Abstract:
An acceleration sensor includes a detection element having a plurality of piezoelectric ceramic layers laminated together and a pair of retaining members that retain an end portion of the detection element in a longitudinal direction thereof at two principal surfaces of the end portion. The detection element includes electrodes between the ceramic layers and on principal surfaces. The detection element obtains a voltage or a charge generated in the detection element in response to an application of acceleration from the principal-surface electrodes and the interlayer electrodes. The piezoelectric ceramic layers are not polarized in areas between the principal-surface electrodes and the interlayer electrodes within a retaining area in which the detection element is retained by the retaining members.

Description:
BACKGROUND OF THE INVENTION 
   1. Field of the Invention 
   The present invention relates to an acceleration sensor using piezoelectric ceramics. 
   2. Description of the Related Art 
   Various acceleration sensors using piezoelectric ceramics have been suggested. An example of such an acceleration sensor includes a detection element having a plurality of piezoelectric ceramic layers laminated together and a pair of retaining members that retain an end portion of the detection element in a longitudinal direction thereof at two principal surfaces of the end portion. This acceleration sensor generates a large amount of energy, which can be expressed as ½ of the product of charge sensitivity and voltage sensitivity, and functions as a high S/N ratio sensor, that is, a high sensitivity sensor. 
     FIG. 6  shows an example of an acceleration sensor disclosed in Japanese Unexamined Patent Application Publication No. 2003-337140 and Japanese Unexamined Patent Application Publication No. 2005-164505. The acceleration sensor  1  includes a detection element  2  and a pair of retaining members  10  and  11  that retain an end portion of the detection element  2  in a longitudinal direction thereof at two principal surfaces of the end portion. The detection element  2  is obtained by integrally firing a laminate of four piezoelectric ceramic layers  2   a  to  2   d . The first layer  2   a , the second layer  2   b , the third layer  2   c , and the fourth layer  2   d  are arranged in that order from one of the principal surfaces of the detection element  2  to the other one of the principal surfaces. An interlayer electrode  3  is provided at the approximate center of the detection element  2  in the thickness direction thereof, that is, between the second layer  2   b  and the third layer  2   c . In addition, interlayer electrodes  4  and  5  are provided between the first layer  2   a  and the second layer  2   b  and between the third layer  2   c  and the fourth layer  2   d , respectively. The detection element  2  includes principal-surface electrodes  6  and  7  on the principal surfaces thereof. 
   The first layer  2   a  and the fourth layer  2   d  of the piezoelectric ceramic layers have substantially the same thickness, and the second layer  2   b  and the third layer  2   c  of the piezoelectric ceramic layers have substantially the same thickness. The thickness of the second layer  2   b  and the third layer  2   c  is greater than the thickness of the first layer  2   a  and the fourth layer  2   d . As shown by the arrows P in  FIG. 6 , the piezoelectric ceramic layers  2   a  to  2   d  are polarized in the thickness direction. The second layer  2   b  and the third layer  2   c  are polarized in the same direction, the first layer  2   a  and the second layer  2   b  are polarized in opposite directions, and the fourth layer  2   d  and the third layer  2   c  are polarized in opposite directions. 
   The end portion of the detection element  2  is retained by retaining portions  10   a  and  11   a  of the retaining members  10  and  11 , respectively. Each of the interlayer electrodes  4  and  5  extends to an end surface of the end portion at one end thereof, and is electrically connected to an external electrode  8  provided continuously on end surfaces of the retaining members  10  and  11  and the end surface of the detection element  2 . Each of the interlayer electrodes  4  and  5  extends to a location spaced part from a free end of the detection element  2  by a predetermined distance at the other end thereof. 
   The interlayer electrode  3  extends to a location corresponding to inner edges of the retaining portions  10   a  and  11   a  of the retaining members  10  and  11  at one end thereof, and to the free end of the detection element  2  at the other end thereof. Each of the principal-surface electrodes  6  and  7  extends to an intermediate location of the portion clamped between the retaining portions  10   a  and  11   a  of the retaining members  10  and  11  at one end thereof, and to the free end of the detection element  2  at the other end thereof. Extraction electrodes  12  and  13  are provided on inner surfaces of the retaining portions  10   a  and  11   a , respectively, and are electrically connected to the principal-surface electrodes  6  and  7 , respectively, with anisotropic conductive adhesive  14 . As mentioned above, each of the principal-surface electrodes  6  and  7  extends to an intermediate location of the retaining portions  10   a  and  11   a  of the retaining members  10  and  11  at one end