Patent Publication Number: US-2023145220-A1

Title: Electromagnetic wave attenuator and electronic device

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS 
     This application is based upon and claims the benefit of priority from Japanese Patent Application No. 2021-182265, filed on Nov. 9, 2021; the entire contents of which are incorporated herein by reference. 
     FIELD 
     Embodiments described herein relate generally to an electromagnetic wave attenuator and an electronic device. 
     BACKGROUND 
     For example, an electromagnetic wave attenuator such as an electromagnetic shield sheet or the like has been proposed. There is an electronic device that includes the electromagnetic wave attenuator and a semiconductor element. It is desirable that the electromagnetic wave attenuator stably attenuates the electromagnetic wave. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG.  1    is a schematic cross-sectional view illustrating an electromagnetic wave attenuator according to a first embodiment; 
         FIG.  2    is a schematic cross-sectional view illustrating an electromagnetic wave attenuator according to the first embodiment; 
         FIGS.  3 A and  3 B  are graphs illustrating evaluation results of the electromagnetic wave attenuator; 
         FIGS.  4 A and  4 B  are electron microscope images of cross section of the electromagnetic wave attenuator according to the first embodiment; 
         FIG.  5    is an electron microscope image of cross section of the electromagnetic wave attenuator according to the first embodiment; 
         FIG.  6    is a graph illustrating characteristics of the electromagnetic wave attenuator; 
         FIG.  7    is a schematic cross-sectional view illustrating the electromagnetic wave attenuator according to the embodiment; 
         FIGS.  8 A to  8 D  are schematic views illustrating an electronic device according to a second embodiment; 
         FIGS.  9 A to  9 D  are schematic views illustrating parts of the electronic device according to the second embodiment; 
         FIG.  10    is a schematic cross-sectional view illustrating an electronic device according to the second embodiment; 
         FIG.  11    is a schematic cross-sectional view illustrating an electronic device according to the second embodiment; 
         FIG.  12    is a schematic cross-sectional view illustrating an electronic device according to the second embodiment; 
         FIG.  13    is a schematic cross-sectional view illustrating an electronic device according to the second embodiment; 
         FIG.  14    is a schematic cross-sectional view illustrating an electronic device according to the second embodiment; and 
         FIG.  15    is a schematic cross-sectional view illustrating an electronic device according to the second embodiment. 
     
    
    
     DETAILED DESCRIPTION 
     According to one embodiment, an electromagnetic wave attenuator includes a stacked member including a first planar portion. The first planar portion includes a first stacked body. The first stacked body includes a plurality of non-magnetic layers including Cr and Ti, and a plurality of first magnetic layers. A direction from one of the first magnetic layers to an other one of the first magnetic layers is along a first direction. One of the non-magnetic layers is between the one of the first magnetic layers and the other one of the first magnetic layers. The one of the first non-magnetic layers includes an amorphous region. The one of the first magnetic layers and the other one of the first magnetic layers include a crystal region. 
     According to another embodiment, an electronic device includes the electromagnetic wave attenuator described above, and an electronic element. 
     Various embodiments are described below with reference to the accompanying drawings. 
     The drawings are schematic and conceptual; and the relationships between the thickness and width of portions, the proportions of sizes among portions, etc., are not necessarily the same as the actual values. The dimensions and proportions may be illustrated differently among drawings, even for identical portions. 
     In the specification and drawings, components similar to those described previously or illustrated in an antecedent drawing are marked with like reference numerals, and a detailed description is omitted as appropriate. 
     First Embodiment 
       FIG.  1    is a schematic cross-sectional view illustrating an electromagnetic wave attenuator according to a first embodiment. 
     As shown in  FIG.  1   , the electromagnetic wave attenuator  10  according to the embodiment includes a stacked member  10 MA. The stacked member  10 MA includes a first planar portion  10   p.    
     The first planar portion  10   p  includes the first stacked body  10 M. The first stacked body  10 M includes multiple first magnetic layers  11  and multiple first non-magnetic layers  11 N. The multiple first non-magnetic layers  11 N include Cr and Ti. For example, the multiple first non-magnetic layers  11 N include alloys including Cr and Ti. 
     A direction from one of the multiple first magnetic layers  11  to another one of the multiple first magnetic layers  11  is along a first direction D 1 . One of the multiple first non-magnetic layers  11 N is between one of the multiple first magnetic layers  11  and another one of the multiple first magnetic layers  11 . For example, one of the multiple first magnetic layers  11  is between one of the multiple first non-magnetic layers  11 N and another one of the multiple first non-magnetic layers  11 N. 
     The first direction D 1  is defined as a Z-axis direction. One direction perpendicular to the Z-axis direction is defined as an X-axis direction. A direction perpendicular to the Z-axis direction and the X-axis direction is defined as a Y-axis direction. 
     The multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N are, for example, layered along an X-Y plane. The multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N are arranged alternately along the Z-axis direction, for example. 
     In the embodiment, one of the multiple first non-magnetic layers  11 N includes an amorphous region. One of the multiple first magnetic layers  11  and another one of the multiple first magnetic layers  11  include a crystal region. 
     With such an electromagnetic wave attenuator  10 , the electromagnetic wave attenuation characteristic can be improved. An example of the experimental results regarding the characteristics of the electromagnetic wave attenuator will be described later. 
     As shown in  FIG.  1   , the electromagnetic wave attenuator  10  may include a base body  10   s . A direction from the base body  10   s  to the first planar portion  10   p  is along the first direction D 1 . For example, the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N are alternately formed on the base body  10   s.    
