CN106816529A - A kind of application phase-change material as tunnel layer spin electric device - Google Patents

A kind of application phase-change material as tunnel layer spin electric device Download PDF

Info

Publication number
CN106816529A
CN106816529A CN201710047209.7A CN201710047209A CN106816529A CN 106816529 A CN106816529 A CN 106816529A CN 201710047209 A CN201710047209 A CN 201710047209A CN 106816529 A CN106816529 A CN 106816529A
Authority
CN
China
Prior art keywords
tunnel layer
spin
electric device
tunnel
change material
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201710047209.7A
Other languages
Chinese (zh)
Other versions
CN106816529B (en
Inventor
林晓阳
郭思德
赵巍胜
张有光
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Beihang University
Original Assignee
Beihang University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Beihang University filed Critical Beihang University
Priority to CN201710047209.7A priority Critical patent/CN106816529B/en
Publication of CN106816529A publication Critical patent/CN106816529A/en
Application granted granted Critical
Publication of CN106816529B publication Critical patent/CN106816529B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N70/00Solid-state devices having no potential barriers, and specially adapted for rectifying, amplifying, oscillating or switching
    • H10N70/20Multistable switching devices, e.g. memristors
    • H10N70/231Multistable switching devices, e.g. memristors based on solid-state phase change, e.g. between amorphous and crystalline phases, Ovshinsky effect
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N70/00Solid-state devices having no potential barriers, and specially adapted for rectifying, amplifying, oscillating or switching
    • H10N70/20Multistable switching devices, e.g. memristors
    • H10N70/257Multistable switching devices, e.g. memristors having switching assisted by radiation or particle beam, e.g. optically controlled devices

Landscapes

  • Hall/Mr Elements (AREA)

Abstract

The present invention relates to a kind of application phase-change material as tunnel layer spin electric device, specially a kind of non-local spia injector part, its bottom is spin raceway groove, outside two ends above the spin raceway groove respectively deposit a common metal electrode, spin raceway groove upper center deposits two tunnel layers, and respectively deposits a feeromagnetic metal electrode on the tunneling layer;It is characterized in that:Described tunnel layer is the material that can be undergone phase transition in the case where temperature and illumination drive;And the device has further included temperature control modules or illumination control module.Phase transformation tunnel layer (such as vanadium dioxide) proposed by the present invention, can control resistance with temperature and illumination.Tunneling resistance can be by artificial adjustment in suitable interval, so as to improve the performance of spin electric device.