thereof. The reason for this is to provide sufficient opposing areas between the principal-surface electrodes  6  and  7  and the extraction electrodes  12  and  13  provided on the inner surfaces of the retaining portions  10   a  and  11   a , respectively, thereby increasing the connection areas. The extraction electrodes  12  and  13  and the principal-surface electrodes  6  and  7  are not conductively connected to the external electrode  8 . The extraction electrodes  12  and  13  extend continuously from the inner surfaces of the retaining portions  10   a  and  11   a  to inner surfaces of portions of the retaining members  10  and  11  at an end opposed to the retaining portions  10   a  and  11   a . The extraction electrodes  12  and  13  are electrically connected to an external electrode  9  provided on end surfaces of the retaining members  10  and  11  and an end surface of an end member  15  at the end opposite to the retaining portions  10   a  and  11   a.    
   The detection element  2  includes a connection electrode  18  formed by vapor deposition or sputtering on a side surface at the free end thereof. The connection electrode  18  connects the interlayer electrode  3  and the principal-surface electrodes  6  and  7  to one another. The connection electrode  18  is provided in an area in which the interlayer electrodes  4  and  5  do not extend, and therefore is not connected to the interlayer electrodes  4  and  5 . Instead of providing the connection electrode  18  on the side surface of the detection element  2 , the connection electrode  18  may also be provided on an end surface of the detection element  2  at the free end thereof. When the connection electrode  18  is provided, an electrode  19  is also provided on side surfaces of the retaining members  10  and  11  and the end member  15 . However, the electrode  19  may also be omitted. 
   As described above, the interlayer electrodes  4  and  5  are connected to the external electrode  8 . In addition, the interlayer electrode  3  and the principal-surface electrodes  6  and  7  are connected to one another via the connection electrode  18 , and are also connected to the external electrode  9  via the extraction electrodes  12  and  13  provided on the inner surfaces of the retaining members  10  and  11 , respectively. Thus, as shown in  FIG. 7 , the four piezoelectric ceramic layers  2   a  to  2   d  are electrically connected in parallel between the external electrodes  8  and  9 . 
   Referring to  FIG. 6 , when an acceleration G is applied in the direction shown by the arrow, the detection element  2  is deflected by inertia in a direction opposite to the direction in which the acceleration is applied. Accordingly, a compressive stress is applied to an upper half of the detection element  2  and a tensile stress is applied to a lower half of the detection element  2 . Therefore, positive charges are generated in the interlayer electrode  3  and the principal-surface electrodes  6  and  7 , and negative charges are generated in the interlayer electrodes  4  and  5 . As a result, the negative charges are obtained from the external electrode  8  that is conductively connected to the interlayer electrodes  4  and  5 , and the positive charges are obtained from the external electrode  9  that is conductively connected to the interlayer electrode  3  and the principal-surface electrodes  6  and  7 . 
   In the acceleration sensor having the above-described structure, when a temperature change is externally applied, heat is transmitted to the detection element  2  through the retaining members  10  and  11 . Accordingly, charges shown by the positive and negative signs in  FIG. 8  are generated in the piezoelectric ceramic layers  2   a  to  2   d  by the pyroelectric effect. If the temperature change is evenly applied to the piezoelectric ceramic layers  2   a  to  2   d , the charges generated by the pyroelectric effect cancel each other between the first layer  2   a  and the fourth layer  2   d  and between the second layer  2   b  and the third layer  2   c . Therefore, no output is obtained. However, if the temperature is increased locally, different temperature changes occur in the piezoelectric ceramic layers  2   a  to  2   d . Therefore, the charges generated by the pyroelectric effect do not cancel each other out between the first layer  2   a  and the fourth layer  2   d  or between the second layer  2   b  and the third layer  2   c . As a result, an unwanted output (thermal fluctuation noise) is output from the acceleration sensor  1 . For example, if the temperature of the retaining member  10  is greater than that of the retaining member  11 , heat is transmitted from the retaining portion  10   a  of the retaining member  10  to the upper surface of the end portion of the detection element  2 . Therefore, a temperature difference is generated between the upper surface and the lower surface of the detection element  2 , and an unwanted output is generated by the pyroelectric effect. 