     The base body  10   s  may include a resin. In one example, the base body  10   s  is a mold resin or the like. In another example, the base body  10   s  may be a resin layer or the like. The resin layer is provided on, for example, a plastic sheet. In the embodiment, the surface of the base body  10   s  may have unevenness. In this case, the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N may have an uneven shape along the uneven surface of the base body  10   s.    
     As shown in  FIG.  1   , for example, at least one of the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N may be grounded. For example, an electromagnetic wave is incident on the electromagnetic wave attenuator  10 . The electromagnetic wave incident on the electromagnetic wave attenuator  10  is attenuated by the electromagnetic wave attenuator  10 . The electromagnetic wave attenuator  10  can be used as, for example, a shield of an electromagnetic wave. 
     As shown in  FIG.  1   , one of the multiple first non-magnetic layers  11 N is in contact with one of the multiple first magnetic layers  11  and another one of the multiple first magnetic layers  11 . A thickness of one of the multiple first non-magnetic layers  11 N along the first direction D 1  is defined as a thickness t 11 N. The thickness t 11 N is, for example, not less than 1 nm and not more than 10 nm. A thickness of one of the multiple first magnetic layers  11  along the first direction D 1  is defined as a thickness t 11 . The thickness t 11  is, for example, not less than 10 nm and not more than 500 nm. 
     The multiple first magnetic layers  11  include at least one selected from the group consisting of Fe, Ni and Co. The multiple first magnetic layers  11  are, for example, soft magnetic layers. The multiple first magnetic layers  11  may further include at least one selected from the group consisting of, for example, Cu, Mo and Cr. In one example, the multiple first magnetic layers  11  are, for example, NiFeCuMo layers. 
     In the first stacked body  10 M, the number of the multiple first magnetic layers  11  may be the same as the number of the multiple first non-magnetic layers  11 N, may be 1 larger than the number of the multiple first non-magnetic layers  11 N, or may be 1 smaller than the number of the multiple first non-magnetic layers  11 N. For example, the number of the multiple first magnetic layers  11  is, for example, not less than 2 and not more than 200. The number of the multiple first non-magnetic layers  11 N is, for example, not less than 2 and not more than 200. 
     As described below, in the embodiment, the first planar portion  10   p  may include another stacked body in addition to the first stacked body  10 M. 
       FIG.  2    is a schematic cross-sectional view illustrating an electromagnetic wave attenuator according to the first embodiment. 
     As shown in  FIG.  2   , in the electromagnetic wave attenuator  10 A according to the embodiment, the first planar portion  10   p  further includes the second stacked body  20 M. The direction from the first stacked body  10 M to the second stacked body  20 M is along the first direction D 1 . The second stacked body  20 M includes multiple second magnetic layers  12  and multiple second non-magnetic layers  12 N. The multiple second non-magnetic layers  12 N include Cu. In the electromagnetic wave attenuator  10 A, the configuration of the first stacked body  10 M may be the same as the configuration of the first stacked body  10 M in the electromagnetic wave attenuator  10 . 
     A direction from one of the multiple second magnetic layers  12  to another of the multiple second magnetic layers  12  is along the first direction D 1 . One of the multiple second non-magnetic layers  12 N is between one of the multiple second magnetic layers  12  and another one of the multiple second magnetic layers  12 . For example, one of the multiple second magnetic layers  12  is between one of the multiple second non-magnetic layers  12 N and another one of the multiple second non-magnetic layers  12 N. The multiple second magnetic layers  12  and the multiple second non-magnetic layers  12 N are, for example, layered along the X-Y plane. The multiple second magnetic layers  12  and the multiple second non-magnetic layers  12 N are arranged alternately along the Z-axis direction, for example. 
     One of the multiple second non-magnetic layers  12 N is in contact with one of the multiple second magnetic layers  12  and another of the multiple second magnetic layers  12 . A thickness t 12 N of one of the multiple second non-magnetic layers  12 N along the first direction D 1  is, for example, not less than 50 nm and not more than 200 nm. A thickness t 12  of one of the multiple second magnetic layers  12  along the first direction D 1  is, for example, not less than 50 nm and not more than 200 nm. 
     The multiple second magnetic layers  12  include at least one selected from the group consisting of Fe, Ni and Co. The multiple second magnetic layers  12  are, for example, soft magnetic layers. The multiple second magnetic layers  12  may further include at least one selected from the group consisting of, for example, Cu, Mo and Cr. In one example, the multiple second magnetic layers  12  are, for example, NiFeCuMo layers. 
     In the second stacked body  20 M, the number of the multiple second magnetic layers  12  may be the same as the number of the multiple second non-magnetic layers  12 N, may be 1 larger than the number of the multiple second non-magnetic layers  12 N, or may be 1 smaller than the number of the multiple second non-magnetic layers  12 N. For example, the number of the multiple second magnetic layers  12  is, for example, not less than 2 and not more than 100. The number of the multiple second non-magnetic layers  12 N is, for example, not less than 2 and not more than 100 or less. 
     In one example, the second stacked body  20 M is provided between the base body  10   s  and the first stacked body  10 M. In the embodiment, the first stacked body  10 M may be provided between the base body  10   s  and the second stacked body  20 M. 
