CN111740005A - High-temperature polarization method for piezoelectric film - Google Patents

High-temperature polarization method for piezoelectric film Download PDF

Info

Publication number
CN111740005A
CN111740005A CN202010553392.XA CN202010553392A CN111740005A CN 111740005 A CN111740005 A CN 111740005A CN 202010553392 A CN202010553392 A CN 202010553392A CN 111740005 A CN111740005 A CN 111740005A
Authority
CN
China
Prior art keywords
change material
piezoelectric
temperature
substrate
phase change
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
CN202010553392.XA
Other languages
Chinese (zh)
Other versions
CN111740005B (en
Inventor
黄凯
欧欣
赵晓蒙
李忠旭
陈阳
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.)
Shanghai Xinsi Polymer Semiconductor Co ltd
Original Assignee
Shanghai Institute of Microsystem and Information Technology of CAS
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 Shanghai Institute of Microsystem and Information Technology of CAS filed Critical Shanghai Institute of Microsystem and Information Technology of CAS
Priority to CN202010553392.XA priority Critical patent/CN111740005B/en
Publication of CN111740005A publication Critical patent/CN111740005A/en
Application granted granted Critical
Publication of CN111740005B publication Critical patent/CN111740005B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N30/00Piezoelectric or electrostrictive devices
    • H10N30/01Manufacture or treatment
    • H10N30/04Treatments to modify a piezoelectric or electrostrictive property, e.g. polarisation characteristics, vibration characteristics or mode tuning
    • H10N30/045Treatments to modify a piezoelectric or electrostrictive property, e.g. polarisation characteristics, vibration characteristics or mode tuning by polarising
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N30/00Piezoelectric or electrostrictive devices
    • H10N30/01Manufacture or treatment
    • H10N30/06Forming electrodes or interconnections, e.g. leads or terminals
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N30/00Piezoelectric or electrostrictive devices
    • H10N30/80Constructional details
    • H10N30/87Electrodes or interconnections, e.g. leads or terminals
    • H10N30/877Conductive materials
    • H10N30/878Conductive materials the principal material being non-metallic, e.g. oxide or carbon based

Landscapes

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)
  • Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)

Abstract

The invention relates to a high-temperature polarization method of a piezoelectric film, which comprises the following steps: preparing a composite structure of the piezoelectric film, the thermotropic phase change material and the support substrate; then, carrying out high-temperature annealing on the composite structure, and applying a polarization electric field on the piezoelectric film by taking the thermotropic phase change material as a bottom electrode; and finally, carrying out surface treatment on the polarized piezoelectric film. According to the invention, by introducing the phase-change material, on one hand, the phase-change material is metallized at the annealing temperature and is used as a bottom electrode to apply polarization voltage, so that the polarization consistency of the piezoelectric film can be improved; on the other hand, the phase-change material is insulated at the working temperature of the device and can be used as a high-resistance isolation layer to improve the radio-frequency performance of the piezoelectric device.

