by substituting Se in As 2 S 3  with Te up to about 50%, As 2 Se 3  in which Se is substituted with S up to about 50%, As x Se y  (x+y=100, 34≦x≦46) obtained by changing As concentration from As 2 Se 3  by about ±15%, and an amorphous Se—Te system containing 5 to 30 wt. % Te. 
     When a substance containing such chalcogenide elements is used, the thickness of the charge accumulating layer  544  is desirably equal to or greater than 0.4 μm and equal to or less than 3.0 μm, more desirably equal to or greater than 0.5 μm and equal to or less than 2 μm. Such a charge accumulating layer  544  may be formed by a single-step formation process, or may be obtained by lamination in a plurality of steps. 
     A compound obtained by doping a polymer such as an acrylic organic resin, a polyimide, BCB, PVA, acryl, polyethylene, a polycarbonate, and a polyetherimide with a charge transfer agent can be advantageously used as the preferred charge accumulating layer  544  using an organic film. Examples of preferred charge transfer agents include molecules selected from a group including tris(8-quinolinolato)aluminum (Alq3), N,N-diphenyl-N,N-di(m-tolyl)benzidine (TPD), polyparaphenylenevinylene (PPV), a polyalkylthiophene, polyvinylcarbazole (PVK), triphenylene (TNF), metal phthalocyanines, 4-(dicyanomethylene)-2-methyl-6-(p-dimethylaminostyryl)-4H-pyran (DCM), liquid crystal molecules, hexapentyloxytriphenylene, discotic liquid crystal molecules in which a central core has a π-conjugated condensation ring or a transition metal, carbon nanotubes, and fullerenes. The doped amount is set between 0.1 wt. % and 50 wt. %. 
     Photoconductive Layer for Reading 
     The photoconductive layer  546  for reading can used a semiconductor substance in which an energy gap is contained within a range of 0.7 eV to 2.5 eV, such as amorphous selenium compounds, amorphous Si:H, crystalline Si, and GaAS, which are photoconductive substance generating electric charges upon absorption of electromagnetic waves, in particular visible light. Among them, amorphous selenium is especially preferred. 
     In the case of amorphous selenium compounds, those can be used for the layer that are microdoped with 0.001 ppm to 1 ppm an alkali metal such as Li, Na, K, Cs, and Rb, those microdoped with 10 ppm to 10,000 ppm a fluoride such as LiF, NaF, KF, CsF, and RbF, those doped with 50 ppm to 0.5% P, As, Sb, or Ge, those doped with 10 ppm to 0.5% As, and those microdoped with 1 ppm to 100 ppm Cl, Br, or I. In particular, amorphous selenium containing about 10 ppm to 200 ppm of As, amorphous selenium containing about 0.2% to 1% As and also 5 ppm to 100 ppm Cl, and amorphous selenium containing about 0.001 ppm to 1 ppm alkali metal can be advantageously used. 
     The photoconductive layer  546  for reading can have any thickness, provided that the reading light can be sufficiently absorbed and an electric field created by electric charges accumulated in the charge accumulating layer  544  can move the electric charges that have been excited by light. The preferred thickness is from about 1 μm to 30 μm. 
     Electrode Interface Layer 
     The electrode interface layer  548  is provided between the photoconductive layer  542  for recording and the upper electrode  518  or between the photoconductive layer  546  for reading and the lower electrode  520 . From the standpoint of preventing crystallization, amorphous selenium having added thereto As within a range of 1% to 20%, amorphous selenium having added thereto S, Te, P, Sb, or Ge within a range of 1% to 10%, and amorphous selenium having added thereto the above-described elements and other elements are preferred. 
