Patent Publication Number: US-2022214308-A1

Title: Chirality detection device, chirality detection method, separation device, separation method, and chiral substance device

Description:
TECHNICAL FIELD OF THE INVENTION 
     The present invention relates to a chirality detector, a chirality detection method, a separator, a separation method, and a chiral material device. 
     BACKGROUND OF THE INVENTION 
     Substances with a molecular structure that has chirality and substances with a crystal structure that has chirality (hereinafter collectively referred to as chiral material) are known. For example, lactic acid C 3 H 6 O 3  has a molecular structure with chirality; and there are D-lactic acid and L-lactic acid, which are related as object and mirror image. Quartz (crystal of SiO 2 ) also has a crystal structure with chirality. Quartz has a crystal structure in which SiO 4  tetrahedra share their respective vertexes. If looking at the arrangement of the connected SiO 4  tetrahedra, the SiO 4  tetrahedra form spirals with respect to a direction of crystal elongation (c-axis), and there are crystals in which the spiral is right-handed (right crystal quartz) and crystals in which the spiral is left-handed (left crystal quartz). The crystal structure of the right crystal quartz and that of the left crystal quartz are related as object and mirror image. 
     Properties of chiral material may differ between right-handed and left-handed forms, and methods for detecting chirality of the chiral material are known (see, for example, PTL 1 and PTL 2). 
     Molecular chiral material has been known to generate spin-polarized electrons by a chirality inductive spin selectivity (CISS) effect (see, for example, PTL 3). It has been also known that when spin polarization of a ferromagnetic body is absorbed by spin absorbing material, an electric charge flow occurs in a direction orthogonal to a spin polarization direction and to a spin propagating direction (inverse spin Hall effect) (see, for example, NPL 1). Also, nonlocal spin valve that can detect spin propagation has been known (see, for example, NPL 2). 
     CROSS REFERENCES 
     Patent Literature Documents 
     PTL 1: Japanese Unexamined Patent Application Publication No. 2018-13351 
     PTL 2: Japanese Unexamined Patent Application Publication No. 2015-31605 
     PTL 3: National Publication of Japanese Translation of PCT Application No. 2015-512159 
     Non-Patent Literature Documents 
     NPL 1: T. Kimura, et al.  Phys. Rev. Lett.  98. 156601 (2007) 
     NPL 2: F. J. Jedema, et al.  Nature.  416. 713 (2002) 
     SUMMARY OF THE INVENTION 
     Object of the Invention 
     In the conventional chirality detection methods, subjects are limited to chiral substances contained in solutions or gaseous substances; and solid substances are difficult to detect chirality thereof. 
     The present invention was devised in view of such circumstances, and provides a chirality detector that is capable of detecting chirality of chiral material in various states. 
     Solution to Problem 
     The present invention provides a chirality detector for detecting chirality of chiral material, comprising: a first electrode and a second electrode that are configured to apply a voltage to a subject containing the chiral material; a spin detection layer configured to be in contact with the subject; a power supply; and a control section, wherein the power supply and the control section are configured to generate an electric field at the subject by applying the voltage between the first electrode and the second electrode; and the control section is configured to detect a voltage generated in the spin detection layer in a direction that goes across a direction of the electric field or a voltage generated between the spin detection layer and the subject, and also is configured to detect chirality of the chiral material on the basis of the detected voltage. 
     Advantageous Effect of the Invention 
     The power supply and the control section are configured to generate the electric field at the subject containing the chiral material by applying the voltage between the first electrode and the second electrode. When the electric field is generated in this way, spin-polarized electrons can be generated in the chiral material by a chirality inductive spin selectivity (CISS) effect. 
     The CISS effect is an effect that electrons are spin-polarized when the electrons pass through a chiral polymer. Experiments conducted by the inventors of the present invention have revealed that the CISS effect occurs not only in polymers but also in chiral materials (for example, inorganic chiral crystal). 
     The control section is provided so as to detect a voltage generated in the spin detection layer in a direction that goes across a direction of the electric field or a voltage generated between the spin detection layer and the subject, the spin detection layer being disposed in contact with the subject. Since the voltage to be detected changes depending upon the chirality of the chiral material, the chirality of the chiral material can be detected based upon the detected voltage. This was revealed by the experiments conducted by the inventors of the present invention. 
     The voltage generated in the spin detection layer is thought to be generated by an inverse spin Hall effect. 
     The voltage generated between the spin detection layer and the subject is thought to be generated by a similar effect to nonlocal spin valve. 
     The experiments conducted by the inventors of the present invention made it clear that the inverse of the CISS effect occurs in chiral material (for example, inorganic chiral crystal). When an electric field is applied to the spin detection layer, the electric field brings about the inverse effect related by a reciprocity theorem to the electric field; that is, a voltage is generated in the chiral material. This voltage can be detected using the voltage application section. Since the voltage to be detected changes depending upon the chirality of the chiral material, the chirality of the chiral material can be detected based upon the detected voltage. The experiments conducted by the inventors of the present invention revealed that the chirality detector can perform the reverse process by interchanging the power supply and the control section. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1  shows a diagrammatic perspective view of a chirality detector in accordance with one Embodiment of the present invention. 
         FIG. 2  shows a diagrammatic perspective view of a chirality detector in accordance with one Embodiment of the present invention. 
         FIG. 3  shows a diagrammatic perspective view of a chirality detector in accordance with one Embodiment of the present invention. 
         FIG. 4  shows a diagrammatic perspective view of a chirality detector in accordance with one Embodiment of the present invention. 
         FIG. 5  shows a diagrammatic perspective view of a chirality detector in accordance with one Embodiment of the present invention. 
         FIG. 6  shows a diagrammatic view of a separator in accordance with one Embodiment of the present invention. 
         FIG. 7  shows a diagrammatic view of a separator in accordance with one Embodiment of the present invention. 
         FIG. 8  shows a diagrammatic perspective view of a chiral material device in accordance with one Embodiment of the present invention. 
         FIG. 9  shows a photograph of a measuring device prepared to measure CrNb 3 S 6  as a subject. 
         FIG. 10  shows a photograph of a measuring device prepared to measure WC as a subject. 
         FIG. 11  shows a graph showing a change in voltage between electrodes for voltage detection and a graph showing a change in electric resistance value, at a time of applying a voltage to CrNb3S6 or WC. 
         FIG. 12  shows a graph showing a change in voltage at a spin detection layer (Pt layer) and a graph showing a change in electric resistance value at the spin detection layer, at a time of applying a voltage to CrNb 3 S 6  or WC. 
         FIG. 13  shows a graph showing a change in voltage at a spin detection layer (Pt layer) and a graph showing a change in electric resistance value at the spin detection layer, at a time of applying a voltage to CrNb 3 S 6 . 
         FIG. 14( a )  shows a photograph of a measuring device prepared to measure CrSi 2  as a subject; and  FIGS. 14( b ) and 14( c )  show graphs showing results of voltage detection experiments using this device. 
         FIG. 15( a )  shows a photograph of a measuring device prepared to measure NbSi 2  as a subject; and  FIGS. 15( b ) and 15( c )  show graphs showing results of voltage detection experiments using this device. 