Description

High-temperature polarization method for piezoelectric film
Technical Field
The invention belongs to the field of electronic components, and particularly relates to a high-temperature polarization method for a piezoelectric film.
Background
With the development of 5G technology, the market of radio frequency front end modules of mobile communication terminals has rapidly increased. Acoustic wave filters based on surface acoustic wave and bulk acoustic wave technologies have become the fastest growing electronic components in radio frequency front end modules. However, with the release of new frequency bands and the application of Carrier Aggregation (CA) and Multiple Input Multiple Output (MIMO) technologies, the market places more demands on the size, power consumption, power, operating frequency, bandwidth, stability, and the like of the acoustic wave filter. Therefore, on the basis of the traditional acoustic wave filter based on the piezoelectric single crystal substrate, researchers adopt a heterogeneous composite substrate to improve the performance of the device and develop a novel working mode. However, at present, heterogeneous composite substrates for high-performance surface acoustic wave filters are prepared by ion beam stripping technology, and the prepared thin films have a large number of implantation defects, so that the piezoelectric thin films are multi-domain. In order to recover the defects, high-temperature annealing is generally adopted for defect recovery, however, the coercive electric field of the piezoelectric material is reduced along with the increase of the temperature, and multiple piezoelectric domains are easily generated due to the existence of a disturbing electric field in the annealing process. In addition, the traditional polarization method is easy to introduce the problems of air breakdown or uneven polarization of electrode contact points and the like.
Disclosure of Invention
The technical problem to be solved by the invention is to provide a piezoelectric film high-temperature polarization method, which is characterized in that a phase-change material is introduced, on one hand, the phase-change material is metalized at an annealing temperature and is used as a bottom electrode to apply polarization voltage, so that the polarization consistency of the piezoelectric film can be improved; on the other hand, the phase-change material is insulated at the working temperature of the device and can be used as a high-resistance isolation layer to improve the radio-frequency performance of the piezoelectric device.
The invention provides a high-temperature polarization method of a piezoelectric film, which comprises the following steps:
preparing a composite structure of the piezoelectric film, the thermotropic phase change material and the supporting substrate by using an ion implantation and heterogeneous bonding process; then, carrying out high-temperature annealing on the composite structure, and applying a polarization electric field on the piezoelectric film by taking the thermotropic phase change material as a bottom electrode; and finally, carrying out surface treatment on the polarized piezoelectric film.
The piezoelectric film is a lithium niobate or lithium tantalate film.
The metal/insulation transition temperature of the thermotropic phase change material is more than 70 ℃; the polarization temperature is between the metal/insulation transition temperature and 0.8 Tc; the resistivity of the insulating phase is more than 1000 omega cm. The required transition temperature (Tc is the Curie temperature of the piezoelectric film) is more than 70 ℃, and the phase-change material can be ensured to keep an insulating phase, namely a high-resistance state at the normal working temperature of the device. The phase transition temperature of part of the material is lower than 70 ℃, and the phase transition temperature can be regulated and controlled by adopting ion doping, strain doping, hole regulation and the like.
The support substrate is made of silicon, sapphire and SiO2One or more of a/Si composite substrate, SiC, GaN and AlN.
The ion implantation and heterogeneous bonding process comprises the steps of firstly growing a thermotropic phase change material (such as magnetron sputtering, PLD, ALD and the like) on the surface of a piezoelectric substrate, then implanting ions into the piezoelectric substrate, finally bonding a support substrate and the piezoelectric substrate, or firstly implanting ions into the piezoelectric substrate, then growing the thermotropic phase change material on the surface of the piezoelectric substrate, and finally bonding the support substrate and the piezoelectric substrate.
A stop layer is grown in advance before the thermotropic phase change material is grown on the surface of the piezoelectric substrate. The cut-off layer is SiO2Although the phase change material is not in contact with the piezoelectric substrate at this time, polarization may be performed by an electric field.
The high-temperature annealing temperature is 0.3-1.2 Tc.
The intensity of the polarized electric field is larger than the coercive electric field of the thermotropic phase change material, and the polarization time is larger than 1 s.
For a radio frequency filter, metal structures such as interdigital electrodes, bus lines and contact electrode plates are formed on the upper surface of the piezoelectric film. If the material under the piezoelectric film layer is a low-resistance material, the low-resistance material can play a role of an electrode, and the low-resistance material, the metal structure on the surface of the piezoelectric film and the piezoelectric film form a capacitor structure to influence the performance of the radio frequency filter.
The phase-change material can be used as a high-resistance isolation layer to improve the radio-frequency performance of the piezoelectric device.
Figure 2 shows the effect of high and low resistivity on the resonant performance of the device, comparing two materials with resistivity of 1e5ohm cm and 0.05ohm cm respectively. The resonance frequency points of the high-resistance substrate and the low-resistance substrate are close to each other and are positioned at about fr 2010 MHz. However, the anti-resonance point of the low-resistance substrate is located at fa of 2198MHz, and the anti-resonance point of the high-resistance substrate is located at fa of 2284 MHz. According to a calculation formula
Figure BDA0002543311470000021