Description

A kind of application phase-change material as tunnel layer spin electric device
【Technical field】
The present invention relates to a kind of application phase-change material as tunnel layer spin electric device, using the phase of tunnelling layer material Become and control tunnel layer resistance, and then regulate and control the tunnelling probability of spinning current, finally realize the regulation and control to spin electric device performance. The invention belongs to area of Spintronics.
【Background technology】
Spintronics mainly studies the characteristic and its control method of the spin free degree of electronics, by produce, regulation and control, it is defeated Fortune and detection spin current realize the electronic device of a new generation.By development for many years, spin electric device attracted scientific circles and The broad interest of industrial quarters, and have important application in multiple fields.
Spin electric device often contains high-resistance tunnel layer.The effect of tunnel layer can use quantum tunneling effect solution Release.The potential barrier that insulating barrier could be formed with higher-energy is inserted in quantum mechanics, between conductor or semiconductor, but energy is relatively low Electronics still has certain probability through potential barrier, and opposite side is reached from side, and the phenomenon is referred to as quantum tunneling effect, insulating barrier here Also referred to as tunnel layer.The tunnelling probability of electronics is relevant with the resistance sizes of tunnel layer, and the size of tunnelling probability can direct shadow Ring the performance of spin electric device.Tunnel layer resistance for example in spia injector part between ferromagnetic electrode and spin raceway groove can shadow Ring the efficiency of spin injection;And the tunnel layer resistance in magnetic tunnel device between two ferromagnetic layers can influence tunnel magneto.
Current transfer in spin injection and magnetic tunnel device all can be by feeromagnetic metal.There is the electricity of different spin directions Son has different charge velocities because the scattering strength in feeromagnetic metal is different, so as to the difference for having concentration and chemical potential. The electric current of skewness of this electronics in two spin directions etc. is referred to as spin polarized current.The product of spin polarized current Power that is raw, transporting and detect the signal that can all influence spin electric device.
Theory analysis shows, in non-local spia injector part, tunnel layer resistance between ferromagnetic electrode and spin raceway groove Spin Injection Efficiency will be influenceed.By taking Graphene spin raceway groove as an example, ratio between spin signals and contact resistance and channel resistance Relation is as shown in Figure 1.As can be seen that contact resistance only has and can just make within the specific limits the signal to have a higher value, and contact resistance Size is relevant with tunnel layer resistance, so the control of tunnel layer resistance needs precision higher, selection and tunnelling to material Thickness degree also has certain requirement;Similarly, in magnetic tunnel-junction, the resistance of tunnel layer can also influence dependency structure and device Performance.It can be seen that the control of tunnel layer resistance is significant for device performance.
Material using constant resistivity has problems with as tunnel layer:
1. to make tunnel layer resistance in scope needed for device, it is necessary to screen resistivity suitable material, and in tunnelling Precise thickness control during layer deposition, this improves selection and the difficulty for preparing.
2. the parameters of tunnel layer are fixed after the completion of device, it is impossible to regulated and controled when needed.
【The content of the invention】
First, goal of the invention:
Spin electric device limited performance caused by precise control is difficult to for the tunnel layer resistance mentioned in above-mentioned background The problem of system, the present invention proposes a kind of spin electric device of application phase-change material as tunnel layer, it is possible to use phase-change material (such as vanadium dioxide) is used as the adjustable tunnel layer of resistance.The characteristic of material phase transformation can be driven for temperature and illumination, by adding Enter temperature or illumination control module, adjust the phase structure of tunnel layer, change tunnel layer resistance and by resistance regulation and control in suitable interval It is interior, so as to realize the purpose of optimized device performance.
2nd, technical scheme:
The technical scheme is that realizing a kind of spin electric device of application phase-change material as tunnel layer.Specific In device, by controlling temperature or additional illumination, the phase transformation of driving tunnel layer, and then regulate and control the resistance of tunnel layer, it is final to realize The regulation and control of spin electric device performance.The present invention proposes two kinds of embodiments altogether.
Scheme one:Phase-change material (such as vanadium dioxide VO2) can be undergone phase transition with temperature change, produce the change of resistance Change.It is VO shown in Fig. 22The curve that varies with temperature of resistance.Temperature at tunnel layer can be adjusted by temperature control, entered And ensure tunnel layer resistance within the scope of required, it is ensured that the performance of device.
Scheme two:When additional illumination, phase-change material (such as vanadium dioxide VO2) can undergo phase transition, produce the change of resistance. It is VO shown in Fig. 32Resistance with illumination variation curve.The intensity of illumination that tunnel layer is subject to can be regulated and controled by light source control, And then ensure tunnel layer resistance within the scope of required, it is ensured that the performance of device.
A kind of application phase-change material of the present invention as tunnel layer spin electric device, specially a kind of non-local spin note Enter device, its bottom is spin raceway groove, the outside two ends above the spin raceway groove respectively deposit a common metal electrode, spin Raceway groove upper center deposits two tunnel layers, and respectively deposits a feeromagnetic metal electrode on the tunneling layer;It is characterized in that:It is described Tunnel layer be the material that can be undergone phase transition in the case where temperature and illumination drive;And the device has further included temperature control mould Block or illumination control module.
A kind of application phase-change material of the present invention as tunnel layer spin electric device, specially a kind of magnetic tunnel-junction device Part, its bottom is common metal electrode, ferromagnetic reference, tunnel layer and ferromagnetic free layer is sequentially depositing thereon, and go up most End one common metal electrode of deposition;It is characterized in that:Described tunnel layer is phase can occur in the case where temperature and illumination drive The material of change;And the device has further included temperature control modules or illumination control module.