         FIG. 16( a )  shows a photograph of a measuring device prepared to measure left-handed crystal quartz as a subject; and  FIG. 16( b )  shows a graph showing results of voltage detection experiments using this device. 
         FIG. 17( a )  shows a photograph of a measuring device prepared to measure right-handed crystal quartz as a subject; and  FIG. 17( b )  shows a graph showing results of voltage detection experiments using this device. 
         FIG. 18( a )  shows a photograph of a measuring device prepared to measure a chiral molecule dispersion solution as a subject; and  FIG. 18( b )  shows a graph showing results of voltage detection experiments using this device. 
     
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     A chirality detector of the present invention for detecting chirality of chiral material, comprises: a first electrode and a second electrode that are configured to apply a voltage to a subject containing the chiral material; a spin detection layer configured to be in contact with the subject; a power supply; and a control section, wherein the power supply and the control section are configured to generate an electric field at the subject by applying the voltage between the first electrode and the second electrode; the control section is configured to detect a voltage generated in the spin detection layer in a direction that goes across a direction of the electric field or a voltage generated between the spin detection layer and the subject, and also is configured to detect chirality of the chiral material on the basis of the detected voltage. 
     It is desirable that the spin detection layer should contain a ferromagnetic body and that the control section should be configured to detect the voltage generated between the spin detection layer and the subject. The voltage to be detected by the control section changes depending upon spin polarization in a similar manner to spin valve, thereby allowing right-handed chiral material and left-handed chiral material to be discriminated from each other. 
     The present invention provides a chirality detector for detecting chirality of chiral material, comprising: a third electrode and a fourth electrode that are electrically connected with a subject containing the chiral material; a spin injection layer configured to be in contact with the subject; a power supply; and a control section, wherein the power supply and the control section are configured to apply an electric current to the spin injection layer; and the control section is configured to detect, with use of the third electrode and the fourth electrode, a voltage generated in the chiral material in a direction that goes across a direction of the electric current, and also is configured to detect chirality of the chiral material on the basis of the detected voltage. 
     The present invention also provides a chirality detection method comprising: upon generating an electric field at a subject containing chiral material, detecting a voltage generated in a spin detection layer in a direction that goes across a direction of the electric field or a voltage generated between the spin detection layer and the subject, the spin detection layer being configured to be in contact with the subject; and detecting chirality of the chiral material on the basis of the detected voltage. 
     The present invention also provides a separator for separating a right-handed form and a left-handed form of chiral material from each other, comprising: a flow channel configured to flow solution, liquid, or gas, any of which containing the right-handed form and the left-handed form; a voltage application section configured to generate an electric field in the solution, the liquid, or the gas flowing through the flow channel; and a magnetic field application section configured to generate a magnetic field in the solution, the liquid, or the gas flowing downstream from the electric field, wherein the separator is characterized by separating the right-handed form and the left-handed form from each other with use of an interaction between the magnetic field and spin polarization of the chiral material that is generated by the electric field. 
     The present invention also provides a separation method comprising: applying a voltage to solution, liquid, or gas, any of which containing chiral material, so as to generate spin polarization in the chiral material with a right-handed form and a left-handed form; and applying a magnetic field so as to generate a magnetic field in the chiral material-containing solution, liquid, or gas where the spin polarization has been generated, wherein the separation method is characterized by separating the right-handed form and the left-handed form from each other with use of an interaction between the spin polarization and the magnetic field. 
     Hereinafter, Embodiments of the present invention will be described with reference to the accompanying drawings. Structures shown in the drawings or described below should be recognized as exemplifications in all respects, and the scope of the present invention is not limited to the drawings and the following descriptions. 
     Chirality Detectors and Chirality Detection Methods 
       FIGS. 1 to 5  show diagrammatic perspective views of chirality detectors in accordance with the present Embodiments, respectively. 
     Chirality detectors  20  in accordance with the present Embodiments are configured to detect chirality of chiral material and are characterized by comprising: electrodes for voltage application  3   a,    3   b  configured to apply a voltage to a subject  9  containing the chiral material; a spin detection layer  4  configured to be in contact with the subject  9 ; a power supply  5 ; and a control section  7 , wherein the power supply  5  and the control section  7  are configured to generate an electric field at the subject  9  by applying a voltage between the electrode for voltage application  3   a  and the electrode for voltage application  3   b;  and the control section  7  is configured to detect a voltage generated in the spin detection layer  4  in a direction that goes across a direction of the electric field or a voltage generated between the spin detection layer  4  and the subject  9  and also is configured to detect chirality of the chiral material on the basis of the detected voltage. 
     Chiral material (chiral substance) is substance having molecular structures with chirality or material having crystal structures with chirality. There are a right-handed form and a left-handed form in the chiral material. The right-handed and the left-handed forms of the chiral material are enantiomers. The chiral material may be inorganic material, macromolecule, organic molecule, or crystal. 
     The chirality detector  20  is to detect chirality of materials. For example, the chirality detector  20  may be a device that detects whether material contained in the subject  9  has chirality. The chirality detector  20  may also be a device that discriminates that chiral material contained in the subject  9  is right-handed or left-handed or that chiral material is in both right-handed form and left-handed form (for example, a racemic body). Also, the chirality detector  20  may be a device that detects a ratio of a right-handed form and a left-handed form of chiral material. The chirality detector  20  may also be a device that measures a configuration and an anisotropy of chiral material. 
     The subject  9  is a subject to be subjected to measurements by the chirality detector  20 . The subject  9  may be solid, liquid, or gas. If the subject  9  is solid, the subject  9  may be monocrystal, polycrystal, microcrystalline, or aggregate of powder. If the subject  9  is solid, chiral material layers  2  of the chirality detectors  20  shown in  FIGS. 1 to 3  are considered subjects  9 . 
     If the subject  9  is liquid, the subject  9  may be a solution containing chiral material molecules, liquid chiral material, a suspension in which chiral material particles are dispersed in the liquid, or liquid crystal. 
     If the subject  9  is gas, the subject  9  may be gaseous chiral material, mixed gas containing chiral material, or gas in which chiral material microparticles float. 
     If the subject  9  is liquid or gas, the chirality detector  20 , such as those shown in  FIGS. 4 and 5 , is capable of flowing or storing the subject  9  (chiral material-containing solution, liquid, or gas  11 ) in a flow channel  16  provided with the electrodes for voltage application  3   a,    3   b  and the spin detection layer  4 . 
     The power supply  5  is to supply electric power to the electrodes for voltage application  3   a,    3   b.  The power supply  5  may be provided in order to supply electric power to the control section  7 . The electric power supplied from the power supply  5  to the electrodes for voltage application  3   a,    3   b  may be controlled by the control section  7 . The power supply  5  may be a battery or any power supply that uses electric power supplied from an electric power system. The electric power supplied from the power supply  5  to the electrodes for voltage application  3   a,    3   b  can be controlled by the control section  7 . 
     The control section  7  is to control the chirality detector  20 . The control section  7  may be a computer, a microcontroller, or a controlling substrate. The control section  7  may comprise a voltage detecting circuit (voltage measuring section  6   a,    6   b,    6   c ) or a power controlling circuit. 