     Furthermore, As 2 S 3  or As 2 Se 3 , which have a higher crystallization temperature, can be also advantageously used. Furthermore, with the object of preventing charge injection from the electrode layers, in addition to the additive elements, alkali metals such as Li, Na, K, Rb, and Cs and molecules such as LiF, NaF, KF, RbF, CsF, LiCl, NaCl, KCl, RbF, CsF, CsCl, and CsBr are desirably doped within a range of 10 ppm to 5000 ppm in particular in order to prevent the injection of holes. Conversely, halogen elements such as Cl, I, and Br and molecules such as In 2 O 3  are desirably doped within a range of 10 ppm to 5000 ppm in order to prevent the injection of electrons. The thickness of the interface layer can be set between 0.05 μm to 1 μm so as to attain sufficiently the above-described objects. 
     The above-described electrode interface layer  548 , photoconductive layer  546  for reading, charge accumulating layer  544 , and photoconductive layer  542  for recording are laminated on the substrate in a vacuum tank with a degree of vacuum of from 10 −3  to 10 −7  Torr by holding the substrate at a temperature equal to or higher than 25° C. and equal to or lower than 70° C., heating a boat or crucible having the aforementioned metals introduced therein by resistance heating or electron beam, and evaporating or sublimating the alloys and compounds. 
     When the evaporation temperatures of the alloys and compounds differ significantly from each other, it is preferred that a plurality of boats corresponding to a plurality to vapor deposition sources be heated simultaneously and controlled individually and that the concentration of additives and concentration of dopants be controlled. For example, an As-doped (10%) layer of amorphous selenium doped with 5000 ppm LiF can be formed by introducing As 2 Se 3 , amorphous selenium, and LiF in respective boats, heating the boat containing As 2 Se 3  to 340° C., the boat containing amorphous selenium (a-Se) to 240° C., and the boat containing LiF to 800° C., and opening and closing shutters of each boat. 
     Underlayer 
     The underlayer  550  can be provided between the photoconductive layer  546  for reading and the lower electrode (charge collecting electrode)  520 . When the electrode interface layer (crystallization preventing layer (A layer))  548  is present, the underlayer is desirably provided between the electrode interface layer  548  and the lower electrode  520 . From the standpoint of reducing a dark current and a leak current, it is preferred that the underlayer  550  have a rectification property. When a positive bias is applied to the upper electrode  518 , the underlayer desirably has an electron blocking ability, and when a negative bias is applied, the underlayer desirably has a hole blocking ability. 
     A resistivity of the underlayer is desirably equal to or higher than 10 8  Ωcm and a thickness thereof is desirably 0.01 μm to 10 μm. A layer having a composition such as Sb 2 S 3 , SbTe, ZnTe, CdTe, SbS, AsSe, and As 2 S 3  or an organic polymer layer is preferred as the layer having an electron blocking ability, that is, an electron injection blocking layer. A film in which NPD and TPD are mixed with a polymer having a hole transfer ability such as PVK or an insulating polymer such as a polycarbonate, polystyrene, a polyimide, and a polycycloolefin can be advantageously used as the organic polymer layer. 
     A film such as CdS and CeO 2  or an organic polymer layer is preferred as the layer having a hole blocking ability, that is, a hole injection blocking layer. A film obtained by mixing a carbon cluster such as C60 (fullerene) or C70 with an insulating polymer such as a polycarbonate, polystyrene, a polyimide, and a polycycloolefin can be advantageously used as the organic polymer layer. 
     A thin insulating polymer layer can be also advantageously used. For example, parylene, a polycarbonate, PVA, PVP, PVB, a polyester resin, and an acrylic resin such as polymethyl methacrylate is preferred as the insulating polymer layer. The layer thickness in this case is desirably equal to or less than 2 μm, more desirably equal to or less than 0.5 μm. 
     Overlayer 
     The overlayer  552  can be provided between the photoconductive layer  542  for recording and the upper electrode (voltage application electrode)  518 . When the electrode interface layer (crystallization preventing layer (C layer))  548  is present, the overlayer is desirably provided between the electrode interface layer  548  and the upper electrode  518 . From the standpoint of reducing a dark current and a leak current, it is preferred that the overlayer  552  have a rectification property. 