Wherein, described temperature control modules, are the prefabricated grooves in a substrate, and temperature control modules are inserted into it In;Described temperature control modules are located at immediately below tunnel layer, and the wire of module is drawn by the space that groove is reserved, and is connected to In total moisture content control unit, so as to realize temperature adjustment.
Wherein, described illumination control module can be the light source for adjusting brightness, and being positioned over the side of tunnel layer (can be But it is not limited to the position in schematic diagram), and tunnelling layer surface is normally incident in as far as possible, the wire of light source is connected to total illumination control On unit processed, so as to realize brightness regulation.
The spin raceway groove, there is the material of certain spin diffusion length including metal, semiconductor, Graphene etc..
One kind in the common metal electrode, including golden (Au), platinum (Pt), copper (Cu) or other non-ferromagnetic metal materials Or it is various.
The ferromagnetic electrode, including barium ferrite (BAM), iron (Fe), cobalt (Co), nickel (Ni), ferro-cobalt boron (CoFeB), nickel One or more in iron (NiFe), lanthanum strontium manganese oxygen (LSMO), heusler alloy or other ferromagnetic materials.
The tunnel layer, including the various materials that can be undergone phase transition in the case where temperature and illumination drive, typical case such as titanium dioxide Vanadium (VO2)。
The ferromagnetic reference, including barium ferrite (BAM), iron (Fe), cobalt (Co), nickel (Ni), ferro-cobalt boron (CoFeB), One or more in ferronickel (NiFe), lanthanum strontium manganese oxygen (LSMO), heusler alloy or other ferromagnetic materials.
The ferromagnetic free layer, including cobalt (Co), ferro-cobalt (CoFe), ferro-cobalt boron (CoFeB), heusler alloy or other iron One or more in magnetic material.
The coercivity of ferromagnetic electrode directly determines the difficulty or ease of the direction of magnetization upset of electrode, and this is in spin electric device There is important application.Electrode material is different or size difference can make it have different coercivitys.Under certain external magnetic field, coercive The direction of magnetization of the small electrode of power first overturns, such that it is able to realize two equal states or opposite of the direction of magnetization of ferromagnetic electrode Conversion between state.Non-local spin injecting structure and magnetic tunnel-junction can in this way, using external magnetic field strength Change, realize the conversion in opposite magnetization direction between ferromagnetic electrode or ferromagnetic layer.In non-local spin injecting structure, for Position between two different electrodes of coercivity does not have strict regulations, can be that big coercivity electrode side is passed through electric current, Opposite side measures voltage;Can also be that small coercivity electrode side is passed through electric current in opposite side measurement voltage.Similarly, in magnetic channel In knot, there is no strict regulations for the position of ferromagnetic reference and ferromagnetic free layer, you being that ferromagnetic reference is in bottom Electrode top, then ferromagnetic free layer is below apex electrode;Can also be ferromagnetic free layer above bottom electrode, then ferromagnetic ginseng Layer is examined below apex electrode.
Wherein, a kind of application phase-change material as tunnel layer spin electric device, a kind of specially non-local spin note Enter device, prepared in substrate spin raceway groove using methods such as magnetron sputtering, electron-beam evaporation or mechanical strippings;Then By electron-beam evaporation tunnel layer, and ferromagnetic electrode is just plated by magnetron sputtering on the tunneling layer, finally by electron beam Evaporation deposits Au electrodes with speed on raceway groove., it is necessary to using photoetching, etching, embedding, deposition etc. in the preparation process of device Method realizes the graphical of device, and adds temperature or illumination control module in relevant position, is finally completed the preparation of device.If For control module is temperature control modules, then should in substrate prefabricated groove, and temperature control modules are inserted wherein.
Wherein, a kind of application phase-change material as tunnel layer spin electric device, specially a kind of magnetic tunnel device, By the methods such as magnetron sputtering or electron-beam evaporation be sequentially depositing on substrate bottom electrode, ferromagnetic reference, tunnel layer, Ferromagnetic free layer and apex electrode.In magnetic tunnel-junction preparation process, need to be realized using methods such as photoetching, etching, embedding, depositions Device it is graphical, while relevant position add temperature or illumination control module, so as to complete the preparation of device.If control Module is temperature control modules, then should in substrate prefabricated groove, and temperature control modules are inserted wherein.
3rd, advantage and effect:
Phase transformation tunnel layer (such as vanadium dioxide) proposed by the present invention, can control resistance with temperature and illumination.Tunneling resistance Can be by artificial adjustment in suitable interval, so as to improve the performance of spin electric device.
【Brief description of the drawings】
Fig. 1 is the relation of spin signals and contact resistance/spin values of channel resistance in the non-local spin injection of Graphene Schematic diagram.
Fig. 2 is VO2Resistance and temperature relation schematic diagram.
Fig. 3 is VO2Resistance and intensity of illumination relation schematic diagram.
Fig. 4 is the schematic diagram of the non-local spin injecting structure of temperature adjusting.
Fig. 5 is the schematic diagram of the non-local spin injecting structure of light regulating and controlling illumination.
Fig. 6 is the structural representation of magnetic tunnel-junction.
Fig. 7 is the structural representation of the magnetic tunnel-junction of temperature adjusting.
Fig. 8 is the structural representation of the magnetic tunnel-junction of light regulating and controlling illumination.
Label declaration in figure:
40 70 substrates
41 51 spin raceway grooves
42 43 52 53 common metal electrodes
44 45 54 55 63 73 83 tunnel layers
46 47 56 57 feeromagnetic metal electrodes
48 49 76 temperature control modules
58 59 86 illumination control modules
61 71 81 apex electrodes
62 72 82 ferromagnetic free layers
64 74 84 ferromagnetic references
65 75 85 bottom electrodes
【Specific embodiment】
The present invention proposes the tunnel layer that available phase transformation regulates and controls resistance.In non-local spin injecting structure instantiation, By regulating and controlling tunnel layer resistance, Spin Injection Efficiency is improve;In magnetic tunnel-junction instantiation, by regulating and controlling tunnel layer electricity Resistance, improves tunnel magneto.
