CN109870593A - A kind of method of excitation probe vibration in atomic force microscope - Google Patents

A kind of method of excitation probe vibration in atomic force microscope Download PDF

Info

Publication number
CN109870593A
CN109870593A CN201711249013.2A CN201711249013A CN109870593A CN 109870593 A CN109870593 A CN 109870593A CN 201711249013 A CN201711249013 A CN 201711249013A CN 109870593 A CN109870593 A CN 109870593A
Authority
CN
China
Prior art keywords
probe
sample
atomic force
force microscope
excitation
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.)
Pending
Application number
CN201711249013.2A
Other languages
Chinese (zh)
Inventor
魏艳萍
卢焕明
陈国新
姚聪迪
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.)
Ningbo Institute of Material Technology and Engineering of CAS
Original Assignee
Ningbo Institute of Material Technology and Engineering 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 Ningbo Institute of Material Technology and Engineering of CAS filed Critical Ningbo Institute of Material Technology and Engineering of CAS
Priority to CN201711249013.2A priority Critical patent/CN109870593A/en
Publication of CN109870593A publication Critical patent/CN109870593A/en
Pending legal-status Critical Current

Links

Landscapes

  • Length Measuring Devices With Unspecified Measuring Means (AREA)

Abstract

The present invention provides a kind of method of excitation probe vibration in atomic force microscope, and PZT (piezoelectric transducer) is arranged below the probe, which generates the mechanical oscillation of vertical direction under signal source effect, and probe issues raw vibration in the mechanical oscillation wave excitation.It is vibrated with existing using probe driver excitation cantilever arm, to which the method for driving probe to vibrate is compared, middle probe needle point of the present invention is easier to shake off the adhesion strength of sample surfaces and the effect of capillary force carries out stable vibration, be conducive to steadily scanning imagery, high-resolution scan image is obtained, and reduces the high performance requirements to cantilever.