     When a positive bias is applied to the upper electrode  518 , the overlayer desirably has a hole blocking ability, and when a negative bias is applied, the overlayer desirably has an electron blocking ability. A resistivity of the overlayer is desirably equal to or higher than 10 8  Ωcm and a thickness thereof is desirably 0.01 μm to 10 μm. 
     An organic polymer layer is preferred as the layer having an electron blocking ability, that is, an electron injection blocking layer. A film in which NPD and TPD are mixed with a polymer having a hole transfer ability such as PVK or an insulating polymer such as a polycarbonate, polystyrene, a polyimide, and a polycycloolefin can be advantageously used as the organic polymer layer. 
     An organic polymer layer is preferred as the layer having a hole blocking ability, that is, a hole injection blocking layer. A film in which a hole blocking material is mixed with an insulating polymer such as a polycarbonate, polystyrene, a polyimide, and a polycycloolefin can be advantageously used as the organic polymer layer. 
     At least one from among the hole blocking materials contained in the hole injection blocking layer  402  is desirably of at least one kind selected from carbon clusters or derivatives thereof. The carbon cluster is desirably of at least one kind selected from fullerene C60, fullerene C70, fullerene oxide, and derivatives thereof. 
     A thin insulating polymer layer can be also advantageously used. For example, parylene, a polycarbonate, PVA, PVP, PVB, a polyester resin, and an acrylic resin such as polymethyl methacrylate is preferred as the insulating polymer layer. The layer thickness in this case is desirably equal to or less than 2 μm, more desirably equal to or less than 0.5 μm. 
     The upper electrode  518  and a surface protective layer  554  formed on the surface of the upper electrode  518  will be explained below. 
     Upper Electrode 
     A thin metal film is desirably used as the upper electrode  518  formed on the upper surface of the photoconductive layer  542  for recording. Examples of materials suitable for forming the upper electrode include metals such as Au, Ni, Cr, Pt, Ti, Al, Cu, Pd, Ag, Mg, a MgAg 3 to 20% alloy, a Mg—Ag intermetallic compound, a MgCu 3 to 20% alloy, and a Mg—Cu intermetallic compound. 
     It is especially preferred that Au, Pt, or a Mg—Ag intermetallic compound be used. for example, when Au is used, the thickness is desirably equal to or greater than 15 nm and equal to or less than 200 nm, more desirably equal to or greater than 30 nm and equal to or less than 100 nm. For example, when a MgAg 3 to 20% alloy is used, it is more preferred that the thickness be equal to or greater than 100 nm and equal to or less than 400 nm. 
     Any method of producing the upper electrode can be used, but the preferred method is vapor deposition employing a resistance heating system. For example, a metal lump is melted in a boat by using a resistance heating system, a shutter is then opened and vapor deposition is performed for 15 sec, followed by cooling. The upper electrode is formed by repeating the above-described operation a plurality of times till a resistance value is sufficiently reduced. 
     Surface Protective Layer 
     In order to form a latent image in a radiation device by irradiation with radiation, a high voltage of several kilovolts is applied to the upper electrode  518 . Where the upper electrode  518  is exposed to the atmosphere, a surface charge occurs and there is a possibility of subjecting the object of imaging to an electric shock. In order to prevent the surface discharge on the upper electrode  518 , an insulating treatment is performed by forming the surface protective layer  554  on the upper surface of the electrode. 
     The insulating treatment has to produce a structure that completely prevents the electrode surface from contact with the atmosphere, this structure tightly covering the surface with an insulator. This insulator has to have an electric breakdown resistance that exceeds the applied potential. Furthermore, for the radiation detection device to maintain its functionality, the insulator has to be a member that does inhibit the penetration of radiation. Vapor deposition or solvent coating of an insulating polymer are the preferred methods and material ensuring the required high covering ability, insulation breakdown resistance, and radiation transmissivity. 