   The cause of the generation of the unwanted output by the pyroelectric effect will be described in more detail. The piezoelectric ceramic layers  2   a  to  2   d  included in the detection element  2  are polarized in the directions shown by the arrows P. As shown by the knurling pattern in  FIG. 8 , polarized areas of the piezoelectric ceramic layers  2   a  to  2   d  correspond to areas of the piezoelectric ceramic layers between the electrodes facing one another. This is because the interlayer electrodes  3 ,  4 , and  5  and the principal-surface electrodes  6  and  7  are also used as polarizing electrodes. In this structure, pyroelectric charges are generated in polarized areas (denoted by S in  FIG. 8 ) of the first layer  2   a  and the fourth layer  2   d  within a retaining area where the end portion is retained by the retaining members  10  and  11 . This is because no pyroelectric charge is generated in non-polarized areas or in areas between electrodes having the same potential. More specifically, portions of the principal-surface electrodes  6  and  7  extend into the areas where the portions of the principal-surface electrodes  6  and  7  face the retaining portions  10   a  and  11   a  of the retaining members  10  and  11 , respectively. Therefore, pyroelectric charges are generated in the areas S between the extending portions of the principal-surface electrodes  6  and  7  and the interlayer electrodes  4  and  5 , and are extracted as an unwanted output. 
   SUMMARY OF THE INVENTION 
   To overcome the problems described above, preferred embodiments of the present invention provide an acceleration sensor that reduces an unwanted output generated by the pyroelectric effect in a retaining area of retaining members. 
   An acceleration sensor according to a preferred embodiment of the present invention includes a detection element and retaining members retaining an end portion of the detection element in a longitudinal direction thereof at two principal surfaces of the end portion, the detection element having a plurality of piezoelectric ceramic layers laminated together. The detection element includes at least one interlayer electrodes interposed between the piezoelectric ceramic layers and principal-surface electrodes on the principal surfaces. The acceleration sensor obtains a voltage or a charge from the principal-surface electrodes and the interlayer electrode, the voltage or the charge being generated in the detection element in response to an application of acceleration. The principal-surface electrodes and the interlayer electrode that is not electrically connected to the principal-surface electrodes extend into a retaining area in which the detection element is retained by the retaining members. The retaining members include extraction electrodes on inner surfaces thereof. At least a portion of each principal-surface electrode extending into the retaining area of the retaining members and at least a portion of the extraction electrode on the inner surface of the corresponding retaining member face each other and are electrically connected to each other. Within the retaining area in which the detection element is retained by the retaining members, the piezoelectric ceramic layers are not polarized in areas between the principal-surface electrodes and the interlayer electrode that is not electrically connected to the principal-surface electrodes. 
   In the acceleration sensor according to this preferred embodiment of the present invention, when, for example, the temperature of one of the retaining members becomes greater than the other one of the retaining members, heat is transmitted from a retaining portion of one of the retaining members to the upper surface of the end portion of the detection element. Therefore, a temperature difference occurs between the upper surface and the lower surface of the detection element, and there is a risk that an unwanted output will be generated by the pyroelectric effect. However, in preferred embodiments of the present invention, within the retaining area in which the detection element is retained by the retaining members, the piezoelectric ceramic layers are not polarized in areas between the principal-surface electrodes and the interlayer electrode that is not electrically connected to the principal-surface electrodes. Therefore, no pyroelectric charge is generated and no unwanted output is obtained from the portion retained by the retaining members. 
   There is a possibility that heat applied to the end portion of the detection element will be transmitted to an acceleration detecting portion (portion that is not retained by the retaining members) of the detection element and cause thermal fluctuation noise. However, since the acceleration detecting portion of the detection element is exposed, the temperature change occurs substantially evenly between the ceramic layers, and the generated pyroelectric charges will be canceled. 
   In a preferred embodiment of the present invention, the detection element includes first to fourth piezoelectric ceramic layers in order from one principal surface to the other principal surface. The interlayer electrode at the approximate center of the detection element in the thickness direction thereof is electrically connected to both of the principal-surface electrodes, and at least one of the principal-surface electrodes extends to a location spaced apart from an end surface on the end portion retained by the retaining members. The at least one of the principal-surface electrodes is electrically connected, with anisotropic conductive adhesive, to the corresponding extraction electrode that is provided on the inner surface of the retaining member and that faces the at least one of the principal-surface electrodes. The interlayer electrode between the first and second