Description

A kind of method of excitation probe vibration in atomic force microscope
Technical field
The present invention relates to excitation probes in atomic force microscope technology field more particularly to a kind of atomic force microscope to vibrate Method.
Background technique
Atomic force microscope (Atomic Force Microscope, AFM) is after scanning tunneling microscope (Scanning Tunneling Microscope, STM) after invent one kind have the high-resolution new instrument of atom level, can be in atmosphere With the physical property for carrying out nano-area to a variety of materials and sample under liquid environment include that pattern detects, or directly into Row nano-manipulation;It has been widely used in semiconductor, nano-functional material, biology, chemical industry, food, medical research and Research Center In the fields such as the research experiment of various nanometer related disciplines, become the basic tool of nano science research.
Have in atomic force microscope a nanoscale probe be fixed on can on the micron order elastic cantilever of sensitive manipulation, When probe is close to sample, the atom and the interatomic active force of sample surfaces on top can make cantilever bending, deviate original Position.3-D image is rebuild according to the bias of probe when scanning sample or vibration amplitude, sample surfaces can be obtained indirectly Pattern or composition information.
According to the difference of probe and sample effect power property, there are mainly three types of imaging patterns by AFM: contact mode (contact Mod), noncontact mode (non-contact mode) and tapping-mode (tapping mode).
Contact mode AFM, probe tip are kept in contact with sample surfaces always, when flying-spot tube guidance needle point is above sample When inswept (or sample moves below needle point), existing coulomb repulsion power keeps cantilever generation curved between contacting with each other the electronics of atom Song, to reflect the fluctuating of pattern.Contact mode can be stablized, high-resolution image, however due to needle point and sample Between contact with each other and active force is very big, so be easy to causeing the deformation and tip wear of sample.
In noncontact mode, needle point and sample work in attraction effect section, and needle point is not contacted always with sample room, visited Needle vibrates near its resonant frequency, and the height by adjusting needle point controls tip vibration amplitude or frequency-invariant, to keep needle point With the constant space of sample.Noncontact mode is suitble to scan soft sample, but realizes this mode very under atmosphere at room temperature environment It is difficult.Because sample surfaces inevitably gather one layer of very thin water, it can set up one layer small between sample and needle point Small wick bridge inhales on needle point and surface together, to increase tip to the pressure on surface, cause image data unstable and Destruction to sample.Therefore, the success rate that noncontact mode operates in air is lower, and use is less.
Tapping-mode is between contact mode and noncontact mode.Compared with contact mode, tapping-mode contacts sample When generated lateral force be obviously reduced.Compared with noncontact mode, its main feature is that scanning process middle probe is also oscillation, and With the amplitude (be greater than 20nm) bigger than noncontact mode.Needle point taps sample, needle point and sample in the bottom of vibration period Interaction its amplitude or resonant frequency can be changed, protected using amplitude or frequency as feedback signal by adjusting the height of needle point Hold the constant space of needle point and sample.When therefore detecting soft sample in air, the tapping-mode of AFM is preferably to select It selects.
As shown in Figure 1, generally being vibrated using probe driver excitation cantilever arm in noncontact mode and tapping-mode. The probe driver routinely used at present is piezoelectric ceramic actuator, and piezoelectric ceramic actuator generates one under signal source effect Exchange vibration, which directly acts on cantilever root, is transferred to probe tip from cantilever root, thus drive cantilever with it is whole A probe oscillation.Since driving force acts only on the root of cantilever, during probe tip scans sample, sample surfaces Adhesion strength and capillary force will generate downward suction to needle point, to inhibit probe oscillation, cause under probe oscillation amplitude Drop, or even zero is fallen to, and then influence scanning imagery, cause imaging to fail.
In order to avoid such case, usually require that cantilever has high coefficient of elasticity (20-60N/m), resonant frequency and big Driving force, destroy the original of sample when but will increase equipment requirement in this way, while also will cause in tapping-mode imaging Structure, especially for soft sample, such as hanging graphene film, gel sample etc., it is also possible to destruction or mobile sample Product, and needle point can be polluted, increase the contact area of needle point and sample, stable high-resolution imaging is made to become more difficult.
Summary of the invention
Status in view of the above technology, the method that the present invention proposes excitation probe vibration in a kind of atomic force microscope, the party Method is simple and easy, can directly excitation probe make its vibration.
The technical solution of the present invention is as follows: a kind of method that excitation probe is vibrated in atomic force microscope, it is characterized in that: in institute It states and PZT (piezoelectric transducer) is set below probe, which generates the mechanical oscillation of vertical direction under signal source effect, The mechanical oscillation wave excitation test needle vibrates.
The signal source is unlimited, can be function generator.
As a kind of implementation, sample is fixed on PZT (piezoelectric transducer) surface.Preferably, sample passes through coupling Mixture is fixed on PZT (piezoelectric transducer) surface.
It is vibrated with existing using probe driver excitation cantilever arm, so that the method for driving probe to vibrate is compared, the present invention It has the following beneficial effects:
(1) motivational techniques of the invention are used, probe is directly vibrated by the excitation of mechanical vibration wave, realization pair The direct precise and tiny control of probe, thus vibrated with existing using probe driver excitation cantilever arm, so that probe be driven to shake Dynamic method is compared, and probe tip is easier to shake off the adhesion strength of sample surfaces and the effect of capillary force carries out stable vibration It is dynamic, be conducive to steadily scanning imagery, obtain high-resolution scan image, and reduces the high performance requirements to cantilever.