     More specifically, a method can be used by which an epoxy resin curable at normal temperature, a polycarbonate resin, a polyvinyl butyral resin, a polyvinyl alcohol resin, an acrylic resin, or a polyparaxylylene derivative are coated by a CVD method. Among them, forming a film of an epoxy resin curable at normal temperature or polyparaxylylene by a CVD method is preferred, and a process for forming a film of a polyparaxylylene derivative by a CVD method is especially preferred. The film thickness is desirably equal to or greater than 10 μm and equal to or less than 1000 μm, more desirably equal to or greater than 20 μm and equal to or less than 100 μm. 
     Because a polyparaxylylene film can be formed at room temperature, it is possible to obtain an insulating film that does not provide thermal stresses to the object of coating and has an extremely high step coverability. However, because such a film is chemically extremely stable, adhesion thereof to the coating object is most often unsatisfactory. A physical treatment such as a treatment with a coupling agent, corona discharge, plasma treatment, ozone cleaning, acid treatment, and surface roughening or a chemical treatment are generally known and can be used for treating the coating object prior to forming a polyparaxylylene film in order to improve adhesion to the coating object. A method of improving adhesion to the coating object is preferred by which a silane coupling agent or a silane coupling agent diluted, if necessary, with an alcohol is coated at least on a portion in which the adhesion to the coating object is wished to be increased and a polyparaxylylene film is then formed. 
     Furthermore, damp proofing is desirably implemented to prevent the radiation detection device from deteriorating with time. More specifically, a structure covered with a damp-proofing material is obtained. A sufficient function cannot be obtained with a resin alone, such as the above-described insulating polymers, and a configuration having at least an inorganic material layer such as glass or aluminum laminate film can be effectively used as the damp-proofing material. Because glass attenuates radiation transmission, a thin aluminum laminate film is preferred as the damp-proofing member. For example, a laminate of PET (12 μm)/rolled aluminum (9 μm)/nylon (15 μm) is an aluminum laminate film that is generally used as a damp-proofing packaging material. 
     The aluminum thickness is desirably equal to or more than 5 μm and equal to or less than 30 μm. The thickness of each of the PET and nylon located above and below the aluminum is equal to or greater than 10 μm and equal to or less than 100 μm. Such a film has an X ray attenuation of about 1% and is optimum as a member demonstrating both the damp-proofing effect and X ray transmission. 
     For example, as illustrated in  FIG. 28 , the entire surface of a radiation detection device subjected to insulating treatment with a polyparaxylylene  554 A is covered with a damp-proofing film  554 B, and the outer periphery of the damp-proofing film  554 B is bonded and fixed to the substrate with an adhesive outside the radiation detection device region. As a result, a configuration is obtained in which the radiation detection device is sealed with the damp-proofing film  554 B. 
     Because the polyparaxylylene  554 A is chemically extremely stable during such bonding and fixing, bonding ability thereof to other members attained with an adhesive is generally poor. However, the bonding ability can be improved by performing light irradiation treatment with ultraviolet radiation prior to bonding. The necessary irradiation time is appropriately adjusted to an optimum value based on the wavelength and power of the ultraviolet radiation source used, but a low-pressure mercury lamp with a power of 1 W to 50 W is preferred, and light irradiation is desirably carried out for 1 min to 30 min. 
     The radiation detection device of the present embodiment uses amorphous selenium and it is possible that at a high temperature equal to or higher than 40° C., amorphous selenium will crystallize and a latent image formation function will not be obtained. Therefore, heating is unsuitable in adhesive processing. Accordingly, an adhesive curable at room temperature is preferred, and a two-liquid mixed epoxy adhesive curable at room temperature that has a high bonding strength is an optimum adhesive. This epoxy adhesive is applied on the outer periphery of the radiation detection device and a damp-proofing film  554 B is covered. The bonding portion is uniformly pressed and fixed from the upper surface of the damp-proofing film  554 B and curing is performed by allowing the joint to stay for 12 hr or longer in this state in an environment at room temperature. The pressure is released after the adhesive is cured and a sealed structure is obtained. 