Calculating the electromechanical coupling coefficient of resonance performance, kt of high-resistance substrate235.6%, kt of low-resistance substrate224.7%. The electromechanical coupling coefficient directly influences the relative bandwidth of the resonator, and the read bandwidth of the high-resistance substrate is superior to that of the low-resistance substrate.
Advantageous effects
According to the invention, by introducing the phase-change material, on one hand, the phase-change material is metallized at the annealing temperature and is used as a bottom electrode to apply polarization voltage, so that the polarization consistency of the piezoelectric film can be improved; on the other hand, the phase-change material is insulated at the working temperature of the device and can be used as a high-resistance isolation layer to improve the radio-frequency performance of the piezoelectric device.
Drawings
FIG. 1 is a schematic diagram of the introduction of phase change materials in accordance with the present invention.
Fig. 2 is a graph showing the effect of high and low resistance materials on the resonant performance of the device.
Detailed Description
The invention will be further illustrated with reference to the following specific examples. It should be understood that these examples are for illustrative purposes only and are not intended to limit the scope of the present invention. Further, it should be understood that various changes or modifications of the present invention may be made by those skilled in the art after reading the teaching of the present invention, and such equivalents may fall within the scope of the present invention as defined in the appended claims.
Example 1
(1) Firstly, a thermotropic phase change material such as VO is grown on the surface of a supporting substrate2Or TiO2(growth method such as magnetron sputtering, PLD, ALD, etc.), then implanting ions such as H ions into the piezoelectric substrate, and bringing the support substrate into contact with pressureBonding the electric thin film and annealing and stripping the piezoelectric material to obtain a composite structure of the piezoelectric thin film, the thermotropic phase change material and the silicon substrate; wherein [3D Local structural of the Metal-Insulator transformation in VO2Thin Film by Defect-InducedLattice Engineering]It is stated that VO increases with temperature2The sheet resistance is reduced from 10^5 to 10^1 by changing from the insulating state to the metal state;
(2) and (3) carrying out high-temperature annealing on the composite structure, wherein the high-temperature annealing temperature is 1.1Tc, so that the bonding strength between the piezoelectric film and the support substrate is enhanced on one hand, and the residual defects of ion implantation can be recovered on the other hand. Theoretically, the higher the temperature, the stronger the bond strength and the better the residual defect recovery. When the temperature exceeds the Curie temperature of the piezoelectric material, the piezoelectric material is changed from ferroelectric to paraelectric, and the piezoelectric performance is lost; with the increase of the temperature, the coercive electric field of the piezoelectric material is reduced, and the polarization of the piezoelectric material is easily influenced by an external electric field;
(3) the thermotropic phase change material is used as a bottom electrode, a polarization electric field is applied to the piezoelectric film, so that the piezoelectric film is polarized, the polarization temperature at the moment is higher than the MIT (Metal-Insulator transition) temperature of the thermotropic phase change material, and the piezoelectric material used as the bottom electrode has small resistivity and high efficiency;
(4) and finally, carrying out surface treatment on the polarized piezoelectric film to remove surface metal.
Example 2
(1) Firstly growing SiO of cut-off layer on the surface of lithium niobate piezoelectric film in advance2Then, thermally induced phase change material is grown again (growth method such as magnetron sputtering, PLD, ALD and the like), ions are implanted into the piezoelectric substrate, the piezoelectric substrate and the supporting substrate are bonded and annealed and peeled off to obtain a piezoelectric film and SiO2The thermotropic phase change material and the silicon substrate are in a composite structure;
(2) carrying out high-temperature annealing on the composite structure, wherein the high-temperature annealing temperature is 0.5 Tc;
(3) the thermotropic phase change material is used as a bottom electrode, and a polarization electric field is applied to the piezoelectric film, so that the piezoelectric film is polarized; since the polarization is the coercive field, at the bottomSiO is inserted between the electrode phase-change material and the piezoelectric film2After the layer, exert the electric field between bottom electrode and surface electrode and still can play the polarization, efficiency can reduce, but can do benefit to the performance promotion of device normal work.
(4) And finally, carrying out surface treatment on the polarized piezoelectric film to remove surface metal.
Example 3
In this embodiment, a silicon substrate is doped to change silicon into a thermotropic phase change material.
Growing SiO on the surface of a silicon substrate by thermal oxidation or film deposition (CVD or magnetron sputtering)2And implanting Te ions into the silicon substrate to convert the silicon layer containing Te component into phase change material. The piezoelectric film is then transferred to silicon/Te-containing silicon/SiO by ion beam lift-off2The material is formed on a support substrate. Annealing, polarization, and surface treatment were performed according to example 1.
Example 4
This example is for LiNbO3Doping is performed to convert the LN underlayer portion to a phase change material.
(1) Preparation of LN/SiO according to the Normal procedure of ion Beam stripping2The structure of the silicon-aluminum alloy/Si,
(2) implanting an element such as (CoFeB) into the LN thin film to form a CoFeB-containing LN layer located on the LN/SiO thin film2Composition of 1/4, CoFeB, in the upper part of the interface, with a thickness not exceeding the LN thickness<50 percent. Form LN/(CoFeB) LN/SiO2a/Si structure in which the (CoFeB) LN layer is a phase change material.
(3) Annealing, polarization, and surface treatment were performed according to example 1.