     The electrodes for voltage application  3   a,    3   b  are to apply a voltage to the subject  9 . The electrodes for voltage application  3   a,    3   b  are configured in such a way that the voltage is applied between the electrode  3   a  and the electrode  3   b  so that an electric field is generated at the subject  9 . The electric field generated at the subject  9  with use of the electrodes  3   a,    3   b  can induce electrons to be spin-polarized in the chiral material contained in the subject  9  by virtue of a chirality inductive spin selectivity (CISS) effect. 
     The CISS effect is an effect that electrons are spin-polarized when the electrons pass through chiral macromolecules. The inventors of the present invention found through experiments that the CISS effect occurred in chiral materials (for example, inorganic chiral crystals) besides the macromolecules. 
     If the subject  9  is solid, the electrodes for voltage application  3   a,    3   b  may be disposed, for example, at edge(s) or on an upper face of the subject  9 , as in the chirality detectors  20  shown in  FIG. 1  to  FIG. 3 . 
     If the subject  9  is liquid or gas, the electrodes for voltage application  3   a,    3   b  may be disposed, for example, in such a way that an electric field is generated in the flow channel  16 , as in the chirality detectors  20  shown in  FIGS. 4 and 5 . In this case, the electrodes for voltage application  3   a,    3   b  each may be in the form of a plate, a ring, or a mesh. 
     The spin detection layer  4  is to absorb spins of spin polarization induced in the subject  9 . The spin detection layer  4  is disposed so as to be in contact with the subject  9 . The spin detection layer  4  may be made of material that is large in conversion efficiency from a spin propagation to an electric charge flow. In this case, the electric charge flow is generated in the spin detection layer  4  due to an inverse spin Hall effect. With the inverse spin Hall effect, the electric charge flow is generated in the spin absorbing material in a direction perpendicular to a spin polarization direction and to a spin propagating direction when the spin absorbing material absorbs the spin polarization. Therefore, a direction and a magnitude of an electromotive force generated in the spin detection layer  4  change depending upon the spin direction of the spin polarization induced in the subject  9 . 
     In this case, the spin detection layer  4  may be disposed as in the chirality detectors  20  shown in  FIGS. 1, 2, 4, and 5 . 
     The spin detection layer  4  is preferably made of spin absorbing material with a large spin Hall angle. Examples of the spin absorbing material include material whose spin orbit interaction is large (such as Pt and W), a topological insulator, (Weyl) semimetal, a two-dimensional gas system, a hybrid film such as metal/oxide or metal/molecule, oxide, molecule, dielectric, semiconductor, and a Rashba system. 
     The spin detection layer  4  may be made of ferromagnetic material. When such a spin detection layer  4  is in contact with the subject  9 , the spin polarization of the chiral material contained in the subject  9  can generate an electromotive force between the spin detection layer  4  and the subject  9 , which similar to a spin valve. In this case, it is desirable that a shape of the spin detection layer  4  should be anisotropic so as to become magnetized uniformly. 
     In this case, the spin detection layer  4  may be disposed as in the chirality detector  20  shown in  FIG. 3 . 
     The spin detection layer  4  may be placed, for example, between the electrode for voltage application  3   a  and the electrode for voltage application  3   b,  as in the chirality detectors  20  shown in  FIG. 1  and  FIG. 4 . The spin detection layer  4  may not be placed between the electrode for voltage application  3   a  and the electrode for voltage application  3   b,  as in the chirality detectors  20  shown in  FIGS. 2, 3, and 5 . The spin polarization generated in the chiral material of the subject  9  with use of the electrodes for voltage application  3   a,    3   b  is generated not only in a portion of the chiral material between the electrode  3   a  and the electrode  3   b  but also in a portion of the chiral material of the subject  9  that has not induced the electric field. This became clear by experiments carried out by the inventors of the present invention. 
     The chirality detector  20  may have electrodes for voltage detection  8   a  to  8   c.  For example, the chirality detector  20  shown in  FIG. 1  has the electrodes  8   a,    8   b  provided so as to detect a voltage in an x direction of the subject  9 . The chirality detector  20  shown in  FIG. 3  has the electrode  8   c  electrically connected with the subject  9  and is capable of detecting a voltage between the spin detection layer  4  and the subject  9  with use of the electrode  8   c.    
     The electrodes for voltage application  3   a,    3   b,  the spin detection layer  4 , the electrodes for voltage detection  8   a  to  8   c,  and so forth may be formed, for example, by a vapor deposition method, a spraying method, an application method, or the like. 
     Next, methods for detecting chirality of the chiral material contained in the subject  9  using the chirality detectors  20  will be described. The below-described methods can be carried out by controlling the chirality detectors  20  by the control section  7 . The control section  7  is provided in order to carry out the following methods. Also, the following methods may be carried out manually without using the control section  7 . 
     The detection methods using the chirality detectors  20  shown in  FIGS. 1, 2, 4 , and  5  will be described. With these methods, a magnetic field is not applied to the subject  9 . With these chirality detectors, the voltage measuring section  6   a  or the control section  7  is provided so as to detect a voltage in a y direction of the spin detection layer  4 . The spin detection layer  4  may be made of material that can convert the spin polarization into an electric charge flow. Examples of the material for the spin detection layer  4  include Pt and W. 
     Firstly, a voltage is applied between the electrode for voltage application  3   a  and the electrode for voltage application  3   b,  generating an electric field at the subject  9 . The electric field generated in this way is capable of generating a spin polarization in the chiral material contained in the subject  9  due to a chirality inductive spin selectivity (CISS) effect. It is believed that a polarization direction of the spin polarization that occurs when the subject  9  contains right-handed chiral material is opposite to a polarization direction of the spin polarization that occurs when the subject  9  contains left-handed chiral material. 
     Secondly, with use of the voltage measuring section  6   a  or the control section  7 , a voltage in a y direction of the spin detection layer  4  is detected. Since the spin detection layer  4  is placed to be in contact with the subject  9 , the chiral material contained in the subject  9  is in contact with the spin detection layer  4 , allowing the spin polarization of the chiral material to induce an electric charge flow in the spin detection layer  4  due to an inverse spin Hall effect. Since the polarization direction of the spin polarization of the right-handed chiral material is opposite to the polarization direction of the spin polarization of the left-handed chiral material, it is believed that a direction of the electric charge flow of the right-handed chiral material also becomes opposite to a direction of the electric charge flow of the left-handed chiral material in the spin detection layer  4 , allowing a direction of an electromotive force of the right-handed chiral material to become opposite to a direction of an electromotive force of the left-handed chiral material. This make it possible to detect a voltage in the y direction of the spin detection layer  4  with use of the voltage measuring section  6   a  or the control section  7  and to compare the direction and the magnitude of the electromotive force with discriminant criteria, with the result that it is possible to discriminate that the chiral material contained in the subject  9  is right-handed or left-handed. 
     The detection method using the chirality detector  20  shown in  FIG. 3  will be described. In this detector, ferromagnetic material is used as material for the spin detection layer  4 . The voltage measuring section  6   a  or the control section  7  is placed so as to detect a voltage between the spin detection layer  4  and the subject  9 . With this method, a magnetic field is not applied to the subject  9 , except for a magnetic field generated from the spin detection layer  4 . 