     Supplementary explanation of the sealing structure member will be given below. When the radiation detection device is used for mammography, image detection at a low dose is preferred to reduce exposure during X ray imaging. In order to detect shadow variations in low-dose irradiation, it is desirable to increase X ray transmissivity of members other than the object of examination (mamma) in the path from the radiation source to the device, thereby making it possible to obtain a clear image. 
     An example of the preferred protective layer and sealing structure is illustrated in  FIG. 28 , but such a configuration is not limiting. By forming a protective film, the humidity environment of the device is desirably maintained at a level of equal to or lower than 30%, more desirably equal to or lower than 10%. 
     Charge Take-Out Amplifier 
     In the present embodiment, the electric charges are amplified by an amplifier and then AD converted.  FIG. 29  is a block diagram illustrating the configuration of the charge take-out amplifier and a connection mode thereof with an image processing device  150  disposed outside the radiation detection substrate  500 . 
     A charge amplifier IC  511  serving as the charge take-out amplifier is provided with a large number of charge amplifiers  633   a  and sample-and-hold units (S/H)  633   b  connected to respective elements  615   a  of the radiation detection substrate  500  and also a multiplexer  633   c  that multiplexes signals from the sample holders  633   b.    
     An electric circuit flowing from the lower electrode is converted into voltage by each charge amplifier  633   a , the voltage is sampled and held at a predetermined timing by the sample-and-hold units  633   b , and the sampled and held voltage corresponding to each element  615   a  is successively outputted from the multiplexer  633   c  so as to be changed into an arrangement sequence of elements  615   a  (corresponds to part of the main scanning). 
     Signals successively outputted from the multiplexer  633   c  are inputted in the multiplexer  631   c  provided on the printed circuit board  631  and a voltage corresponding to each element  615   a  is successively outputted from the multiplexer  631   c  so as to be converted into an arrangement sequence of elements  615   a.    
     Signals successively outputted from the multiplexer  631   c  are converted into digital signals by an A/D conversion unit  631   a , and the digital signals are stored in the memory  631   b.  Image signals stored in the memory  631   b  are sent via a signal cable to an external image processing unit  150 , an appropriate image processing is performed in the image processing unit  150 , and the processed image is uploaded together with pick-up information to a network  151  and sent to a server or a printer. 
     Image Acquisition Sequence 
     An image formation sequence of the present image recording and reading system is basically composed of a process of irradiating with a recording light (or X rays) under applied high voltage and accumulating latent image charges and a process of irradiating with a reading light and reading the latent image charges after completion of high-voltage application. A method of scanning a line light source  301  in the electrode direction (see  FIG. 30 ) as a reading light L is optimum, but other methods can be also used. 
     If necessary, a process of completely erasing the residual latent image charges can be included. This erasure process is carried out by irradiating the entire surface of the panel with an erasure light. It is possible to irradiate the entire surface once or scan a line light or spot line over the entire surface. The erasure process is carried out after the reading process and/or before the latent image accumulation process. When the erasure light is irradiated, the erasing efficiency can be increased by combining high-voltage application with the irradiation. Furthermore, electric charges (dark current charges) created by a dark current generated during high-voltage application can be erased by performing “pre-exposure” after the high-voltage application, but before the irradiation with recording light. 
     It is also known that various charges can be accumulated for a variety of other reasons on electrostatic recording bodies prior to irradiation with recording light. It is desirable that these residual signals be reduced by correction in order to prevent them from adversely affecting image information signals that are successively outputted as residual image development. 
     A method in which a residual image reading process is added to the above-described image recording and reading processes is effective as a method of correcting the residual image signals. The residual image reading process is carried out by performing the high-voltage application without irradiation with a recording light and then reading the “residual image”. The residual image signal can be corrected by subjecting the “residual image” signals to appropriate processing and subtracting them from “recorded images”. The residual image reading process is carried out before the image recording and reading process or after it. Furthermore, an appropriate erasure process can be combined before and/or after the residual image reading process. 