piezoelectric ceramic layers of the detection element and the interlayer electrode between the third and fourth piezoelectric ceramic layers of the detection element are electrically connected to each other and extend to the end surface of the end portion retained by the retaining member. In this case, the detection element has a four-layer laminate structure including four piezoelectric ceramic layers that are connected in parallel to extract the charge generated in each layer in response to the application of acceleration. Since the voltage or the charge generated in response to the application of acceleration can be reliably extracted to different portions of the retaining member, the acceleration sensor can be easily configured as a surface-mount device. In addition, at least one of the principal-surface electrodes on the detection element is conductively connected to the extraction electrode on the corresponding retaining member with the anisotropic conductive adhesive. Therefore, even when the distance from the principal-surface electrodes or the extraction electrodes to the end surfaces of the retaining members is relatively small, insulation from one of the external electrodes is ensured. Therefore, the size of the acceleration sensor can be reduced. 
   In another preferred embodiment of the present invention, the first and fourth piezoelectric ceramic layers of the detection element have substantially the same thickness, the second and third piezoelectric ceramic layers of the detection element have substantially the same thickness, and the thickness of the second piezoelectric ceramic layer is greater than the thickness of the first piezoelectric ceramic layer. By setting the thickness of the two inner layers greater than that of the two outer layers and making the potentials generated in the layers substantially equal to one another, increased energy can be generated. 
   In another preferred embodiment of the present invention, the detection element includes first and second piezoelectric ceramic layers in order from one principal surface to the other principal surface. Both of the principal-surface electrodes of the detection element extend to a location spaced apart from an end surface on the end portion retained by the retaining members. The principal-surface electrodes are electrically connected, with anisotropic conductive adhesive, to the corresponding extraction electrodes that are provided on the inner surfaces of the retaining members that face the principal-surface electrodes. The interlayer electrode of the detection element extends to the end surface of the end portion retained by the retaining members. This acceleration sensor has a two-layer structure, and the structure thereof is simplified. The two piezoelectric ceramic layers are connected in parallel. 
   In another preferred embodiment of the present invention, portions of the principal-surface electrodes in the retaining area of the retaining members are not provided at the time when the piezoelectric ceramic layers are polarized but are arranged so as to be electrically connected to portions of the principal-surface electrodes outside the retaining area of the retaining members after the piezoelectric ceramic layers are polarized using the portions of the principal-surface electrodes outside the retaining area of the retaining members. In this case, the end portion of the detection element retained by the retaining members can be easily maintained in a non-polarized state. In addition, the principal-surface electrodes can be easily electrically connected to the extraction electrodes on the inner surfaces of the retaining members. 
   According to preferred embodiments of the present invention, within the retaining area in which the detection element is retained by the retaining members, the piezoelectric ceramic layers are not polarized in areas between the principal-surface electrodes and the interlayer electrodes that are not electrically connected to the principal-surface electrodes. Therefore, no pyroelectric charge is generated by a temperature change and no unwanted output is obtained from the portion retained by the retaining members. 
   Other features, elements, steps, characteristics and advantages of the present invention will become more apparent from the following detailed description of preferred embodiments of the present invention with reference to the attached drawings. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
       FIG. 1  is a front view of an acceleration sensor according to a first preferred embodiment of the present invention. 
       FIG. 2  is an enlarged view of a portion of the acceleration sensor shown in  FIG. 1 . 
       FIG. 3  is a temperature distribution diagram obtained when a temperature change is applied to the acceleration sensor shown in  FIG. 1 . 
       FIG. 4  shows a temperature distribution at the approximate center of each piezoelectric ceramic layer when a temperature change is applied under the same conditions as those in  FIG. 3 . 
       FIG. 5  is a front view of an acceleration sensor according to a second preferred embodiment of the present invention. 
       FIG. 6  is a front view showing an example of a known acceleration sensor. 
       FIG. 7  is a circuit diagram of the acceleration sensor shown in  FIG. 6 . 
       FIG. 8  illustrates charges generated by the pyroelectric effect in the acceleration sensor shown in  FIG. 6 . 
   

   DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS 
   Preferred embodiments of the present invention will be described below with reference to the drawings. 
   First Preferred Embodiment 
     FIGS. 1 and 2  show an acceleration sensor according to a first preferred embodiment of the present invention. The basic structure of this acceleration sensor  1 A is similar to the known acceleration sensor  1  shown in  FIG. 6 . Therefore, components similar to those shown in  FIG. 6  are denoted by the same reference numerals and redundant descriptions thereof are omitted. 
   In the acceleration sensor  1 A according to the first preferred embodiment of the present invention, within a retaining area in which a detection element  2  is retained by retaining members  10  and  11 , piezoelectric ceramic layers  2   a  to  2   d  are not polarized in areas (denoted by S in  FIGS. 1 and 2 ) between electrodes that face each other across the piezoelectric ceramic layers  2   a  to  2   d  and are not connected to each other. In other words, as shown by the knurling pattern in  FIG. 1 , the piezoelectric ceramic layers are polarized only in the areas between the electrodes  3  to  7  with different potentials and outside the retaining area in which the detection element  2  is retained by the retaining members  10  and  11 . Therefore, the first layer  2   a  is not polarized in the retaining area of the retaining members  10  and  11 , and the fourth layer  2   d  is not polarized in the retaining area of the retaining members  10  and  11 . 
   The second layer  2   b  and the third layer  2   c  may be polarized in the retaining area of the retaining members  10  and  11  because interlayer electrodes  4  and  5  are connected to each other by an external electrode  8 . In addition, it is not necessary that the first layer  2   a  and the fourth layer  2   d  be non-polarized in the entire retaining area of the retaining members  10  and  11 . For example, electrodes  16  and  17  (see  FIG. 2 ) connected to the interlayer electrodes  4  and  5  may preferably be provided on the outer surfaces of the first layer  2   a  and the fourth layer  2   d , respectively. In such an arrangement, within the retaining area of the retaining members  10  and  11 , the first layer  2   a  and the fourth layer  2   d  may be polarized in areas between the electrodes  16  and  17  and the interlayer electrodes  4  and  5 . 
   To keep the first layer  2   a  and the fourth layer  2   d  non-polarized in the retaining area of the retaining members  10  and  11 , as shown in  FIG. 2 , the principal-surface electrodes  6  and  7  are respectively defined by detection electrodes  6   a  and  7   a  and extraction electrodes  6   b  and  7   b . The detection electrode  6   a  is used to polarize the first layer  2   a  located between the detection electrode  6   a  and the interlayer electrode  4 . After the first layer  2   a  is polarized, the extraction electrode  6   b  is arranged so as to overlap the detection electrode  6   a . Similarly, the detection electrode  7   a  is used to polarize the fourth layer  2   d  located between the detection electrode  7   a  and the interlayer electrode  5 . After the fourth layer  2   d  is polarized, the extraction electrode  7   b  is arranged so as to overlap the detection electrode  7   a.    
   The method for keeping the first layer  2   a  and the fourth layer  2   d  non-polarized in the retaining area of the retaining members  10  and  11  is not limited to the method shown in  FIG. 2 . For example, the detection electrodes  6   a  and  7   a  may preferably be provided separately from the extraction electrodes in advance. Then, after the polarization process using the detection electrodes  6   a  and  7   a , connection electrodes may be arranged to connect the extraction electrodes to the corresponding detection electrodes  6   a  and  7   a.    