     Firstly, a voltage is applied between the electrode for voltage application  3   a  and the electrode for voltage application  3   b,  generating an electric field at the subject  9 . The electric field generated in this way is capable of generating a spin polarization in the chiral material contained in the subject  9  due to a chirality inductive spin selectivity (CISS) effect. 
     Secondly, with use of the voltage measuring section  6   a  or the control section  7 , a voltage between the spin detection layer  4  and the subject  9  is detected. Since the spin detection layer  4  made of a ferromagnetic body is placed to be in contact with the subject  9 , a spin polarization of the chiral material generates an electromotive force between the spin detection layer  4  and the subject  9 , depending upon a magnetization state of the ferromagnetic body, which similar to a nonlocal spin valve. Since the polarization direction of the spin polarization of the right-handed chiral material is opposite to the polarization direction of the spin polarization of the left-handed chiral material, the electromotive force, which is generated between the spin detection layer  4  and the subject  9 , of the right-handed chiral material is different from the electromotive force generated in the left-handed chiral material. This makes it possible to detect a voltage between the spin detection layer  4  and the subject  9  with use of the voltage measuring section  6   a  or the control section  7  and to compare the direction and the magnitude of the electromotive force with discriminant criteria, with the result that it is possible to discriminate that the chiral material contained in the subject  9  is right-handed or left-handed. 
     Chirality Detector in which the Inverse of CISS Effect is Used 
     The above-described chirality detectors  20  are configured to detect the chirality of the chiral materials by using the CISS effect. In the present Embodiments, chirality of chiral material is detected by using an inverse effect of the CISS effect. In the present Embodiment, the above-described spin detection layer  4  functions as a spin injection layer  4 ; and the above-described electrodes for voltage application  3   a,    3   b  function as electrodes for voltage detection  3   a,    3   b,  respectively, that are configured to detect a voltage generated in the subject  9 . A structure of a detector in accordance with the present Embodiment is the same as the above-described chirality detectors  20 . 
     A chirality detector  20  in accordance with the present Embodiment is configured to detect chirality of chiral material and is characterized by comprising: an electrode  3   a  and an electrode  3   b  that are electrically connected with a subject  9  containing the chiral material; a spin injection layer  4  configured to be in contact with the subject  9 ; a power supply  5 ; and a control section  7 , wherein the power supply  5  and the control section  7  are configured to apply an electric current to the spin injection layer  4 ; and the control section  7  is configured to detect, with use of the electrode  3   a  and the electrode  3   b,  a voltage generated in the chiral material in a direction that goes across a direction of the electric current, and also is configured to detect chirality of the chiral material on the basis of the detected voltage. 
     In the present Embodiment, the power supply  5  is to supply electric power to the spin injection layer  4 ; and the control section  7  is configured to detect the voltage with use of the electrodes  3   a,    3   b  and to detect the chirality of the chiral material on the basis of the detected voltage. 
     Separators and Separation Methods 
       FIG. 6  and  FIG. 7  show schematic views of separators in accordance with the present Embodiments, respectively. 
     Separators  25  in accordance with the present Embodiments are configured to separate a right-handed form and a left-handed form of chiral material from each other, each of the separators being characterized by comprising: a flow channel  16  configured to flow solution, liquid, or gas, any of which containing the right-handed form and the left-handed form; a voltage application section  12  configured to generate an electric field in the solution, the liquid, or the gas flowing through the flow channel  16 ; and a magnetic field application section  13  configured to generate a magnetic field in the solution, the liquid, or the gas flowing downstream from the electric field, wherein the separators each are characterized by separating the right-handed form and the left-handed form from each other with use of an interaction between the magnetic field and spin polarization of the chiral material that is generated by the electric field. 
     The separators  25  in accordance with the present Embodiments are to separate right-handed chiral material  17  and left-handed chiral material  18  from each other in the solution, the liquid, or the gas. The solution, the liquid, or the gas before the separation contains both the right-handed chiral material  17  and the left-handed chiral material  18 . 
     The separators  25  each in accordance with the present Embodiments is provided with the flow channel  16  configured to flow chiral material-containing solution, liquid, or gas  11 . The flow channel  16  is provided with electrodes for voltage application  3   a,    3   b  (voltage application sections  12 ) configured to generate an electric field in the chiral material-containing solution, liquid, or gas  11 . The electrodes for voltage application  3   a,    3   b  may be disposed in such a way that a direction of the generated electric field becomes parallel to a direction of the flow in the flow channel  16 . 
     The electric field generated by applying a voltage between the electrode  3   a  and the electrode  3   b  with use of a power supply  5   a  (voltage application section  12 ) can generate a spin polarization at the right-handed chiral material  17  and the left-handed chiral material  18 , both of the materials flowing through the flow channel  16 , due to a chirality inductive spin selectivity (CISS) effect. It is believed that a polarization direction of the spin polarization generated at the right-handed chiral material  17  is opposite to a polarization direction of the spin polarization generated at the left-handed chiral material  18 . The relation between the directions of the right-handed chiral material  17  and the left-handed chiral material  18  indicated by arrows in  FIG. 6  and  FIG. 7  is schematic and is not limited to these directions. 
     The magnetic field application section  13  is placed in such a way as to generate a magnetic field at the flow channel  16  that is downstream from the electric field generated between the electrode for voltage application  3   a  and the electrode for voltage application  3   b.  The magnetic field application section  13  may include, for example, power supplys  5   a,    5   b,    5   c  and coils  19 ,  19   a,    19   b.  Magnetic field application sections  13 ,  13   a,    13   b  each may be made of permanent magnet or micro-magnet. The magnetic field application sections  13 ,  13   a,    13   b  may be disposed so that a direction of the magnetic field generated in the flow channel  16  becomes parallel to a flow direction in the flow channel  16 , a direction of the electric field generated between the electrode for voltage application  3   a  and the electrode for voltage application  3   b,  or the spin polarization directions of the right-handed chiral material  17  and the left-handed chiral material  18 . 
     The magnetic field application section  13  may be disposed as in, for example, the separator  25  shown in  FIG. 6 . The coil  19  of this separator is placed to wrap around the flow channel  16 ; and a direct current is applied to this coil  19  by the power supply  5   b.  This makes it possible to generate a magnetic field that is parallel to the flow direction in the flow channel  16 . 
     When the right-handed chiral material  17  having the spin polarization generated thereat and the left-handed chiral material  18  having the spin polarization generated thereat flow through such a magnetic field, one of the right-handed chiral material  17  and the left-handed chiral material  18  in the flow channel  16  becomes faster in flow speed due to the relation between the polarization direction of the spin polarization and the direction of the magnetic field, whereas the other one becomes slower in flow speed in the flow channel  16 . This makes it possible to separate the right-handed chiral material  17  and the left-handed chiral material  18  from each other in the flow in the flow channel  16 . This separator  25  thus separates the right-handed chiral material  17  and the left-handed chiral material  18  from each other in a chromatography manner. 