     In the radiation detection substrate  500  serving as a radiation detector of an optical reading system, the upper electrode  518  corresponds to the first electrode in accordance with the present invention, the radiation detection layer  522  having the photoconductive layer  542  for recording corresponds to the photoconductive layer in accordance with the present invention, the lower electrode  520  corresponds to the second electrode in accordance with the present invention, the TCP connection portion  530  corresponds to the take-out electrode in accordance with the present invention, and the overlayer  552  corresponds to the organic polymer layer in accordance with the present invention. 
     In the radiation detection substrate  500  of an optical reading system, the overlayer  552  can be configured in the below-described manner as in the above-described radiation detector  400 . 
     The outer edge portion of the overlayer  552  serving as an organic polymer layer, that is a circumferential edge serving as a boundary with other layers, is located in a predetermined position, thereby producing a configuration in which the overlayer  552  is formed in a predetermined range and covers the predetermined range. 
     In the present embodiment, the outer edge portion of the overlayer  552  is positioned between the TCP connection portion  530  and the region end GI of the image information acquisition region G in which image information is acquired within a region irradiated with radiation carrying image information. The range represented by arrow A in  FIG. 31A  is a range between the TCP connection portion  530  and the region end G 1  of the image information acquisition region G 
     In the preferred configuration, the outer edge portion of the overlayer  552  of the present embodiment is located outside the image information acquisition region G and within a region having a film thickness equal to or greater than 10% the average film thickness of the flat portion of the radiation detection layer  522 . The average film thickness of the flat portion of the radiation detection layer  522  is determined by measuring a film thickness in any nine points within a region of the image information acquisition region G of the radiation detection layer  522  and finding an average film thickness for these nine points. The film thickness is measured by observing the cross section of the film under a microscope with a magnification factor of 100. 
     A range represented by arrow B in  FIG. 31A  is outside the image information acquisition region G and within a region having a film thickness equal to or greater than 10% the average film thickness of the flat portion of the radiation detection layer  522 . 
     In even more preferred configuration, the outer edge portion of the overlayer  552  of the present embodiment is located outside the upper electrode  518  and within a region having a film thickness equal to or greater than 10% the average film thickness of the flat portion of the radiation detection layer  522 . 
     A range represented by arrow C in  FIG. 31A  is outside the upper electrode  518  and within a region having a film thickness equal to or greater than 10% the average film thickness of the flat portion of the radiation detection layer  522 . 
     In even more preferred configuration, the outer edge portion of the overlayer  552  of the present embodiment is located outside the upper electrode  518  and within a region in which a gradient of an end portion bevel of the radiation detection layer  522  is equal to or less than 50%. 
     The outer edge portion of the overlayer  552  is positioned within a region with a gradient of equal to or less than 50% in the end portion bevel of the radiation detection layer  522  in which the gradient gradually increases from the flat portion to the outer edge, that is, within a range in which the gradient is more gradual than a gradient of 50%. The gradient of 50% is a gradient formed by an inclined side in a rectangular triangle configured by a side along the film thickness direction of the radiation detection layer  522 , a side perpendicular to this side, and the inclined side, as illustrated in  FIG. 31B , in which where the length of the side along the film thickness direction of the radiation detection layer  522  is taken as 1, the length of the side perpendicular to this side is 2. The gradient is measured by observing the cross section under a microscope with a magnification of 100. 
     A range represented by arrow D in  FIG. 31A  is outside the upper electrode  518  and within a region in which the gradient of the end portion bevel of the radiation detection layer  522  is equal to or less than 50%. 
     The radiation detection layer  522  is formed in a region wider than the upper electrode  518 . Furthermore, the lower electrode  520  is formed in a region wider than the image information acquisition region G. 
     The present invention is not limited to the above-described embodiments, and various changes, variations, and modifications, can be made. 
     It should be understood that there is no intention to limit the invention to the specific forms disclosed, but on the contrary, the invention is to cover all modifications, alternate constructions and equivalents falling within the spirit and scope of the invention as expressed in the appended claims.