   When a temperature change is applied to the acceleration sensor  1 A, the temperature change is transmitted to the detection element  2  through the retaining members  10  and  11 . However, no charge is generated by the pyroelectric effect because the piezoelectric ceramic layers  2   a  and  2   d  are not polarized in the retaining area of the retaining members  10  and  11 . An acceleration detecting portion of the detection element  2  is not retained by the retaining members  10  and  11 . In the acceleration detecting portion, charges generated by the pyroelectric effect are canceled between the first layer  2   a  and the fourth layer  2   d  and between the second layer  2   b  and third layer  2   c  irrespective of whether or not the temperature change is evenly applied to the acceleration sensor  1 A, because the temperature change is applied evenly between the ceramic layers. As a result, no unwanted output is generated from the portion clamped between the retaining members  10  and  11  and the thermal fluctuation noise can be greatly reduced. 
   As another method of reducing the thermal fluctuation noise, the polarized areas of the detection element  2  may preferably be shifted toward the free end of the detection element  2  instead of eliminating the polarized areas of the detection element  2  from the retaining area of the retaining members  10  and  11 . However, in this case, the sensitivity is greatly reduced. If the polarized areas are eliminated only in the retaining area of the retaining members  10  and  11  as in the present preferred embodiment of the present invention, the same sensitivity as that of the known structure shown in  FIG. 6  can be obtained. In other words, according to the present preferred embodiment, the thermal fluctuation noise can be greatly reduced without reducing the sensitivity as compared to that of the known structure. 
     FIG. 3  illustrates a temperature distribution in the acceleration sensor  1 A shown in  FIG. 1 . More specifically,  FIG. 3  shows the results of a finite element method (FEM) analysis of the temperature distribution in the acceleration sensor  1 A obtained when the temperature of the acceleration sensor  1 A is maintained at about 25° C., for example, and then the acceleration sensor  1 A is heated from above in the figure at about 50° C., for example, for about one second. Here, it is assumed that the size of the acceleration sensor  1 A is about 2.0 mm×about 3.8 mm (thickness of the detection element is about 0.27 mm), the length of the retaining portions D is about 0.8 mm, and the length of the principal-surface electrodes  6  and  7  in the retaining area of the retaining members  10  and  11  S is about 0.4 mm. In  FIG. 3 , H denotes a high-temperature area (about 50° C., for example), C denotes a low-temperature area (about 25° C., for example), and M denotes an intermediate temperature area (about 37° C., for example). 
     FIG. 4  shows the temperature distribution in each of the piezoelectric ceramic layers  2   a  to  2   d  at the approximate center thereof in the thickness direction. The temperature distribution shown in  FIG. 4  is obtained under substantially the same heating condition as those of  FIG. 3 . The retaining area D of the retaining members  10  and  11  preferably corresponds to the range X of about 0 mm to about 0.8 mm, for example. As shown in  FIG. 4 , the portion of the detection element  2  that is not retained by the retaining members  10  and  11  (X&gt;about 0.8 mm) has almost no temperature variation in the thickness direction. Therefore, almost no thermal fluctuation noise is generated from the portion of the detection element  2  that is not retained by the retaining members  10  and  11 . The pyroelectric effect is affected by the temperature difference between the first layer  2   a  and the fourth layer  2   d  of the detection element  2  in the retaining area of the retaining members  10  and  11 . In this example, the temperature of the first layer  2   a  is about 42° C. and the temperature of the fourth layer  2   d  is about 35° C. 
   The table provided below shows a comparison between the thermal fluctuation noise caused in the structure of the present preferred embodiment of the present invention ( FIG. 1 ) and that caused in a comparative example ( FIG. 6 ) on the basis of the temperature distribution shown in  FIGS. 3 and 4 . As shown in Table 1, because the first layer  2   a  and the fourth layer  2   d  are not polarized in the retaining area of the retaining members, the thermal fluctuation noise generated in the structure of the present preferred embodiment is reduced to about half or less of that generated in the comparative example. 
   