Referring to the drawings, substantive distinguishing features of the invention are further illustrated.Accompanying drawing is schematic diagram, each function being directed to Layer or the non-actual size of thickness in region, the non-actual value of distance between functional areas, the electric current and magnitude of voltage in mode of operation are also non- Actual value.
Detailed exemplary embodiment is disclosed that, its specific CONSTRUCTED SPECIFICATION and function detail are only to represent description The purpose of example embodiment, therefore, it can implement the present invention in many selectable forms, and the present invention not it should be understood that It is all changes, the equivalence that are limited only to the example embodiment for herein proposing, but should cover fall within the scope of the present invention Thing and refill.
Fig. 4 show the structural representation of the non-local spia injector part of temperature adjusting.Structure includes:Substrate 40; Spin raceway groove 41, such as Graphene;Common metal electrode 42,43, such as golden (Au);Using the tunnel layer 44,45 of phase-change material, such as VO2;Feeromagnetic metal electrode 46,47, such as FeCo alloy;Temperature control modules 48,49.Temperature control modules 48,49 are respectively in base In two grooves in bottom 40, and the underface of 44 tunnel layers 44 and tunnel layer 45 is respectively at, the He of tunnel layer 44 can be adjusted The temperature of tunnel layer 45.Common metal electrode 42 and feeromagnetic metal electrode 46 are other end of by constant-current source control input electric current Detection voltage at feeromagnetic metal electrode 47 and common metal electrode 43.Because ferromagnetic electrode is to the electricity of the electronics of different spin directions Lead variant, cause in feeromagnetic metal electrode 46 two kinds of electron injection speed of spin direction when by electric current, so that Spin polarization is formed in feeromagnetic metal base part.Because two concentration of the electronics of spin direction are different, therefore both chemistry Gesture is also.The two different chemical potentials are by the drift in the raceway groove that spins and are diffused in below feeromagnetic metal electrode 47 still Certain difference is kept, is detected by feeromagnetic metal, be embodied between feeromagnetic metal electrode 47 and common metal electrode 43 There is electrical potential difference.The ratio of the input current of the electrical potential difference and feeromagnetic metal electrode 46 is defined as R.Changing external magnetic field can use two The direction of magnetization of ferromagnetic electrode is in parallel or antiparallel state, and measurement obtains different R, and spin signals are then defined as Δ R/R. Theory analysis shows that, when the contact resistance that tunnel layer is obtained is in certain interval, spin signals Δ R/R can reach maximum Value, realizes the optimization of device.And two temperature control modules 48,49 regulate and control two phase transformations of tunnel layer, tunnel layer can be made Resistance to be in this interval, it is ensured that device has the spin signals of maximum all the time.
Fig. 5 show the structural representation of the non-local spia injector part of light regulating and controlling illumination.Concrete structure includes:It is spin Raceway groove 51, such as Graphene;Common metal electrode 52,53, such as golden (Au);Using the tunnel layer 54,55 of phase-change material, such as titanium dioxide Vanadium (VO2);Feeromagnetic metal electrode 56,57, such as FeCo alloy;Illumination control module 58,59.Two illumination control modules 58,59 The light for sending focuses on the side of tunnel layer 54 and tunnel layer 55 respectively, and the illumination of regulation tunnel layer 54 and tunnel layer 55 is strong Degree.Common metal electrode 52 and feeromagnetic metal electrode 56 are electric in other end of feeromagnetic metal by constant-current source control input electric current Detection voltage at pole 57 and common metal electrode 53.According to temperature control identical principle, when illumination control module adjust tunnel Wearing layer intensity of illumination makes the resistance of tunnel layer be in when in suitable interval, and device can be made to have the spin signals of maximum.
Fig. 6 is the structural representation of magnetic tunnel-junction.Including:The apex electrode 61 of common metal composition, such as golden (Au);It is ferromagnetic Free layer 62, such as cobalt (Co);Using the tunnel layer 63 of phase-change material, such as vanadium dioxide (VO2);Ferromagnetic reference 64, such as ferro-cobalt Boron (CoFeB);The bottom electrode 65 of common metal composition, such as golden (Au).
Fig. 7 is the structural representation of the magnetic tunnel device of temperature adjusting, has used magnetic tunneling junction shown in Fig. 6.Structure Including:Substrate 70;The apex electrode 71 of common metal composition, such as golden (Au);Ferromagnetic free layer 72, such as cobalt (Co);Use phase transformation The tunnel layer 73 of material, such as vanadium dioxide (VO2);Ferromagnetic reference 74, such as ferro-cobalt boron (CoFeB);The bottom of common metal composition Termination electrode 75, such as golden (Au).Temperature control modules 76 are in the groove of substrate 70, and the underface in device, for controlling The temperature of tunnel layer 73.Constant-current source control electric current is injected from apex electrode 71, is flowed out at bottom electrode 75, voltmeter measurement two The voltage at end.When ferromagnetic free layer is identical with the reference layer direction of magnetization, voltage and current ratio R is obtained;Change the bars such as external magnetic field During part, the direction of magnetization of ferromagnetic reference is constant, and the direction of magnetization of ferromagnetic free layer produces upset, between ferromagnetic reference When relative orientation turns into antiparallel, different R are obtained, knots modification is Δ R, tunnels through magnetic resistance and is defined as Δ R/R.By to tunnelling The regulation and control of the temperature of layer 73, change tunnel layer resistance, so as to regulate and control electron tunneling probability, can make the absolute value of signal delta R/R Maximum is reached, the optimization of device performance is realized.
Fig. 8 is the structural representation of the magnetic tunnel-junction of light regulating and controlling illumination, has used magnetic tunneling junction shown in Fig. 6.Structure includes: The apex electrode 81 of common metal composition, such as golden (Au);Ferromagnetic free layer 82, such as cobalt (Co);Use the tunnel layer of phase-change material 83, such as vanadium dioxide (VO2);Ferromagnetic reference 84, such as ferro-cobalt boron (CoFeB);The bottom electrode 85 of common metal composition, such as gold (Au).The light focusing that illumination control module 86 sends adjusts the intensity of illumination suffered by it on tunnel layer 83.By to illumination The regulation of intensity, using the magnetic tunnel-junction identical principle with temperature adjusting, can be such that the absolute value of signal delta R/R reaches most Greatly, the optimization of device performance is realized.