Claims (10)

1. A piezoelectric thin film high temperature polarization method comprises:
preparing a composite structure of the piezoelectric film, the thermotropic phase change material and the supporting substrate by using an ion implantation and heterogeneous bonding process; then, carrying out high-temperature annealing on the composite structure, taking the thermotropic phase change material as a bottom electrode, and applying a polarization electric field on the piezoelectric film; and finally, carrying out surface treatment on the polarized piezoelectric film.
2. The method of claim 1, wherein: the piezoelectric film is a lithium niobate or lithium tantalate film.
3. The method of claim 1, wherein: the metal/insulation transition temperature of the thermotropic phase change material is more than 70 ℃; the polarization temperature is between the metal/insulation transition temperature and 0.8 Tc; the resistivity of the insulating phase is more than 1000 omega cm.
4. The method of claim 1, wherein: the support substrate is made of silicon, sapphire and SiO2One or more of a/Si composite substrate, SiC, GaN and AlN.
5. The method of claim 1, wherein: the ion implantation and heterogeneous bonding process comprises the steps of firstly growing a thermotropic phase change material on the surface of a piezoelectric substrate, then implanting ions into the piezoelectric substrate, finally bonding a support substrate and the piezoelectric substrate, or firstly implanting ions into the piezoelectric substrate, then growing the thermotropic phase change material on the surface of the piezoelectric substrate, and finally bonding the support substrate and the piezoelectric substrate.
6. The method of claim 5, wherein: a stop layer is grown in advance before the thermotropic phase change material is grown on the surface of the piezoelectric substrate.
7. The method of claim 6, wherein: the cut-off layer is SiO2
8. The method of claim 1, wherein: the high-temperature annealing temperature is 0.3-1.2 Tc.
9. The method of claim 1, wherein: the surface treatment is to remove surface metal.
10. The method of claim 1, wherein: the intensity of the polarized electric field is larger than the coercive electric field of the thermotropic phase change material, and the polarization time is larger than 1 s.
CN202010553392.XA 2020-06-17 2020-06-17 High-temperature polarization method for piezoelectric film Active CN111740005B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202010553392.XA CN111740005B (en) 2020-06-17 2020-06-17 High-temperature polarization method for piezoelectric film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202010553392.XA CN111740005B (en) 2020-06-17 2020-06-17 High-temperature polarization method for piezoelectric film

Publications (2)

Publication Number Publication Date
CN111740005A true CN111740005A (en) 2020-10-02
CN111740005B CN111740005B (en) 2022-05-24

Family

ID=72649510

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202010553392.XA Active CN111740005B (en) 2020-06-17 2020-06-17 High-temperature polarization method for piezoelectric film

Country Status (1)

Country Link
CN (1) CN111740005B (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113314346A (en) * 2021-06-07 2021-08-27 通号(北京)轨道工业集团有限公司轨道交通技术研究院 Variable capacitance capacitor
CN114277443A (en) * 2021-12-28 2022-04-05 中国科学院苏州纳米技术与纳米仿生研究所 Nitride single crystal film, and preparation method and application thereof

Citations (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4019074A (en) * 1974-10-07 1977-04-19 Tokyo Shibaura Electric Co., Ltd. LiNbO3 saw device
US4405402A (en) * 1979-10-12 1983-09-20 The Marconi Company Limited Piezoelectric/pyroelectric elements
CN1447455A (en) * 2002-03-25 2003-10-08 小川敏夫 Domain controlled piezoelectric monocrystal component and its mfg. method
JP2005093133A (en) * 2003-09-12 2005-04-07 Tomoshi Wada Ferroelectric crystal material and its manufacturing method
CN101009354A (en) * 2006-12-22 2007-08-01 上海师范大学 A temperature inductive reversible phase transition iron electrical film
US20080266930A1 (en) * 2007-04-24 2008-10-30 Uchicago Argonne, Llc Piezoelectrically actuated ultrananocrystalline diamond tip array integrated with ferroelectric or phase change media for high-density memory
US20090307885A1 (en) * 2008-06-17 2009-12-17 Yasukazu Nihei Piezoelectric film poling method and piezoelectric element structure manufacturing method
CN101805182A (en) * 2010-02-09 2010-08-18 上海师范大学 Zirconium-rich lead zirconate-titanate ferroelectric (high-temperature) -ferroelectric (low temperture) phase change film material and preparation method thereof
US20110175047A1 (en) * 2008-11-26 2011-07-21 President And Fellows Of Harvard College Electric field induced phase transitions and dynamic tuning of the properties of oxide structures
CN103403804A (en) * 2010-12-10 2013-11-20 国际商业机器公司 Phase change material cell with piezoelectric or ferroelectric stress inducer liner
US20150083196A1 (en) * 2013-09-25 2015-03-26 Prime Photonics, Lc Magneto-thermoelectric generator for energy harvesting
CN110204754A (en) * 2019-06-05 2019-09-06 东南大学 A kind of preparation method of the high phase transition temperature composite piezoelectric material of fluoro
CN110474616A (en) * 2019-08-29 2019-11-19 华南理工大学 A kind of air-gap type thin film bulk acoustic wave resonator and preparation method thereof

Patent Citations (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4019074A (en) * 1974-10-07 1977-04-19 Tokyo Shibaura Electric Co., Ltd. LiNbO3 saw device
US4405402A (en) * 1979-10-12 1983-09-20 The Marconi Company Limited Piezoelectric/pyroelectric elements
CN1447455A (en) * 2002-03-25 2003-10-08 小川敏夫 Domain controlled piezoelectric monocrystal component and its mfg. method
JP2005093133A (en) * 2003-09-12 2005-04-07 Tomoshi Wada Ferroelectric crystal material and its manufacturing method
CN101009354A (en) * 2006-12-22 2007-08-01 上海师范大学 A temperature inductive reversible phase transition iron electrical film
US20080266930A1 (en) * 2007-04-24 2008-10-30 Uchicago Argonne, Llc Piezoelectrically actuated ultrananocrystalline diamond tip array integrated with ferroelectric or phase change media for high-density memory
US20090307885A1 (en) * 2008-06-17 2009-12-17 Yasukazu Nihei Piezoelectric film poling method and piezoelectric element structure manufacturing method
US20110175047A1 (en) * 2008-11-26 2011-07-21 President And Fellows Of Harvard College Electric field induced phase transitions and dynamic tuning of the properties of oxide structures
CN101805182A (en) * 2010-02-09 2010-08-18 上海师范大学 Zirconium-rich lead zirconate-titanate ferroelectric (high-temperature) -ferroelectric (low temperture) phase change film material and preparation method thereof
CN103403804A (en) * 2010-12-10 2013-11-20 国际商业机器公司 Phase change material cell with piezoelectric or ferroelectric stress inducer liner
US20150083196A1 (en) * 2013-09-25 2015-03-26 Prime Photonics, Lc Magneto-thermoelectric generator for energy harvesting
CN110204754A (en) * 2019-06-05 2019-09-06 东南大学 A kind of preparation method of the high phase transition temperature composite piezoelectric material of fluoro
CN110474616A (en) * 2019-08-29 2019-11-19 华南理工大学 A kind of air-gap type thin film bulk acoustic wave resonator and preparation method thereof

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
CHAO HE: "self-polarized high piezoelectricity and its memory effect in ferroelectric single crystals", 《ACTA MATERIAL》 *
KEIKO KOGA等: "crystallization,field-induced phase transformation,thermally induce phase transition, and piezoelectric activity in p(vinylidene fluoride-TrFE) copolymers with high molar content of vinylidene fluoride", 《JOURNAL OF APPLIED PHYSICS》 *

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113314346A (en) * 2021-06-07 2021-08-27 通号(北京)轨道工业集团有限公司轨道交通技术研究院 Variable capacitance capacitor
CN114277443A (en) * 2021-12-28 2022-04-05 中国科学院苏州纳米技术与纳米仿生研究所 Nitride single crystal film, and preparation method and application thereof

Also Published As

Publication number Publication date
CN111740005B (en) 2022-05-24

Similar Documents

Publication Publication Date Title
CN107342748B (en) Bulk acoustic wave resonator based on single crystal piezoelectric film and preparation method thereof
CN102569640B (en) Method for manufacturing composite piezoelectric substrate
CN111740005B (en) High-temperature polarization method for piezoelectric film
US10553778B2 (en) Piezoelectric device and method for manufacturing piezoelectric device
CN112532195B (en) Passive cavity type single crystal film bulk acoustic resonator structure and preparation method thereof
CN111817681A (en) Preparation method of film bulk acoustic resonator
JP2003017967A (en) Surface acoustic wave element and its manufacturing method
CN103765769B (en) Piezoelectrics wave device and manufacture method thereof
JPH1155070A (en) Surface acoustic wave element and its producing method
CN111262543A (en) Scandium-doped aluminum nitride lamb wave resonator and preparation method thereof
CN108493325A (en) A kind of high-frequency high-performance SAW device and preparation method thereof
WO2024055980A1 (en) Surface acoustic wave resonance device and forming method therefor
CN111799368B (en) Preparation method of heterostructure film for reducing film peeling thermal stress
Reinhardt et al. Acoustic filters based on thin single crystal LiNbO 3 films: status and prospects
CN114584101A (en) Surface acoustic wave resonator, method for manufacturing the same, and surface acoustic wave filter
CN212163290U (en) Scandium-doped aluminum nitride lamb wave resonator
CN210444234U (en) Radio frequency surface acoustic wave filter chip
JP2021520755A (en) Film bulk acoustic wave resonator and its manufacturing method
WO2022188779A1 (en) Resonator and manufacturing method therefor, filter, and electronic device
Katada et al. Second harmonic mode polarization inverted resonator consisting of PbTiO 3 thin film
CN114381808B (en) Method for preparing composite film by microwave heating, composite film and electronic component
CN117750868B (en) Composite piezoelectric substrate and preparation method thereof
JP2002100958A (en) Surface acoustic wave element and its manufacturing method
CN117042579A (en) Piezoelectric monocrystalline film composite material and preparation method thereof
CN118091994A (en) Preparation method of lithium niobate composite film for high-performance electro-optic modulator

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
TA01 Transfer of patent application right

Effective date of registration: 20220317

Address after: 201815 zone a, floor 2, building 2, No. 163, xinlai Road, Jiading District, Shanghai

Applicant after: Shanghai Xinsi polymer semiconductor Co.,Ltd.

Address before: 200050 No. 865, Changning Road, Shanghai, Changning District

Applicant before: SHANGHAI INSTITUTE OF MICROSYSTEM AND INFORMATION TECHNOLOGY, CHINESE ACADEMY OF SCIENCES

TA01 Transfer of patent application right
GR01 Patent grant
GR01 Patent grant