     
       
             
             
             
           
         
             
               TABLE 1 
             
             
                 
             
             
               Present Invention 
               Comparative Example 
               Ratio to Comparative 
             
             
               [mGrms] 
               [mGrms] 
               Example 
             
             
                 
             
           
           
             
               62.3 
               136.3 
               46% 
             
             
                 
             
           
        
       
     
   
   Second Preferred Embodiment 
     FIG. 5  shows an acceleration sensor according to a second preferred embodiment of the present invention. Components similar to those of the first preferred embodiment are denoted by the same reference numerals, and redundant descriptions thereof are omitted. The acceleration sensor  1 B according to the present preferred embodiment includes a detection element  20  supported by retaining members  10  and  11  at one end thereof. The detection element  20  is obtained by integrally firing a laminate of two piezoelectric ceramic layers  20   a  and  20   b . An interlayer electrode  21  is provided at the approximate center of the detection element  20  in the thickness direction thereof, and principal-surface electrodes  22  and  23  are provided on upper and lower surfaces, respectively, of the detection element  20 . The two piezoelectric ceramic layers  20   a  and  20   b  are polarized in the same direction along the thickness thereof, as shown by the arrows P. 
   The interlayer electrode  21  extends from an end of the detection element  20  in which an external electrode  8  is provided to an intermediate location of the detection element  20 . In other words, an electrode gap is provided at a free end of the detection element  20 . The principal-surface electrodes  22  and  23  extend from an end portion of the detection element  20  that is retained by the retaining members  10  and  11  to the free end thereof. The principal-surface electrodes  22  and  23  are electrically connected to extraction electrodes  12  and  13  provided on the retaining members  10  and  11 , respectively, with anisotropic conductive adhesive  14 . The detection element  20  includes a connection electrode  18  provided on a side surface at the free end thereof. The connection electrode  18  connects the principal-surface electrodes  22  and  23  to each other. However, the connection electrode  18  is not conductively connected to the interlayer electrode  21 . The piezoelectric ceramic layers  20   a  and  20   b  are electrically connected in parallel. 
   In this acceleration sensor  1 B, as shown by the knurling pattern in  FIG. 5 , the piezoelectric ceramic layers  20   a  and  20   b  are polarized only in areas between the electrodes  21  and  22  and between the electrodes  21  and  23  and outside the retaining area in which the detection element  20  is retained by the retaining members  10  and  11 . In other words, within the retaining area D in which the detection element  20  is retained by the retaining members  10  and  11 , the piezoelectric ceramic layers  20   a  and  20   b  are not polarized in areas (denoted by S in  FIG. 5 ) between the electrodes  21  and  22  facing each other across the piezoelectric ceramic layer  20   a  without electrical connection and between the electrodes  21  and  23  facing each other across the piezoelectric ceramic layer  20   b  without electrical connection. Therefore, no charge is generated by the pyroelectric effect and the thermal fluctuation noise can be greatly reduced. 
   The present invention is not limited to the above-described preferred embodiments. The structure of the piezoelectric ceramic layers defining the detection element is not limited to the four-layer structure or the two-layer structure, and may also be other multilayer structures, such as a six-layer structure and an eight-layer structure, for example. In addition, the piezoelectric ceramic layers defining the detection element may be subjected to firing in an integral state, or may be laminated together after firing. 
   While preferred embodiments of the present invention have been described above, it is to be understood that variations and modifications will be apparent to those skilled in the art without departing the scope and spirit of the present invention. The scope of the present invention, therefore, is to be determined solely by the following claims.