(2) method of the invention is suitable for the probe vibrational excitation of all vibration mode atomic force microscope, including non-connects Other spin-off models of touch formula and tapping-mode and tapping-mode: such as magnetic force microscopy, electrostatic force microscope.The party When method is imaged for tapping-mode, the realization possibility of stable high-resolution imaging is increased, especially for soft sample, Such as hanging graphene film, gel sample etc., there is imaging advantage;When for noncontact mode imaging, it can be improved in sky The success rate of noncontact mode is realized in gas.
(3) motivational techniques of the invention are used, without requiring cantilever that there is very high coefficient of elasticity, resonant frequency and big Driving force reduces the requirement to equipment.
In order to avoid such case, usually require that cantilever has high coefficient of elasticity (20-60N/m), resonant frequency and big Driving force, destroy the original of sample when but will increase equipment requirement in this way, while also will cause in tapping-mode imaging Structure, especially for soft sample, such as hanging graphene film, gel sample etc., it is also possible to destruction or mobile sample Product, and needle point can be polluted, increase the contact area of needle point and sample, stable high-resolution imaging is made to become more difficult.
Detailed description of the invention
Fig. 1 is the energisation mode structural schematic diagram of conventional AFM probe vibration;
Fig. 2 is in the embodiment of the present invention 1 using the structural schematic diagram of mechanical vibration wave excitation probe vibration;
Fig. 3 is the probe vibration frequency-amplitude obtained in the embodiment of the present invention 1 using the vibration of mechanical vibration wave excitation probe Response curve;
Fig. 4 is the probe vibration frequency-vibration obtained in comparative example 1 using conventional energisation mode excitation probe vibration Width response curve;
Fig. 5 is the hanging graphene sample shape obtained in the embodiment of the present invention 1 using the vibration of mechanical vibration wave excitation probe Looks figure;
Fig. 6 is the hanging graphene sample obtained in comparative example 1 using conventional energisation mode excitation probe vibration Shape appearance figure.
Specific embodiment
Below with reference to embodiment, present invention is further described in detail, it should be pointed out that embodiment described below purport It is being convenient for the understanding of the present invention, and is not playing any restriction effect to it.
Embodiment 1:
In the present embodiment, using the atomic force microscope of model Aglient 5500, there is one in atomic force microscope Nanoscale probe is fixed on micron order elastic cantilever, which is the silicon probe that force constant is 0.1N/m.
In the present embodiment, sample is graphene, which is covered on the silicon substrate of the hole configurations with 250nm depth On bottom, the hanging graphene sample in part is formed.
As shown in Fig. 2, PZT (piezoelectric transducer) is fixed on the sample stage of atomic force microscope, sample is passed through into glycerol It is fixed on PZT (piezoelectric transducer) surface;
Probe is located above sample, by probe close to sample surfaces.It can make first with the contact mode of atomic force microscope Needle point contacts sample, then raises needle point again, raising distance may be configured as 5um-100um.In the present embodiment, it is set as 10um。
It is generated using atomic force microscope and drives piezoelectricity using the continuous continuous sinusoidal excitation voltage of function generator generation Energy converter generates the mechanical oscillation of vertical direction, and probe issues raw vibration in the mechanical oscillation wave excitation.
Using the frequency-amplitude response curve of atomic force microscope test mechanical vibration wave excitation test needle vibration, as a result As shown in figure 3, display does not have miscellaneous peak interference using the formant that mechanical vibration wave driving obtains, signal-to-noise ratio is high.
The driving voltage frequency and amplitude that PZT (piezoelectric transducer) is arranged are respectively 11.2KHz and 5v, at this time probe free vibration Amplitude be about 50nm, be imaged using atomic force microscope tapping-mode.It can using mechanical vibration wave driving probe vibration Obtain clearly feature image, high resolution, as shown in Figure 5.
Comparative example 1:
In the present embodiment, atomic force microscope, probe and sample with it is identical in embodiment 1.
Sample is placed on the sample stage of atomic force microscope.Probe is located above sample, by probe close to sample Surface.Needle point can be made to contact sample first with the contact mode of atomic force microscope, then raise needle point again, raising distance can It is set as 5um-100um.In the present embodiment, it is set as 10um.
As shown in Figure 1, an exchange vibration, the vibration are generated under the effect of function generator source using piezoelectric ceramic actuator Power directly acts on cantilever root, is transferred to probe tip from cantilever root, so that cantilever and entire probe be driven to vibrate.
Using the frequency-amplitude response curve of atomic force microscope test mechanical vibration wave excitation test needle vibration, as a result As shown in Figure 4.Figure 4, it is seen that compared with Fig. 3, using Conventional piezoelectric ceramics motivate the lower formant obtained exist compared with More miscellaneous peak interference, signal-to-noise ratio are low.
Setting probe driver driving voltage frequency and amplitude are respectively 11.2KHz and 1v, probe free vibration at this time Amplitude is about 50nm, is imaged using atomic force microscope tapping-mode, image is as shown in Figure 6.From fig. 6 it can be seen that Compared with Fig. 5, image is fuzzy, there is noise.That is, vibrated using identical probe using excitation probe under conventional energisation mode, Under tapping-mode, identical region can not obtain full resolution pricture.
Technical solution of the present invention is described in detail in embodiment described above, it should be understood that the above is only For specific embodiments of the present invention, it is not intended to restrict the invention, all any modifications made in spirit of the invention, Supplement or similar fashion substitution etc., should all be included in the protection scope of the present invention.