     The magnetic field application sections  13   a,    13   b  may be disposed as in, for example, the separator  25  shown in  FIG. 7 . The magnetic field application sections  13   a,    13   b  are disposed so as to form the magnetic fields in the flow channel  16  by using leakage magnetic fields. The magnetic field application section  13   a  includes the power supply  5   b  and the coil  19   a  and is disposed so as to form the leakage magnetic field in the flow channel  16 . The magnetic field application section  13   b  includes the power supply  5   c  and the coil  19   b  and is disposed so as to form the leakage magnetic field at the flow channel  16 . The magnetic field formed by the magnetic field application section  13   a  and the magnetic field formed by the magnetic field application section  13   b  are located at the same channel cross-section. 
     When the right-handed chiral material  17  at which the spin polarization has been generated and the left-handed chiral material  18  at which the spin polarization has been generated flow through such magnetic fields, the relation between the polarization direction of the spin polarization and the direction of the magnetic field allows one of the right-handed chiral material  17  and the left-handed chiral material  18  to flow through the magnetic field formed by the magnetic field application section  13   a,  and allows the other chiral material to flow through the magnetic field formed by the magnetic field application section  13   b.  This makes it possible to separate the right-handed chiral material  17  and the left-handed chiral material  18  from each other in the flow in the flow channel  16 . 
     The flow channel  16  is branched in such a way that the chiral material having flowed through the magnetic field formed by the magnetic field application section  13   a  flows through the flow channel  16   a,  and that the chiral material having flowed through the magnetic field formed by the magnetic field application section  13   b  flows through the flow channel  16   b.  This makes it possible to prevent the right-handed chiral material  17  and the left-handed chiral material  18  from being mixed together, both of said chiral materials having been separated using the magnetic fields. This thus makes it possible to collect the chiral materials from the flow channel  16   a  and the flow channel  16   b,  respectively, and to collect the right-handed chiral material  17  and the left-handed chiral material  18  separately. 
     Chiral Material Device 
       FIG. 8  shows a diagrammatic perspective view of a chiral material device in accordance with the present Embodiment. 
     A chiral material device  30  in accordance with the present Embodiment is characterized by comprising: a chiral material layer  2 ; a first electrode for voltage application  3   a  and a second electrode for voltage application  3   b  that are configured to generate an electric field at the chiral material layer  2 ; and a spin detection layer  4  configured to be in contact with the chiral material layer  2 , wherein the first electrode for voltage application  3   a  and the second electrode for voltage application  3   b  are provided so that at least one of the first electrode for voltage application  3   a  and the second electrode for voltage application  3   b  inputs an input signal and are configured to generate the electric field at the chiral material layer  2  by inputting the input signal; and the chiral material device  30  is characterized in that a voltage generated in a direction across the electric field of the spin detection layer  4  changes according to the input signal. 
     The chiral material device  30  is a device that uses properties of chiral material, and may be a transistor, a memory, or a logic device. 
     The chiral material layer  2  is a layer that contains chiral material. The chiral material layer  2  may mainly contain either right-handed chiral material or left-handed chiral material. The chiral material layer  2  may have a structure formed of a layer comprising the right-handed chiral material and a layer comprising the left-handed chiral material. 
     The chiral material layer  2  may be made of single crystal, polycrystalline, microcrystalline, liquid crystal, or aggregate of powder. The chiral material layer  2  may be made of gel containing chiral material. The chiral material layer  2  may be made of a conductor, a semiconductor, or an insulator. 
     The first electrode for voltage application  3   a  and the second electrode for voltage application  3   b  are configured to generate an electric field in the chiral material layer  2 . By applying a voltage between the first electrode for voltage application  3   a  and the second electrode for voltage application  3   b,  the electric field is generated in the chiral material layer  2 . The chiral material device  30  may have the pair of electrodes for voltage application  3   a,    3   b,  as in the device shown in  FIG. 8 , or may have a plurality of pairs of electrodes for voltage application  3   a,    3   b.    
     The electric field generated at the chiral material layer  2  by using the electrodes  3   a,    3   b  is capable of generating spin-polarized electrons in the chiral material contained in the chiral material layer  2  due to a chirality inductive spin selectivity (CISS) effect. If a direction of the electric field generated at the chiral material layer  2  changes, a direction of the spin polarization changes. 
     The spin detection layer  4  is configured to absorb spins of the spin polarization generated in the chiral material layer  2 . The spin detection layer  4  may be arranged, for example, between the electrodes for voltage application  3   a,    3   b,  as in the chiral material device  30  shown in  FIG. 8 . The spin detection layer  4 , however, does not have to be arranged between the electrodes for voltage application  3   a,    3   b.    
     When the plurality of pairs of electrodes for voltage application  3   a,    3   b  are arranged, a plurality of spin detection layers  4  may be placed between the pair of electrodes for voltage application  3   a,    3   b  and the adjacent pair of electrodes for voltage application  3   a,    3   b.  This makes it possible to select the spin detection layer  4  that outputs an output signal. 
     An input section  26  is configured to input an input signal to at least one of the electrodes for voltage application  3   a,    3   b  and to generate an electric field between the electrode for voltage application  3   a  and the electrode for voltage application  3   b  at the chiral material layer  2 . This allows the electric field that changes according to the input signal to be formed at the chiral material layer  2 . For example, the input section  26  may be disposed so that a direction of the electric field to be generated in the chiral material layer  2  changes according to the input signal. When the direction of the electric field of the chiral material layer  2  changes, a direction of the spin polarization of the chiral material layer  2  also changes. Therefore, when the spin detection layer  4  is placed as in the device  30  shown in  FIG. 8 , a direction of the voltage generated in the spin detection layer  4  in a direction across the electric field also changes according to the input signal. By outputting the direction of this voltage from an output section  27  as the output signal, the input signal can be converted into the output signal. 
     The above descriptions of the chirality detectors  20  and other components hold true with the chiral material device unless there is any contradiction. 
     First Chirality Detection Experiment 
     A device A similar to the device in  FIG. 1  was prepared using CrNb 3 S 6 , which is chiral material, as a subject. For the CrNb 3 S 6 , single crystal having a size of 16.9 μm×9.5 μm×500 nm was used. The CrNb 3 S 6  was arranged so that a c-axis (spiral axis) of the CrNb 3 S 6  was positioned in an x direction. For the spin detection layer, a Pt layer having a size of 2 μm×9.5 μm×25 nm was used. The resistivity of the Pt layer was 450 μΩcm, and the resistivity of the CrNb 3 S 6  single crystal was 650 μΩcm. 
       FIG. 9  shows a photograph of the device A as prepared above. Wirings (1) and (2) function as electrodes for voltage application, and are to apply a voltage in the x direction of the CrNb 3 S 6  single crystal. Wirings (5) and (6) function as electrodes for voltage detection, and are to detect a voltage in the x direction of the CrNb 3 S 6  single crystal. Wirings (4) and (8) function as electrodes connected to ends of the Pt layer, respectively, and are to detect a voltage in a y direction of the Pt layer. 
     A device B similar to the device was prepared using WC (tungsten carbide), which is non-chiral material, as a subject. For the WC, one having a size of 16.4 μm×8.4 μm×40 nm was used. For the spin detection layer, a Pt layer having a size of 2 μm×8.4 μm×25 nm was used. The resistivity of the Pt layer is 450 μΩcm, and the resistivity of the WC is 530 μΩcm. 
       FIG. 10  shows a photograph of the device B as prepared above. Wirings (1) and (2) function as electrodes for voltage application, and are to apply a voltage in an x direction of the WC. Wirings (4) and (5) function as electrodes for voltage detection, and are to detect a voltage in the x direction of the WC. Wirings (3) and (6) function as electrodes connected to ends of a Pt layer, respectively, and are to detect a voltage in a y direction of the Pt layer. 
     The voltage applied between the wirings (1) and (2) was changed so that an electric current flowing through the CrNb 3 S 6  single crystal of the device A (from (1) to (2)) would change from −5 mA to 5 mA, thereby measuring a voltage V xx  (the voltage in the x direction of the CrNb 3 S 6  single crystal) between the wirings (5) and (6) and a voltage V xy  (the voltage in the y direction of the Pt layer) between the wirings (4) and (8). From the measured values, a resistance value R xx  of the CrNb 3 S 6  single crystal and a resistance value R xy  of the Pt layer were calculated. 
     An electric current value when the electric current flowed through the CrNb 3 S 6  single crystal from the wiring (1) to the wiring (2) was set to be plus, and an electric current value when the electric current flowed from the wiring (2) to the wiring (1) was set to be minus. The voltage V xx  was set to a plus voltage when an electric potential of the wiring (5) was higher than an electric potential of the wiring (6). The voltage V xy  was set to a plus voltage when an electric potential of the wiring (4) (which is on the right side when facing a direction of the plus electric current flowing through the CrNb 3 S 6 ) was higher than an electric potential of the wiring (8) (which is on the left side when facing the direction of the plus electric current flowing through the CrNb 3 S 6 ). 
     The voltage applied between the wirings (1) and (2) was changed so that an electric current flowing through the WC of the device B (from (1) to (2)) would change from −5 mA to 5 mA, thereby measuring a voltage V xx  (the voltage in the x direction of the WC) between the wirings (4) and (5) and a voltage V xy  (the voltage in the y direction of the Pt layer) between the wirings (3) and (6). From the measured values, a resistance value R xx  of the WC and a resistance value R xy  of the Pt layer were calculated. 
     An electric current value when the electric current flowed through the WC from the wiring (1) to the wiring (2) was set to be plus, and an electric current value when the electric current flowed from the wiring (2) to the wiring (1) was set to be minus. The voltage V xx  was set to a plus voltage when an electric potential of the wiring (4) was higher than an electric potential of the wiring (5). The voltage V xy  was set to a plus voltage when an electric potential of the wiring (3) (which is on the right side when facing a direction of the plus electric current flowing through the WC) was higher than an electric potential of the wiring (6) (which is on the left side when facing the direction of the plus electric current flowing through the WC). 
       FIG. 11( a )  shows a graph showing a change in the measured voltage value V xx  in a horizontal direction; and  FIG. 11( b )  shows a graph showing a change in the calculated resistance value R xx . In both devices A and B, the V xx  changed according to the voltage applied between the wirings (1) and (2). The R xx  was constant. 
       FIG. 12( a )  shows a graph showing a change in the measured voltage value V xy  in a vertical direction of the Pt layer; and  FIG. 12( b )  shows a graph showing a change in the calculated resistance value R xy . In the device B (using the WC), the V xy  was not outputted, and the R xy  was zero, whereas in the device A (using the CrNb 3 S 6 ), when the voltage was applied to the CrNb 3 S 6  so that the plus electric current flowed through it, the plus voltage V xy  was generated in the Pt layer, and when the voltage was applied to the CrNb 3 S 6  so that the minus electric current flowed through it, the minus voltage V xy  was generated in the Pt layer. The voltage V xy  and an electric current I that has flowed through the CrNb 3 S 6  were proportional to each other. In the device A, the R xy  showed a slightly nonlinear behavior as the electric current I flowing through the CrNb 3 S 6  increased. 
     It was thus found that when the subject was the chiral material, and the electric current was applied to the subject, an electromotive force was generated in the Pt layer, which was the spin detection layer. From this finding, it was also found that it was possible to discriminate whether or not the subject was the chiral material by applying the electric current to the subject and examining whether or not the electromotive force was generated in the spin detection layer. 
     The reason why the electromotive force was generated in the spin detection layer is thought to be that the chirality inductive spin selectivity (CISS) effect has generated a spin-polarized state in the chiral material; and this spin-polarized state was converted into the electric charge flow in the Pt (the spin detection layer), which is the material with the large spin orbit interaction, by the inverse spin Hall effect. 
     Next, a voltage V xy  (the voltage in the y direction of the Pt layer) was measured with use of different electrodes for voltage application in the device A. More specifically, the voltage V xy  (the voltage in the y direction of the Pt layer) between the wirings (4) and (8) was measured when an electric current was passed from the wiring (5) to the wiring (2) as shown by a solid arrow in  FIG. 13( a ) . Also, the voltage V xy  (the voltage in the y direction of the Pt layer) between the wirings (4) and (8) was measured when an electric current was passed from the wiring (6) to the wiring (2) as shown by a dotted arrow in  FIG. 13( a ) . A resistance value R xy  of the Pt layer was calculated from the voltages V xy . 
     A distance between the electrodes for voltage application (which is the distance where the electric current flows in the CrNb 3 S 6  single crystal) is longer for the solid arrow than for the dotted arrow. The plus and the minus of the electric current I and the plus and the minus of the voltage V xy  are the same as the measurements as in the device A described above. 
       FIG. 13( b )  shows a graph showing a change in voltage V xy , and  FIG. 13( c )  shows a graph showing a change in resistance value R xy . Similar to the measurement results for the device A shown in  FIG. 12( a ) , when the voltage was applied to the CrNb 3 S 6  so that the plus electric current flowed through it, the plus voltage V xy  was generated in the Pt layer, and when the voltage was applied to the CrNb 3 S 6  so that the minus electric current flowed through it, the minus voltage V xy  was generated in the Pt layer. 
     It was thus found that an electromotive force was generated in the spin detection layer even when the Pt layer, which was the spin detection layer, was not arranged between the electrodes for voltage application. 
     The reason why the electromotive force was generated in the spin detection layer placed to be in contact with a region of the chiral material where the electric current was not flowing is thought to be that the spin-polarized state generated in the chiral material due to the chirality inductive spin selectivity (CISS) effect has induced the spin polarization in the region where the electric current was not flowing. It is thought that this induced spin polarization has been converted to the electric charge flow in the Pt (the spin detection layer) by the inverse spin Hall effect, thereby generating the electromotive force. It was found that the electromotive force was detectable over a relatively long distance, although it could change depending upon the distance. More specifically, in addition to detecting the signals as small as a few micrometers (μm), the signals up to a distance of about 10 mm are detected. 
     Chirality Discrimination Experiments 
     Experiments were carried out to confirm whether left-handed and right-handed forms of chiral material can be discriminated from each other on account of an electromotive force generated in a spin detection layer. 
     Bulk polycrystal of CrSi 2  (P6 4 22 (D 6   5 )) was used as left-handed chiral material. The CrSi 2  has a crystal structure with a left-handed helical atomic arrangement. The orientation of a spiral axis in the polycrystal is uneven (unoriented sample). 
       FIG. 14( a )  shows a photograph of a device C prepared using the CrSi 2  bulk polycrystal. The CrSi 2  bulk polycrystal is provided with wirings (1) and (2), which function as electrodes for voltage application, at both ends of the polycrystal, respectively. The device C had two Pt layers placed between wirings (1) and (2); and wirings (3) and (5) were connected to both ends of the left Pt layer, respectively; and wirings (4) and (6) were connected to both ends of the right Pt layer, respectively. 
     A voltage applied between the wirings (1) and (2) was changed so that an electric current (from (1) to (2)) flowing through the CrSi 2  bulk polycrystal of the device C would change from −21 mA to 21 mA, thereby measuring a voltage V xx  (the voltage in an x direction of the CrSi 2  bulk polycrystal) between the wirings (3) and (4) and a voltage V xy  (the voltage in a y direction of the Pt layer) between the wirings (4) and (6). 
     An electric current value when the electric current flowed through the CrSi 2  bulk polycrystal from the wiring (1) to the wiring (2) was set to be plus, and an electric current value when the electric current flowed from the wiring (2) to the wiring (1) was set to be minus. The voltage V xx  was set to a plus voltage when an electric potential of the wiring (3) was higher than an electric potential of the wiring (4). The voltage V xy  was set to a plus voltage when an electric potential of the wiring (4) (which is on the right side when facing a direction of the plus electric current flowing through the CrSi 2  bulk polycrystal) was higher than an electric potential of the wiring (6) (which is on the left side when facing the direction of the plus electric current flowing through the CrSi 2  bulk polycrystal). 
       FIG. 14( b )  shows a graph showing a change in measured voltage value V xx  in the x direction; and  FIG. 14( c )  shows a graph showing a change in measured voltage value V xy  in the y direction of the Pt layer. The voltage value V xx  has changed depending upon the voltage applied between the wirings (1) and (2). The voltage value V xy  became minus when the voltage was applied, and the plus electric current flowed through the CrSi 2  bulk polycrystal, and became plus when the voltage was applied, and the minus electric current flowed through the CrSi 2  bulk polycrystal. The voltage V xy  and the electric current I flowing through the CrSi 2  bulk polycrystal had a proportionality relation in which a proportionality constant was minus. 
     As the right-handed chiral material, bulk polycrystal of NbSi 2  (P6 4 22 (D 6   4 )) was used. The NbSi 2  has a crystal structure with a right-handed helical atomic arrangement. The orientation of a spiral axis in the polycrystal is uneven (unoriented sample). 
       FIG. 15( a )  shows a photograph of a device D prepared using the NbSi 2  bulk polycrystal. The NbSi 2  bulk polycrystal is provided with wirings (1) and (2), which function as electrodes for voltage application, at both ends of the polycrystal, respectively. The device D had two Pt layers placed between the wirings (1) and (2); and wirings (3) and (5) were connected to both ends of the left Pt layer, respectively; and wirings (4) and (6) were connected to both ends of the right Pt layer, respectively. 
     A voltage applied between the wirings (1) and (2) was changed so that an electric current (from (1) to (2)) flowing through the NbSi 2  bulk polycrystal of the device D would change from −21 mA to 21 mA, thereby measuring a voltage V xx  (the voltage in an x direction of the NbSi 2  bulk polycrystal) between the wirings (5) and (6) and a voltage V xy  (the voltage in a y direction of the Pt layer) between the wirings (4) and (6). 
     An electric current value when the electric current flowed through the NbSi 2  bulk polycrystal from the wiring (1) to the wiring (2) was set to be plus, and an electric current value when the electric current flowed from the wiring (2) to the wiring (1) was set to be minus. The voltage V xx  was set to a plus voltage when an electric potential of the wiring (5) was higher than an electric potential of the wiring (6). The voltage V xy  was set to a plus voltage when an electric potential of the wiring (4) (which is on the right side when facing a direction of the plus electric current flowing through the NbSi 2  bulk polycrystal) was higher than an electric potential of the wiring (6) (which is on the left side when facing the direction of the plus electric current flowing through the NbSi 2  bulk polycrystal). 
       FIG. 15( b )  shows a graph showing a change in measured voltage value V xx  in the x direction; and  FIG. 15( c )  shows a graph showing a change in measured voltage value V xy  in the y direction of the Pt layer. The voltage value V xx  has changed depending upon the voltage applied between the wirings (1) and (2). The voltage value V xy  became plus when the voltage was applied, and the plus electric current flowed through the NbSi 2  bulk polycrystal, and became minus when the voltage was applied, and the minus electric current flowed through the NbSi 2  bulk polycrystal. The voltage V xy  and the electric current I flowing through the NbSi 2  bulk polycrystal had a proportionality relation in which a proportionality constant was plus. 
     From these experiments, it was found that the direction of the electromotive force generated in the spin detection layer of the device using the right-handed chiral material was opposite to the direction of the electromotive force generated in the spin detection layer of the device using the left-handed chiral material. It was then found from this result that it was possible to discriminate whether the chiral material was right-handed or left-handed by applying the electric current to the subject (chiral material) and examining the direction of the electromotive force generated in the spin detection layer. 
     The reason why the directions of the electromotive forces generated in the spin detection layer are opposite to each other is thought to be that the polarization direction of the spin-polarized state of the chiral material is reversed between the right-handed form and the left-handed form due to the chirality inductive spin selectivity (CISS) effect. Therefore, the direction of the electromotive force of the right-handed form in the spin detection layer is also thought to be opposite to the direction of the electromotive force of the left-handed form, both of the forces being generated by the conversion of a spin propagation by the inverse spin Hall effect. 
     Since the electromotive forces were generated in the spin detection layers of the devices C and D, which used the polycrystalline chiral materials as the unoriented samples, it was found that the directions of the electromotive forces generated in the spin detection layer were determined by whether the chiral material was right-handed or left-handed, regardless of the directions of the spin axes. Therefore, the CISS effect was found to be brought about at a molecular level (or a crystal level) of the chiral material. This suggests that chiral material in a solution, liquid crystal that is chiral material, and an insulator that is chiral material can likewise discriminate between a right-handed form and a left-handed form. 
     Second Chirality Detection Experiment 
     In the first chirality detection experiment and the chirality discrimination experiments described above, the conductors were used as the chiral materials, which were the subjects, while a second chirality detection experiment was carried out using left-handed crystal quartz and right-handed crystal quartz, which are insulators, as subjects. The left-handed crystal quartz is left-handed chiral material with a left-handed helical atomic arrangement in a crystal structure, and the right-handed crystal quartz is right-handed chiral material with a right-handed helical atomic arrangement in a crystal structure. Since the crystal quartzes are the insulators, no electric current flows through the chiral materials. Therefore, the measurement was performed by using an inverse effect of the CISS effect. In other words, a voltage is applied to both ends of a Pt layer, and a voltage generated in the chiral materials is detected. 