     In this example, the first planar portion  10   p  further includes a third stacked body  30 M. The third stacked body  30 M includes multiple third magnetic layers  13  and multiple third non-magnetic layers  13 N. The direction from one of the multiple third magnetic layers  13  to another one of the multiple third magnetic layers  13  is along the first direction D 1 . One of the multiple third non-magnetic layers  13 N is between one of the multiple third magnetic layers  13  and another one of the multiple third magnetic layers  13 . For example, one of the multiple third magnetic layers  13  is between one of the multiple third non-magnetic layers  13 N and another one of the multiple third non-magnetic layers  13 N. The multiple third non-magnetic layers  13 N include at least one selected from the group consisting of Cr, Cu, Ta, Ti, W, Mo, Nb and Hf. In one example, the multiple third non-magnetic layers  13 N are Ta layers. In another example, the multiple third non-magnetic layers  13 N are alloy layers including Cr and Ti. 
     One of the multiple third non-magnetic layers  13 N is in contact with one of the multiple third magnetic layers  13  and another one of the multiple third magnetic layers  13 . A thickness t 13 N of one of the multiple third non-magnetic layers  13 N along the first direction D 1  is, for example, not less than 50 nm and not more than 200 nm. A thickness t 13  of one of the multiple third magnetic layers  13  along the first direction D 1  is, for example, not less than 50 nm and not more than 500 nm. 
     The multiple third magnetic layers  13  include at least one selected from the group consisting of Fe, Ni and Co. The multiple third magnetic layers  13  are, for example, soft magnetic layers. The multiple third magnetic layers  13  may further include at least one selected from the group consisting of, for example, Cu, Mo and Cr. In one example, the multiple third magnetic layers  13  are, for example, NiFeCuMo layers. 
     In the third stacked body  30 M, the number of the multiple third magnetic layers  13  may be the same as the number of the multiple third non-magnetic layers  13 N, and may be 1 larger, or may be 1 smaller. For example, the number of the multiple third magnetic layers  13  is, for example, not less than 2 and not more than 100. The number of the multiple third non-magnetic layers  13 N is, for example, not less than 2 and not more than 100. 
     For example, at least one of the multiple third non-magnetic layers  13 N may include an amorphous region. One of the multiple third magnetic layers  13  and another one of the multiple third magnetic layers  13  may include a crystal region. 
     The order in which the first stacked body  10 M, the second stacked body  20 M, and the third stacked body  30 M are arranged is arbitrary. 
     An example of the experimental result regarding the electromagnetic wave attenuator will be described below. 
       FIGS.  3 A and  3 B  are graphs illustrating evaluation results of the electromagnetic wave attenuator. 
     The horizontal axis of these figures is frequency f 1 . The vertical axis is attenuation performance MSE (Magnetic Shielding Effect). A large absolute value of the attenuation performance MSE value corresponds to a large attenuation of the electromagnetic wave. 
       FIG.  3 A  illustrates evaluation results of a first sample SP 1  and a third sample SP 3 .  FIG.  3 B  illustrates evaluation results of a second sample SP 2  and the third sample SP 3 . The characteristics of the third sample SP 3  shown in  FIG.  3 B  are the same as the characteristics of the third sample SP 3  shown in  FIG.  3 A . 
     The first sample SP 1  has the above-mentioned configuration of the electromagnetic wave attenuator  10 A. In the first sample SP 1 , the first magnetic layer  11  is a NiFeCuMo layer. The first non-magnetic layer  11 N is a CrTi alloy layer. The thickness t 11  is 50 nm. The thickness t 11 N is 5 nm. The number of repetitions of the first magnetic layer  11  and the first non-magnetic layer  11 N is 55. The second magnetic layer  12  is a NiFeCuMo layer. The second non-magnetic layer  12 N is a Cu layer. The thickness t 12  is 100 nm. The thickness t 12 N is 100 nm. The number of repetitions of the second magnetic layer  12  and the second non-magnetic layer  12 N is 10. The third magnetic layer  13  is a NiFeCuMo layer. The third non-magnetic layer  13 N is a CrTi layer. The thickness t 13  is 300 nm. The thickness t 13 N is 5 nm. The number of repetitions of the third magnetic layer  13  and the third non-magnetic layer  13 N is 10. These layers are formed, for example, by a sputtering method. 
     In the second sample SP 2 , in the configuration of the first sample SP 1  described above, the first non-magnetic layer  11 N and the third non-magnetic layer  13 N are Ta layers. The other configurations of the second sample SP 2  are the same as those of the first sample SP 1 . 
     In the third sample SP 3 , the first stacked body  10 M, the second stacked body  20 M, and the third stacked body  30 M are not provided, but a Cu layer is provided. A thickness of the Cu layer is 8 μm. 
     As shown in  FIGS.  3 A and  3 B , the attenuation performance MSE obtained in the third sample SP 3  is larger than that obtained in the first sample SP 1  and the second sample SP 2  in the high frequency range (for example, not less than 100 MHz and not more than 2 GHz or less). This is an effect of the Cu material. However, in the third sample SP 3 , the attenuation performance MSE is small in the low frequency region (for example, not more than 100 MHz). 
     As shown in  FIG.  3 B , in the second sample SP 2 , the attenuation performance MSE is larger than that of the third sample SP 3  in the low frequency region. In the second sample SP 2 , there is a peak of the attenuation performance MSE when the frequency f 1  is 40 MHz to 50 MHz. 
     As shown in  FIG.  3 A , in the first sample SP 1 , in the low frequency region, the attenuation performance MSE is larger than that of the third sample SP 3 . In the first sample SP 1 , the large attenuation performance MSE can be obtained in a wide range of frequencies f 1  of about 15 MHz to 50 MHz. Comparing  FIGS.  3 A and  3 B , in the first sample SP 1 , the attenuation performance MSE is larger than that of the second sample SP 2  in a low frequency region of not more than 50 MHz. In particular, the large attenuation performance MSE can be obtained even at 20 MHz. 
     As described above, by using the first non-magnetic layer  11 N including Cr and Ti, the large attenuation performance MSE can be obtained. According to the embodiment, it is possible to provide an electromagnetic wave attenuator with larger attenuation capability. In particular, the large attenuation performance MSE can be obtained in a low frequency region (for example, not more than 100 MHz). Electromagnetic waves in the low frequency region can be effectively attenuated. 
       FIGS.  4 A and  4 B  are electron microscope images of cross section of the electromagnetic wave attenuator according to the first embodiment. 
       FIG.  4 B  is a magnified image of a part of  FIG.  4 A . These images are cross-sectional TEM (Transmission Electron Microscopy) images of the first stacked body  10 M in the first sample SP 1 . 
     As shown in  FIGS.  4 A and  4 B , the multiple first magnetic layers  11  include crystal grains (first crystal grains  11   g ). Crystal grains are not observed in the multiple first non-magnetic layers  11 N. The multiple first non-magnetic layers  11 N are amorphous. In these figures, a line of the outer shape of the cross section of the crystal grain is drawn based on the cross-sectional TEM image so that the first crystal grain  11   g  can be easily seen. 
     An amorphous first non-magnetic layer  11 N is provided between one of the multiple first magnetic layers  11  and another one of the multiple first magnetic layers  11 . As a result, the crystal state in each of the multiple first magnetic layers  11  is divided. For example, the size of the crystal grains (multiple first crystal grains  11   g ) in each of the multiple first magnetic layers  11  tends to be small. As a result, it is considered that the large attenuation performance MSE can be obtained. 
     For example, exchange coupling interactions align spins in a ferromagnet. For example, when the magnetic material is a polycrystalline material, this exchange coupling interaction becomes small or zero at the grain boundaries. Therefore, when an alternating magnetic field is applied to the magnetic material of the polycrystalline material, the spins in a group of crystal grains precess as one unit. It is considered that when the size of the crystal grains is small, the unit that performs this dynamic behavior becomes small, and for example, the static magnetic interaction becomes stronger. As a result, for example, it is considered that the attenuation of electromagnetic waves is improved. 
     In the case of a soft magnetic thin film, it is considered that good soft magnetic properties can be obtained when the crystal grain size is small. For example, when the crystal grain size is small, the coercive force is small and the magnetic permeability is large. In the embodiment, it is easy to obtain crystals having a small size. Thereby, good soft magnetic properties can be obtained. Good shielding performance can be obtained. On the other hand, the thickness of the first non-magnetic layer  11 N provided between the two magnetic layers is thin. As a result, it is considered that a strong magnetostatic coupling interaction acts between the two first magnetic layers  11 . As a result, it is considered that a cooperative precession occurs in the entire stacked multiple first magnetic layers  11 . As a result, it is considered that a large shielding performance is obtained. 
       FIG.  5    is an electron microscope image of cross section of the electromagnetic wave attenuator according to the first embodiment. 
       FIG.  5    is a cross-sectional TEM image of the first stacked body  10 M and the second stacked body  20 M in the first sample SP 1 . As shown in  FIG.  5   , the multiple second magnetic layers  12  include crystal grains (multiple second crystal grains  12   g ). The multiple first magnetic layers  11  include crystal grains (multiple first crystal grains  11   g ). An average diameter of the multiple second crystal grains  12   g  is larger than an average diameter of the multiple first crystal grains  11   g . In  FIG.  5   , a line of the outer shape of the cross section of the crystal grain is drawn based on the cross-sectional TEM image so that the second crystal grain  12   g  can be easily seen. 
     Each of the multiple first crystal grains  11   g  has a first crystal grain width of  11   w . The first crystal grain width  11   w  is a width of each of the multiple first crystal grains  11   g  along the vertical direction. The vertical direction is perpendicular to the first direction D 1 . The vertical direction is, for example, the X-axis direction. In the multiple first crystal grains  11   g , the average of the first crystal grain width  11   w  is, for example, not less than 2 nm and not more than 20 nm. 
     Each of the multiple second crystal grains  12   g  has a second crystal grain width  12   w  along the above-mentioned vertical direction. In the multiple second crystal grains  12   g , the average of the second crystal grain width  12   w  is, for example, not less than 30 nm and not more than 200 nm. 
     In the second stacked body  20 M, the second non-magnetic layer  12 N includes Cu. When the second stacked body  20 M including the second non-magnetic layer  12 N of Cu is provided, a large eddy current loss occurs in the Cu layer. As a result, the baseline of the shielding effect can be raised in a wide frequency range. When the second stacked body  20 M including the second non-magnetic layer  12 N of Cu is provided, the shielding characteristics in a wide frequency range (for example, not less than 20 MHz and not more than 6 GHz) are improved as compared with the case where the second stacked body  20 M is not provided. This effect is considered to be an effect peculiar to Cu. 
     For example, the first stacked body  10 M that can obtain the large attenuation performance MSE in a low frequency region and the second stacked body  20 M that can obtain the large attenuation performance MSE in a wide frequency region are combined. As a result, the attenuation performance MSE larger than that of the third sample SP 3  can be obtained in the low frequency region, and relatively large attenuation performance MSE can be obtained even in the high frequency region. 
     An amorphous third non-magnetic layer  13 N is provided between one of the multiple third magnetic layers  13  and another one of the multiple third magnetic layers  13 . As a result, the crystal in each of the multiple third magnetic layers  13  is divided. For example, the size of the crystal grains in each of the multiple third magnetic layers  13  tends to be small. As a result, it is considered that the large attenuation performance MSE is obtained. 
     As described with respect to  FIGS.  3 A and  3 B , the attenuation performance MSE in the first sample SP 1  (CrTi) is larger than the attenuation performance MSE in the second sample SP 2  (Ta) in the low frequency region. This is considered to be related to the fact that good soft magnetic properties can be obtained by using the CrTi layer as described below. 
       FIG.  6    is a graph illustrating characteristics of the electromagnetic wave attenuator. 
     The horizontal axis of  FIG.  6    is the magnetic field H 1  applied to the electromagnetic wave attenuator. The vertical axis is the magnetization M 1 . The magnetization M 1  is normalized.  FIG.  6    shows measurement results for the first sample SP 1  and the second sample SP 2 . 
     As shown in  FIG.  6   , the hysteresis of the first sample SP 1  is smaller than that of the second sample SP 2 . The coercive force Hc in the first sample SP 1  is about 1.4 Oe. The coercive force Hc in the second sample SP 2  is about 2.4 Oe. The coercive force of the first sample SP 1  including the CrTi layer is smaller than that of the second sample SP 2  including the Ta layer. By using the CrTi layer, good soft magnetic properties can be obtained. The small coercive force of the CrTi layer may be due to, for example, a difference in the concentration of an unintended element (for example, residual oxygen) included in the soft magnetic layer. 
     In the embodiment, as described below, each of the multiple first magnetic layers  11  may have an uneven shape. 
       FIG.  7    is a schematic cross-sectional view illustrating the electromagnetic wave attenuator according to the embodiment. 
     As shown in  FIG.  7   , each of the multiple first magnetic layers  11  has an uneven shape. The multiple first non-magnetic layers  11 N follow the uneven shape of the multiple first magnetic layers  11 . 
     One of the multiple first magnetic layers  11  includes a first magnetic layer surface  11   fa . The first magnetic layer surface  11   fa  faces one of the multiple first non-magnetic layers  11 N. The first magnetic layer surface  11   fa  includes a first top portion  11   pp , a second top portion  11   pq , and a first bottom portion  11   dp . One direction that crosses the first direction D 1  is defined as a crossing direction De 2 . The crossing direction De 2  is, for example, the X-axis direction. 
     A position of the first bottom portion  11   dp  in the crossing direction De 2  is between a position of the first top portion  11   pp  in the crossing direction De 2  and a position of the second top portion  11   pq  in the crossing direction De 2 . At least a part of the multiple first non-magnetic layers  11 N is between the first top portion  11   pp  and the second top portion  11   pq  in the crossing direction De 2 . A distance along the first direction D 1  between the first top portion  11   pp  and the first bottom portion  11   dp  is, for example, not less than 10 nm. The distance corresponds to the height (depth) of the unevenness. 
     It is considered that magnetostatic interaction of magnetization can be made larger between one of the multiple first magnetic layers  11  and another one of the multiple first magnetic layers  11  by providing such an uneven shape, for example. 
     In the embodiment, a concentration of Cr in the multiple first non-magnetic layers  11 N is, for example, not less than 30 atomic % and not more than 70 atomic %. At such a concentration, for example, good soft magnetic properties can be easily obtained. 
     Second Embodiment 
     The second embodiment relates to an electronic device. The electronic device according to the embodiment includes the electromagnetic wave attenuator according to the first embodiment and an arbitrary electronic element. The electromagnetic wave attenuator according to the first embodiment is, for example, the electromagnetic wave attenuator  10  or the electromagnetic wave attenuator  10 A, or the like. 
       FIGS.  8 A to  8 D  are schematic views illustrating an electronic device according to a second embodiment. 
       FIG.  8 A  is a perspective view.  FIG.  8 B  is a line A 1 -A 2  cross-sectional view of  FIG.  8 A .  FIG.  8 C  is a line B 1 -B 2  cross-sectional view of  FIG.  8 A .  FIG.  8 D  is a plan view as viewed along arrow AA of  FIG.  8 A .  FIG.  1  or  2    corresponds to a line C 1 -C 2  cross section of  FIG.  8 B . 
     As shown in  FIG.  8 A , the electronic device  110  according to the embodiment includes an electronic element  50  and the electromagnetic wave attenuator (in the example, electromagnetic wave attenuator  10 ). A substrate  60  is further provided in the example. The electromagnetic wave attenuator  10  covers at least a part of the electronic element  50 . The electronic element  50  is, for example, a semiconductor element. 
     In the example as shown in  FIG.  8 B , the electronic element  50  includes a semiconductor chip  50   c , an insulating portion  50   i , and a wire  50   w . In the example, an electrode  50   e , a substrate connector  50   f , and a connector  58  are provided at the substrate  60 . The wire  50   w  electrically connects the electrode  50   e  and a part of the semiconductor chip  50   c . The electrode  50   e  and the connector  58  are electrically connected by the substrate connector  50   f . The substrate connector  50   f  pierces the substrate  60 . The connector  58  functions as an input/output portion of the semiconductor chip  50   c . The connector  58  may be, for example, a terminal. The insulating portion  50   i  is provided around the semiconductor chip  50   c . The insulating portion  50   i  includes, for example, at least one of a resin or a ceramic, etc. The semiconductor chip  50   c  is protected by the insulating portion  50   i.    
     The electronic element  50  includes, for example, at least one of an arithmetic circuit, a control circuit, a memory circuit, a switching circuit, a signal processing circuit, or a high frequency circuit. 
     The base body  10   s  of the electromagnetic wave attenuator  10  (referring to  FIG.  1   ) may be, for example, at least a part of the electronic element  50 . The base body  10   s  of the electromagnetic wave attenuator  10  may be, for example, at least a part of the insulating portion  50   i.    
     In the example as illustrated in  FIG.  8 B , the electromagnetic wave attenuator  10  is electrically connected to a terminal  50   t  provided at the substrate  60 . The electromagnetic wave attenuator  10  is set to one potential (e.g., the ground potential) via the terminal  50   t . For example, the electromagnetic wave attenuator  10  attenuates the electromagnetic waves radiated from the electronic element  50 . For example, the electromagnetic wave attenuator  10  functions as a shield. 
     As shown in  FIGS.  8 A to  8 C , the stacked member  10 MA of the electromagnetic wave attenuator  10  includes a first planar portion  10   p . In the example, the stacked member  10 MA further includes first to fourth side surface portions  10   a  to  10   d . A direction from the electronic element  50  to the first planar portion  10   p  is aligned with the first direction D 1  (e.g., the Z-axis direction). 
     As shown in  FIGS.  8 B and  8 C , the electronic element  50  is positioned between the first planar portion  10   p  and the substrate  60  in the first direction D 1 . 
     As shown in  FIGS.  8 C and  8 D , the electronic element  50  is positioned between the first side surface portion  10   a  and the third side surface portion  10   c  in the X-axis direction. 
     As shown in  FIGS.  8 B and  8 D , the electronic element  50  is positioned between the second side surface portion  10   b  and the fourth side surface portion  10   d  in the Y-axis direction. 
     By using the electromagnetic wave attenuator  10 A described with respect to the first embodiment, for example, electromagnetic waves in the low frequency domain of not more than 100 MHz can be attenuated effectively. An electronic device can be provided in which the attenuation characteristics for electromagnetic waves can be improved. 
     For example, the external emission of the electromagnetic waves generated by the electronic element  50  can be suppressed. For example, the electromagnetic waves from the outside that reach the electronic element  50  can be suppressed. Stable operations are obtained easily in the electronic element  50 . 
     The first planar portion  10   p  may be, for example, substantially a quadrilateral (including a parallelogram, a rectangle, or a square). 
       FIGS.  9 A to  9 D  are schematic views illustrating parts of the electronic device according to the second embodiment. 
     As shown in  FIG.  9 A , the first side surface portion  10   a  of the electromagnetic wave attenuator  10  includes the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N. The stacking direction of the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N in the first side surface portion  10   a  is a second direction D 2 . 
     As shown in  FIG.  9 B , the second side surface portion  10   b  of the electromagnetic wave attenuator  10  includes the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N. The stacking direction of the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N in the second side surface portion  10   b  is a third direction D 3 . 
     As shown in  FIG.  9 C , the third side surface portion  10   c  of the electromagnetic wave attenuator  10  includes the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N. The stacking direction of the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N in the third side surface portion  10   c  is the second direction D 2 . 
     As shown in  FIG.  9 D , the fourth side surface portion  10   d  of the electromagnetic wave attenuator  10  includes the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N. The stacking direction of the multiple first magnetic layers  11  and the multiple first non-magnetic layers  11 N in the fourth side surface portion  10   d  is the third direction D 3 . 
     The first magnetic layers  11  that are included in the first to fourth side surface portions  10   a  to  10   d  each may be continuous with the first magnetic layer  11  included in the first planar portion  10   p . The first non-magnetic layers  11 N that are included in the first to fourth side surface portions  10   a  to  10   d  each may be continuous with the first non-magnetic layer  11 N included in the first planar portion  10   p.    
     Thus, the electronic device  110  according to the embodiment includes the electronic element  50  and the electromagnetic wave attenuator  10  according to the first embodiment. For example, a direction from the electronic element  50  to the electromagnetic wave attenuator  10  is the first direction. 
     As described above, the stacked member  10 MA may further include the first side surface portion  10   a  (see  FIG.  9 A ). The first side surface portion  10   a  includes a first side surface stacked body  10   a M. The first side surface stacked body  10   a M includes multiple first side surface magnetic layers  11   s  and multiple first side surface non-magnetic layers  11   s N. The multiple first side surface non-magnetic layers  11   s N include Cr and Ti. The multiple first side surface magnetic layers  11   s  correspond to the multiple first magnetic layers  11  in the first planar portion  10   p . The multiple first side surface non-magnetic layers  11   s N correspond to the multiple first non-magnetic layers  11 N in the first planar portion  10   p.    
     A direction from one of the multiple first side surface magnetic layers  11   s  to another of the multiple first side surface magnetic layers  11   s  is along the second direction D 2  crossing the first direction D 1 . One of the multiple first side surface non-magnetic layers  11   s N is between one of the multiple first side surface magnetic layers  11   s  and another one of the multiple first side surface magnetic layers  11   s . One of the multiple first side surface magnetic layers  11   s  is between one of the multiple first side surface non-magnetic layers  11   s N and another one of the multiple first side surface non-magnetic layers  11   s N. 
     One of the multiple first side surface non-magnetic layers  11   s N includes an amorphous region. One of the multiple first side surface magnetic layers  11   s  and another one of the multiple first side surface magnetic layers  11   s  include a crystal region. 
     For example, the electromagnetic wave attenuator  10  includes multiple regions (or multiple portions). At least a part of the electronic element  50  is provided between the multiple regions. The multiple electromagnetic wave attenuation bodies  10  may be provided. The multiple electromagnetic wave attenuators  10  correspond to, for example, the first planar portion  10   p  and the first to fourth side surface portions  10   a  to  10   d . For example, at least a part of the electronic element  50  may be provided between the multiple electromagnetic wave attenuation bodies  10 . 