Claims (10)

1. a kind of application phase-change material as tunnel layer spin electric device, specially a kind of non-local spia injector part, Its bottom is spin raceway groove, and the outside two ends above the spin raceway groove respectively deposit a common metal electrode, on spin raceway groove Side middle part two tunnel layers of deposition, and a feeromagnetic metal electrode is respectively deposited on the tunneling layer;It is characterized in that:Described tunnelling Layer is the material that can be undergone phase transition in the case where temperature and illumination drive;And the device has further included temperature control modules or light According to control module.
2. a kind of application phase-change material as tunnel layer spin electric device, specially a kind of magnetic tunnel device, its most under It is common metal electrode to hold, and ferromagnetic reference, tunnel layer and ferromagnetic free layer is sequentially depositing thereon, and deposit one in the top Common metal electrode;It is characterized in that:Described tunnel layer is the material that can be undergone phase transition in the case where temperature and illumination drive;And The device has further included temperature control modules or illumination control module.
3. a kind of application phase-change material according to claim 1 and 2 as tunnel layer spin electric device, its feature exists In:Described temperature control modules, are the prefabricated grooves in a substrate, and temperature control modules are inserted wherein;Described temperature Degree control module is located at immediately below tunnel layer, and the wire of module is drawn by the space that groove is reserved, and is connected to total moisture content control On unit, so as to realize temperature adjustment.
4. a kind of application phase-change material according to claim 1 and 2 as tunnel layer spin electric device, its feature exists In:Described illumination control module can be the light source for adjusting brightness, be positioned over the side of tunnel layer, and vertical incidence as far as possible In tunnelling layer surface, the wire of light source is connected on total lighting control unit, so as to realize brightness regulation.
5. a kind of application phase-change material according to claim 1 as tunnel layer spin electric device, it is characterised in that: The spin raceway groove, there is the material of certain spin diffusion length including metal, semiconductor, Graphene etc..
6. a kind of application phase-change material according to claim 1 as tunnel layer spin electric device, it is characterised in that: The common metal electrode, one or more in including but not limited to golden (Au), platinum (Pt), copper (Cu).
7. a kind of application phase-change material according to claim 1 as tunnel layer spin electric device, it is characterised in that: The feeromagnetic metal electrode, including but not limited to barium ferrite (BAM), iron (Fe), cobalt (Co), nickel (Ni), ferro-cobalt boron (CoFeB), one or more in ferronickel (NiFe), lanthanum strontium manganese oxygen (LSMO), heusler alloy.
8. a kind of application phase-change material according to claim 1 and 2 as tunnel layer spin electric device, its feature exists In:The tunnel layer includes but is not limited to vanadium dioxide (VO2)。
9. a kind of application phase-change material according to claim 2 as tunnel layer spin electric device, it is characterised in that: The ferromagnetic reference, including but not limited to barium ferrite (BAM), iron (Fe), cobalt (Co), nickel (Ni), ferro-cobalt boron (CoFeB), One or more in ferronickel (NiFe), lanthanum strontium manganese oxygen (LSMO), heusler alloy.
10. a kind of application phase-change material according to claim 2 as tunnel layer spin electric device, its feature exists In:In the ferromagnetic free layer, including but not limited to cobalt (Co), ferro-cobalt (CoFe), ferro-cobalt boron (CoFeB), heusler alloy One or more.
CN201710047209.7A 2017-01-22 2017-01-22 A kind of spin electric device using phase-change material as tunnel layer Active CN106816529B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710047209.7A CN106816529B (en) 2017-01-22 2017-01-22 A kind of spin electric device using phase-change material as tunnel layer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710047209.7A CN106816529B (en) 2017-01-22 2017-01-22 A kind of spin electric device using phase-change material as tunnel layer