       FIG. 16( a )  shows a photograph of a device E prepared using the left-handed crystal quartz. The left-handed crystal quartz is provided with wirings (1) and (2), which function as electrodes for voltage detection, at both ends of the left-handed crystal quartz, respectively. The device E had a Pt layer placed between the wirings (1) and (2); and wirings (3) and (4) were connected to both ends of the Pt layer, respectively. This Pt layer functioned as the spin detection layer in the first chirality detection experiment; however, in the second chirality detection experiment using the inverse effect, the Pt layer functions as an electrode for voltage application. 
     A voltage V yx  (the voltage in an x direction of the crystal quartz) between the wiring (1) and the wiring (2) was measured by changing a voltage (pulse voltage) to be applied to the Pt layer by using the wirings (3) and (4). 
     An electric current value when the electric current flowed through the Pt layer from the wiring (3) to the wiring (4) was set to be plus, and an electric current value when the electric current flowed from the wiring (4) to the wiring (3) is set to be minus. The voltage V yx  was set to a plus voltage when an electric potential of the wiring (1) (which is on the right side when facing a direction of the plus electric current flowing through the Pt layer) was higher than an electric potential of the wiring (2) (which is on the left side when facing the direction of the plus electric current flowing through the Pt layer). 
       FIG. 16( b )  shows a graph showing a change in measured voltage value V yx  in the x direction of the crystal quartz. In  FIG. 16( b ) , the voltage applied to the Pt layer is indicated as an electric current value I (mA). 
     By changing the voltage applied to the wirings (3) and (4), an electromotive force was generated in the crystal quartz. The measured voltage value V yx  generated in the left-handed crystal quartz and the voltage applied to the Pt layer had a proportionality relation in which a proportionality constant was minus. Such a tendency in the change of the voltage value V yx  was similar to those seen in the first chirality detection experiment and the chirality discrimination experiments. 
       FIG. 17( a )  shows a photograph of a device F prepared using the right-handed crystal quartz. The right-handed crystal quartz is provided with wirings (1) and (2), which function as electrodes for voltage detection, at both ends of the right-handed crystal quartz, respectively. The device F had a Pt layer placed between wirings (1) and (2); and wirings (3) and (4) were connected to both ends of the Pt layer, respectively. This Pt layer functioned as the spin detection layer in the first chirality detection experiment, but functions as an electrode for voltage application when using the inverse effect. 
     A voltage V yx  (the voltage in an x direction of the crystal quartz) between the wiring (1) and the wiring (2) was measured by changing a voltage (pulse voltage) to be applied to the Pt layer by using the wirings (3) and (4). 
     An electric current value when the electric current flowed through the Pt layer from the wiring (3) to the wiring (4) was set to be plus, and an electric current value when the electric current flowed from the wiring (4) to the wiring (3) is set to be minus. The voltage V yx  was set to a plus voltage when an electric potential of the wiring (1) (which is on the right side when facing a direction of the plus electric current flowing through the Pt layer) was higher than an electric potential of the wiring (2) (which is on the left side when facing the direction of the plus electric current flowing through the Pt layer). 
       FIG. 17( b )  shows a graph showing a change in measured voltage value V yx  in the x direction of the right-handed crystal quartz. In  FIG. 17( b ) , the voltage applied to the Pt layer is indicated as an electric current value I (mA). 
     By changing the voltage applied to the wirings (3) and (4), an electromotive force was generated in the crystal quartz. The measured voltage value V yx  generated in the right-handed crystal quartz and the voltage applied to the Pt layer had a proportionality relation in which a proportionality constant was plus. A tendency in the change of the voltage value V yx  was similar to those seen in the first chirality detection experiment and the chirality discrimination experiments. 
     From the experimental results of the device E and the device F, it was found that it was possible to discriminate whether the insulating chiral material was right-handed or left-handed by examining the direction of the electromotive force generated in the chiral material. 
     The reason why the electromotive force was generated in the insulating chiral materials of the device E and the device F is thought to be as follows. When the voltage is applied to the Pt layer, a spin propagation is injected into the chiral material from the Pt layer due to the spin Hall effect, resulting in spin polarization in the chiral material. This spin polarization of the chiral material is thought to generate the electromotive force in the chiral material due to the inverse effect of the chirality inductive spin selectivity (CISS) effect. 
     Third Chirality Detection Experiment 
     A third chirality detection experiment was carried out using a chiral molecule dispersion solution, in which tartaric acid (chiral molecule) is dispersed, as a subject. 
       FIG. 18( a )  shows a photograph of a device G. For the device G, three platinum electrodes are provided on a glass substrate: To both ends of the upper platinum electrode, wirings (1) and (2) are connected, respectively; to both ends of the middle platinum electrode, wirings (3) and (4) are connected, respectively; and to both ends of the lower platinum electrode, wirings (5) and (6) are connected, respectively. The chiral molecule dispersion solution is dropped onto the substrate so that it overlaps the three platinum electrodes. 
     A voltage applied between the wirings (2) and (6) was changed so that an electric current (the electric current flowing from the upper platinum electrode to the lower platinum electrode) flowing through the chiral molecule dispersion solution of the device G would change from −100 μA to +100 μA, thereby measuring a voltage V between the wirings (3) and (4). 
     An electric current value when the electric current flows through the chiral molecule dispersion solution from the wiring (2) to the wiring (6) was set to be plus, and an electric current value when the electric current flows from the wiring (6) to the wiring (2) was set to be minus. 
     The voltage V was set to a plus voltage when an electric potential of the wiring (3) (which is on the right side when facing a direction of the plus electric current flowing through the chiral molecule dispersion solution) was higher than an electric potential of the wiring (4) (which is on the left side when facing the direction of the plus electric current flowing through the chiral molecule dispersion solution). 
       FIG. 18( b )  shows a graph showing a change in measured voltage value V. The voltage value V has changed depending upon the voltage applied between the wirings (2) and (6). The voltage value V became minus when the voltage was applied so that the plus electric current flowed through the chiral molecule dispersion solution, and became plus when the voltage was applied so that the minus electric current flowed through the chiral molecule dispersion solution. The voltage V and an electric current I flowing through the chiral molecule dispersion solution had a proportionality relation in which a proportionality constant was minus. 
     A tendency in the change of the voltage value V was similar to those seen in the first and the second chirality detection experiments and the chirality discrimination experiments. 
     REFERENCE SIGNS LIST 
       2 : chiral material layer 
       3   a,    3   b:  electrodes for voltage application 
       4  spin detection layer 
       5 ,  5   a,    5   b,    5   c:  power supply 
       6   a,    6   b,    6   c:  voltage measuring section 
       7 : control section 
       8   a,    8   b,    8   c:  electrodes for voltage detection 
       9 : subject 
       11 : chiral material-containing solution, liquid, or gas 
       12 : voltage application section 
       13 ,  13   a,    13   b:  magnetic field application section 
       15 : flow channel material 
       16 ,  16   a,    16   b:  flow channel 
       17 : right-handed chiral material 
       18 : left-handed chiral material 
       19 ,  19   a,    19   b:  coil 
       20 : chirality detector 
       25 : separator 
       26 : input section 
       27 : output section 
       30 : chiral material device