Claims (8)

1. a kind of method that excitation probe is vibrated in atomic force microscope is changed it is characterized in that: piezoelectricity is arranged below the probe Energy device, the PZT (piezoelectric transducer) generate the mechanical oscillation of vertical direction under signal source effect, and probe is in the mechanical oscillation wave excitation It is lower to vibrate.
2. the method that excitation probe is vibrated in atomic force microscope as described in claim 1, it is characterized in that: the signal source It is function generator.
3. the method that excitation probe is vibrated in atomic force microscope as described in claim 1, it is characterized in that: sample is fixed In PZT (piezoelectric transducer) surface.
4. the method that excitation probe is vibrated in atomic force microscope as described in claim 1, it is characterized in that: sample passes through Couplant is fixed on PZT (piezoelectric transducer) surface.
5. the method that excitation probe is vibrated in atomic force microscope as described in claim 1, it is characterized in that: using non-contact mould Formula is scanned imaging to sample.
6. the method that excitation probe is vibrated in atomic force microscope as described in claim 1, it is characterized in that: using tapping-mode Imaging is scanned to sample.
7. such as the method for excitation probe vibration in atomic force microscope described in claim 5 or 6, it is characterized in that: sample It is soft sample.
8. the method that excitation probe is vibrated in atomic force microscope as claimed in claim 7, it is characterized in that: sample is outstanding Graphene film, the gel sample of sky.
CN201711249013.2A 2017-12-01 2017-12-01 A kind of method of excitation probe vibration in atomic force microscope Pending CN109870593A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201711249013.2A CN109870593A (en) 2017-12-01 2017-12-01 A kind of method of excitation probe vibration in atomic force microscope

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201711249013.2A CN109870593A (en) 2017-12-01 2017-12-01 A kind of method of excitation probe vibration in atomic force microscope

Publications (1)

Publication Number Publication Date
CN109870593A true CN109870593A (en) 2019-06-11

Family

ID=66914672

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201711249013.2A Pending CN109870593A (en) 2017-12-01 2017-12-01 A kind of method of excitation probe vibration in atomic force microscope

Country Status (1)

Country Link
CN (1) CN109870593A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2022151645A1 (en) * 2021-01-15 2022-07-21 长鑫存储技术有限公司 Dimension measurement method and device for semiconductor structure

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH11142419A (en) * 1997-11-06 1999-05-28 Hitachi Constr Mach Co Ltd Scanning probe microscope
CN1821743A (en) * 2006-03-27 2006-08-23 北京航空航天大学 Atomic force microscopic detecting method and device for moonscape environment locating measurement
CN102495238A (en) * 2011-11-11 2012-06-13 北京航空航天大学 Sixth harmonic imaging system based on tapping mode atomic force microscope
CN102749480A (en) * 2012-07-10 2012-10-24 上海交通大学 Method for improving vibration amplitude of electrostatic force driven atomic force microscope probe cantilever
CN104062466A (en) * 2014-07-01 2014-09-24 哈尔滨工业大学 Micro-nano structure sidewall surface imaging device based on atomic force microscope (AFM) and imaging method thereof
CN105910560A (en) * 2016-04-21 2016-08-31 长春理工大学 Biological cell ultrasonic atomic force microscopic detection system and method
CN106501552A (en) * 2015-09-07 2017-03-15 中国科学院苏州纳米技术与纳米仿生研究所 A kind of while the method for measurement surface magnetic and surface potential
CN107192857A (en) * 2016-03-14 2017-09-22 中国科学院沈阳自动化研究所 A kind of nano film thickness detection means and its method based on ultrasonic AFM