Publications (2)

Publication Number Publication Date
CN106816529A true CN106816529A (en) 2017-06-09
CN106816529B CN106816529B (en) 2019-01-29

Family

ID=59111292

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710047209.7A Active CN106816529B (en) 2017-01-22 2017-01-22 A kind of spin electric device using phase-change material as tunnel layer

Country Status (1)

Country Link
CN (1) CN106816529B (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109524459A (en) * 2018-09-17 2019-03-26 北京应用物理与计算数学研究所 The controllable spinning current filter of polarization direction based on chromium triiodide
CN109888088A (en) * 2019-03-01 2019-06-14 西安交通大学 A kind of fabrication of magnetoresistance sensor structure and its manufacturing method
CN111681691A (en) * 2020-05-28 2020-09-18 北京航空航天大学 Phase change assisted disk media, disks, devices and methods
CN111883641A (en) * 2020-07-22 2020-11-03 北京大学 Room temperature heat-induced spin polarization current source and implementation method thereof

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20130229866A1 (en) * 2009-10-20 2013-09-05 Avalanche Technology, Inc. Spin-transfer torque magnetic random access memory (sttmram) using a synthetic free layer
CN104813472A (en) * 2012-12-21 2015-07-29 英特尔公司 Perpendicular Spin Transfer Torque Memory (STTM) devices with enhanced stability and methods of forming the same
CN105304812A (en) * 2015-06-08 2016-02-03 清华大学 Phase-change spinning nonvolatile storage unit
CN105745760A (en) * 2013-11-20 2016-07-06 Tdk株式会社 Magnetoresistive element, Spin-MOSFET, magnetic sensor, and magnetic head