       FIGS.  10  to  15    are schematic cross-sectional views illustrating electronic devices according to the second embodiment. 
     As shown in  FIG.  10   , an electronic device  111  according to the embodiment includes the electromagnetic wave attenuator  10  and multiple electronic elements (electronic elements  51 ,  51 B,  52 ,  53 ,  53 B,  53 C, etc.). 
     The electronic elements are provided between the multiple regions of the electromagnetic wave attenuator  10 . An insulating region (insulating portions  41  and  42 , etc.) may be provided between the electronic element and one of the multiple regions of the electromagnetic wave attenuator  10 . A resin portion (resin portions  511 ,  521 ,  531 , etc.) may be provided between the electronic element and the insulating region (the insulating portions  41  and  42 , etc.). A connection member (connection members  51 N,  52 N,  53 N, etc.) may be provided for each of the multiple electronic elements. For example, the electronic element and the connector  58  may be electrically connected by the connection member. 
     As in an electronic device  112  shown in  FIG.  11   , the connection member  51 N may be sunk into a substrate  55 . In the electronic device  112 , the electromagnetic wave attenuator  10  is provided between the multiple electronic elements. For example, it is suppressed that the electromagnetic waves generated by one of the multiple electronic elements is incident on another one of the multiple electronic elements. 
     As in an electronic device  113  shown in  FIG.  12   , a mounting member  220  may be provided. The mounting member  220  includes the substrate  55  and the electromagnetic wave attenuator  10 . The electronic elements (electronic elements  51  and  51 B) are provided between the mounting member  220  and another electromagnetic wave attenuator  10 . 
     As in an electronic device  114  shown in  FIG.  13   , the electromagnetic wave attenuator  10  may be provided at the side surface of the electronic element  51 . The side surface crosses the X-Y plane. 
     As in an electronic device  115  shown in  FIG.  14   , the electromagnetic wave attenuator  10  may be provided to continuously surround the multiple electronic elements (electronic elements  51  and  52 ). 
     As in an electronic device  116  shown in  FIG.  15   , one of the multiple electronic elements (electronic element  51 ) is provided between the multiple regions of the electromagnetic wave attenuator  10 . Another one of the multiple electronic elements electronic element  52 ) may not be provided between the multiple regions of the electromagnetic wave attenuator  10 . 
     According to the electronic devices  111  to  116  as well, an electronic device can be provided in which the attenuation characteristics for electromagnetic waves can be improved. 
     For example, the embodiments are applicable to an electronic device and an electromagnetic wave attenuator for EMC 
     (Electro Magnetic Compatibility). 
     The embodiments may include the following configurations (e.g., technological proposals). 
     Configuration 1 
     An electromagnetic wave attenuator, comprising: 
     a stacked member including a first planar portion, 
     the first planar portion including a first stacked body, 
     the first stacked body including a plurality of non-magnetic layers including Cr and Ti, and a plurality of first magnetic layers, 
     a direction from one of the plurality of first magnetic layers to an other one of the plurality of first magnetic layers being along a first direction, 
     one of the plurality of non-magnetic layers being between the one of the plurality of first magnetic layers and the other one of the plurality of first magnetic layers, 
     the one of the first non-magnetic layers including an amorphous region, and 
     the one of the plurality of first magnetic layers and the other one of the plurality of first magnetic layers including a crystal region. 
     Configuration 2 
     The electromagnetic wave attenuator according to Configuration 1, wherein 
     the one of the plurality of first non-magnetic layers is in contact with the one of the plurality of first magnetic layers and the other one of the plurality of the first magnetic layers. 
     Configuration 3 
     The electromagnetic wave attenuator according to Configuration 1 or 2, wherein 
     a thickness of the one of the plurality of first non-magnetic layers along the first direction is not less than 1 nm and not more than 10 nm. 
     Configuration 4 
     The electromagnetic wave attenuator according to any one of Configurations 1 to 3, wherein 
     a thickness of the one of the plurality of first magnetic layers along the first direction is not less than 10 nm and not more than 500 nm. 
     Configuration 5 
     The electromagnetic wave attenuator according to any one of Configurations 1 to 4, wherein 
     the plurality of first magnetic layers include at least one selected from the group consisting of Fe, Ni and Co. 
     Configuration 6 
     The electromagnetic wave attenuator according to any one of Configurations 1 to 5, wherein 
     the first planar portion further includes a second stacked body, 
     a direction from the first stacked body to the second stacked body is along the first direction, 
     the second stacked body includes a plurality of second non-magnetic layers including Cu, and a plurality of second magnetic layers, 
     a direction from one of the plurality of second magnetic layers to an other one of the plurality of second magnetic layers is along the first direction, and 
     one of the plurality of second non-magnetic layers is between the one of the plurality of second magnetic layers and the other one of the plurality of second magnetic layers. 
     Configuration 7 
     The electromagnetic wave attenuator according to Configuration 6, wherein 
     the one of the plurality of second non-magnetic layers is in contact with the one of the plurality of second magnetic layers and the other one of the plurality of second magnetic layers. 
     Configuration 8 
     The electromagnetic wave attenuator according to Configuration 6 or 7, wherein 
     a thickness of the one of the plurality of second non-magnetic layers along the first direction is not less than 50 nm and not more than 200 nm. 
     Configuration 9 
     The electromagnetic wave attenuator according to any one of Configurations 6 to 8, wherein 
     a thickness of the one of the plurality of second magnetic layers along the first direction is not less than 50 nm and not more than 200 nm. 
     Configuration 10 
     The electromagnetic wave attenuator according to any one of Configurations 6 to 9, wherein 
     the plurality of second magnetic layers include at least one selected from the group consisting of Fe, Ni and Co. 
     Configuration 11 
     The electromagnetic wave attenuator according to any one of Configurations 6 to 10, wherein 
     the one of the plurality of first magnetic layers includes a plurality of first crystal grains, 
     the one of the plurality of second magnetic layers includes a plurality of second crystal grains, and 
     an average diameter of the plurality of second crystal grains is larger than an average diameter of the plurality of first crystal grains. 
     Configuration 12 
     The electromagnetic wave attenuator according to Configuration 11, wherein 
     each of the plurality of first crystal grains has a first crystal grain width along a vertical direction perpendicular to the first direction, 
     an average of the first crystal grain width is not less than 2 nm and not more than 20 nm in the plurality of first crystal grains, 
     each of the plurality of second crystal grains has a second crystal grain width along the vertical direction, and 
     an average of the second crystal grain width is not less than 30 nm and not more than 200 nm in the plurality of second crystal grains. 
     Configuration 13 
     The electromagnetic wave attenuator according to any one of Configurations 1 to 12, wherein 
     the first planar portion includes a third stacked body, 
     the third stacked body includes a plurality of third magnetic layers and a plurality of third non-magnetic layers, 
     a direction from one of the plurality of third magnetic layers to an other one of the plurality of third magnetic layers is along the first direction, 
     one of the plurality of third non-magnetic layers is between the one of the plurality of third magnetic layers and the other one of the plurality of third magnetic layers, and 
     the plurality of third non-magnetic layers include at least one selected from the group consisting of Cr, Cu, Ta, Ti, W, Mo, Nb and Hf. 
     Configuration 14 
     The electromagnetic wave attenuator according to Configuration 13, wherein 
     the one of the plurality of third non-magnetic layers is in contact with the one of the plurality of third magnetic layers and the other one of the plurality of third magnetic layers. 
     Configuration 15 
     The electromagnetic wave attenuator according to Configuration 13 or 14, wherein 
     the one of the plurality of third non-magnetic layers includes an amorphous region, and 
     the one of the plurality of third magnetic layers and the other one of the plurality of third magnetic layers include a crystal region. 
     Configuration 16 
     The electromagnetic wave attenuator according to any one of Configurations 1 to 15, wherein 
     the one of the plurality of first magnetic layers includes a first magnetic layer surface facing the one of the plurality of non-magnetic layers, 
     the first magnetic layer surface includes a first top portion, a second top portion, and a first bottom portion, 
     a position of the first bottom portion in a crossing direction crossing the first direction is between a position of the first top portion in the crossing direction and a position of the second top portion in the crossing direction, and 
     at least a part of the one of the plurality of first non-magnetic layers is between the first top portion and the second top portion in the crossing direction. 
     Configuration 17 
     The electromagnetic wave attenuator according to any one of Configurations 1 to 16, further comprising: 
     a base body, 
     a direction from the base body to the first planar portion being along the first direction. 
     Configuration 18 
     The electromagnetic wave attenuator according to Configuration 17, wherein 
     the base body includes a resin. 
     Configuration 19 
     The electromagnetic wave attenuator according to any one of Configurations 1 to 18, wherein 
     the stacked member further includes a first side surface portion, 
     the first side surface portion includes a first side surface stacked body, 
     the first side surface stacked body includes a plurality of first side surface non-magnetic layers including Cr and Ti, and a plurality of first side surface magnetic layers, 
     a direction from one of the plurality of first side surface magnetic layers to an other one of the plurality of first side surface magnetic layers is along a second direction crossing the first direction, 
     one of the plurality of first side surface non-magnetic layers is between the one of the plurality of first side surface magnetic layers and the other one of the plurality of first side surface magnetic layers, 
     the one of the plurality of first side surface non-magnetic layers includes an amorphous region, and 
     the one of the plurality of first side surface magnetic layers and the other one of the plurality of first side surface magnetic layers include a crystal region. 
     Configuration 20 
     An electronic device, comprising: 
     the electromagnetic wave attenuator according to any one of Configurations 1 to 19; and 
     an electronic element. 
     According to the embodiment, an electromagnetic wave attenuator and an electronic device can be provided in which attenuation characteristics of the electromagnetic wave can be improved. 
     Hereinabove, exemplary embodiments of the invention are described with reference to specific examples. However, the embodiments of the invention are not limited to these specific examples. For example, one skilled in the art may similarly practice the invention by appropriately selecting specific configurations of components included in electromagnetic wave attenuators such as stacked bodies, magnetic layers, nonmagnetic layers, etc., from known art. Such practice is included in the scope of the invention to the extent that similar effects thereto are obtained. 
     Further, any two or more components of the specific examples may be combined within the extent of technical feasibility and are included in the scope of the invention to the extent that the purport of the invention is included. 
     Moreover, all electromagnetic wave attenuators, and electronic devices practicable by an appropriate design modification by one skilled in the art based on the electromagnetic wave attenuators, and the electronic devices described above as embodiments of the invention also are within the scope of the invention to the extent that the purport of the invention is included. 
     Various other variations and modifications can be conceived by those skilled in the art within the spirit of the invention, and it is understood that such variations and modifications are also encompassed within the scope of the invention. 
     While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the inventions. Indeed, the novel embodiments described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the embodiments described herein may be made without departing from the spirit of the inventions. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the invention.