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH11142419A (en) * 1997-11-06 1999-05-28 Hitachi Constr Mach Co Ltd Scanning probe microscope
CN1821743A (en) * 2006-03-27 2006-08-23 北京航空航天大学 Atomic force microscopic detecting method and device for moonscape environment locating measurement
CN102495238A (en) * 2011-11-11 2012-06-13 北京航空航天大学 Sixth harmonic imaging system based on tapping mode atomic force microscope
CN102495238B (en) * 2011-11-11 2013-03-13 北京航空航天大学 Sixth harmonic imaging system based on tapping mode atomic force microscope
CN102749480A (en) * 2012-07-10 2012-10-24 上海交通大学 Method for improving vibration amplitude of electrostatic force driven atomic force microscope probe cantilever
CN104062466A (en) * 2014-07-01 2014-09-24 哈尔滨工业大学 Micro-nano structure sidewall surface imaging device based on atomic force microscope (AFM) and imaging method thereof
CN106501552A (en) * 2015-09-07 2017-03-15 中国科学院苏州纳米技术与纳米仿生研究所 A kind of while the method for measurement surface magnetic and surface potential
CN107192857A (en) * 2016-03-14 2017-09-22 中国科学院沈阳自动化研究所 A kind of nano film thickness detection means and its method based on ultrasonic AFM
CN105910560A (en) * 2016-04-21 2016-08-31 长春理工大学 Biological cell ultrasonic atomic force microscopic detection system and method

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
杨春来: "超声振动原子力显微镜成像研究", 《中国博士学位论文全文数据库 工程科技II辑》 *
黄新民等: "《材料研究方法》", 30 November 2017 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2022151645A1 (en) * 2021-01-15 2022-07-21 长鑫存储技术有限公司 Dimension measurement method and device for semiconductor structure

Similar Documents

Publication Publication Date Title
US10156585B2 (en) Cantilevered probes having piezoelectric layer, treated section, and resistive heater, and method of use for chemical detection
Eaton et al. Atomic force microscopy
JP4832296B2 (en) Atomic force microscope probe
US9069007B2 (en) Multiple frequency atomic force microscopy
JP5000076B2 (en) Force scanning probe microscope
Rana et al. Improvement in the imaging performance of atomic force microscopy: A survey
US6945099B1 (en) Torsional resonance mode probe-based instrument and method
JP6154319B2 (en) Method for surface measurement and modification by scanning probe microscopy functioning in continuous curve mode, scanning probe microscope and device for implementing it
JPH10507000A (en) Flick atomic force microscope with phase or frequency detection
Fairbairn et al. Control techniques for increasing the scan speed and minimizing image artifacts in tapping-mode atomic force microscopy: Toward video-rate nanoscale imaging
US7013717B1 (en) Manual control with force-feedback for probe microscopy-based force spectroscopy
CN109870593A (en) A kind of method of excitation probe vibration in atomic force microscope
US8689358B2 (en) Dynamic mode nano-scale imaging and position control using deflection signal direct sampling of higher mode-actuated microcantilevers
Das et al. Intelligent tracking control system for fast image scanning of atomic force microscopes
Meyer et al. Introduction to scanning probe microscopy
JP4931640B2 (en) Scanning probe microscope
WO2008156722A1 (en) Material property measurements using multiple frequency atomic forece microsocopy
Satoh et al. Using dynamic force microscopy with piezoelectric cantilever for indentation and high-speed observation
JP4282588B2 (en) Probe and scanning probe microscope
Habibullah High-precision nanopositioning control of a piezoelectric tube scanner: Atomic force microscopy
JP2006300592A (en) Scanning mechanism and scanning probe microscope
アクラミ,セイドモハマド Improvement of stability and speed in liquid-environment atomic force microscopy
Suzuki et al. The displacement measurement device using a comb-drive actuator
Grant Development of Non-Contact Scanning Force Microscopy for Imaging in Liquid Environments
Kolluru Mems atomic force microscope

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
RJ01 Rejection of invention patent application after publication

Application publication date: 20190611

RJ01 Rejection of invention patent application after publication