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20130229866A1 (en) * 2009-10-20 2013-09-05 Avalanche Technology, Inc. Spin-transfer torque magnetic random access memory (sttmram) using a synthetic free layer
CN104813472A (en) * 2012-12-21 2015-07-29 英特尔公司 Perpendicular Spin Transfer Torque Memory (STTM) devices with enhanced stability and methods of forming the same
CN105745760A (en) * 2013-11-20 2016-07-06 Tdk株式会社 Magnetoresistive element, Spin-MOSFET, magnetic sensor, and magnetic head
CN105304812A (en) * 2015-06-08 2016-02-03 清华大学 Phase-change spinning nonvolatile storage unit

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
ADAM L. FRIEDMAN, ET AL.: "Hydrogenated Graphene as a Homoepitaxial Tunnel Barrier for Spin and Charge Transport in Graphene", 《ACS NANO》 *

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109524459A (en) * 2018-09-17 2019-03-26 北京应用物理与计算数学研究所 The controllable spinning current filter of polarization direction based on chromium triiodide
CN109524459B (en) * 2018-09-17 2019-10-08 北京应用物理与计算数学研究所 The controllable spinning current filter of polarization direction based on chromium triiodide
CN109888088A (en) * 2019-03-01 2019-06-14 西安交通大学 A kind of fabrication of magnetoresistance sensor structure and its manufacturing method
CN111681691A (en) * 2020-05-28 2020-09-18 北京航空航天大学 Phase change assisted disk media, disks, devices and methods
CN111883641A (en) * 2020-07-22 2020-11-03 北京大学 Room temperature heat-induced spin polarization current source and implementation method thereof
CN111883641B (en) * 2020-07-22 2022-01-28 北京大学 Room temperature heat-induced spin polarization current source and implementation method thereof

Also Published As

Publication number Publication date
CN106816529B (en) 2019-01-29

Similar Documents

Publication Publication Date Title
CN106816529B (en) A kind of spin electric device using phase-change material as tunnel layer
Spaldin et al. Multiferroics: Past, present, and future
US8269293B2 (en) Spin transistor and method of operating the same
Nozaki et al. Quantum oscillation of the tunneling conductance in fully epitaxial double barrier magnetic tunnel junctions
CN100390561C (en) Semiconductor element comprising semimagnetic contact
CN102637939B (en) Spinning microwave oscillator based on vertical magnetizing free layer and manufacturing method thereof
US11937513B2 (en) Magnon spin valve, magnon sensor, magnon field effect transistor, magnon tunnel junction and magnon memory
Häfner et al. Theoretical study of the conductance of ferromagnetic atomic-sized contacts
Łączkowski et al. Spin signal in metallic lateral spin valves made by a multiple angle evaporation technique
US8012771B2 (en) Method for manufacturing magnetic field detection devices and devices therefrom
Peng et al. Characteristic tunnel-type conductivity and magnetoresistance in a CoO-coated monodispersive Co cluster assembly
Mandal et al. High-field magnetotransport properties of La 2/3 Sr 1/3 MnO 3 and Nd 2/3 Sr 1/3 MnO 3 systems
US9245923B2 (en) Method of fabricating a semiconductor device having a colossal magneto-capacitive material being formed close to a channel region of a transistor
Hong et al. A multifunctional molecular spintronic platform with magnetoresistive and memristive responses via a self-assembled monolayer
Deac et al. Current driven resistance changes in low resistance x area magnetic tunnel junctions with ultra-thin Al-Ox barriers
CN1742376A (en) High performance spin-valve transistor
CN106328805A (en) Magnetic tunnel junction with quantum effect, and spin diode and spin transistor comprising magnetic tunnel junction
CN104269493B (en) Organic single-crystal spinning diode and manufacturing method thereof
CN105470116B (en) A method of regulation dilute magnetic semiconductor material room temperature magnetism
Volkov et al. Magneto-transport phenomena in metal/SiO2/n (p)-Si hybrid structures
CN106876395A (en) A kind of spin electric device that tunnel layer is made of resistive material
CN106449738B (en) A kind of coaxial spia injector part
Krivoruchko et al. Subgap magnetotransport in Pb/LaCaMnO point contacts
CN104241335B (en) A kind of zno-based magnetism pn-junction and preparation method thereof with spin rectification characteristic
Volkov et al. Switching of current channels and new mechanism of magnetoresistance in a tunneling structure

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant