TWI582429B - Scanning method for an atomic force microscopy - Google Patents

Scanning method for an atomic force microscopy Download PDF

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TWI582429B
TWI582429B TW104100807A TW104100807A TWI582429B TW I582429 B TWI582429 B TW I582429B TW 104100807 A TW104100807 A TW 104100807A TW 104100807 A TW104100807 A TW 104100807A TW I582429 B TWI582429 B TW I582429B
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probe
probes
scanning
inclination angle
atomic force
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TW201625955A (en
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傅立成
吳俊緯
林奕廷
羅宇廷
劉韋志
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國立臺灣大學
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原子力顯微鏡掃描方法 Atomic force microscope scanning method

本發明乃是與一種原子力顯微鏡掃描方法相關,且尤其是與應用雙探針進行掃描之原子力顯微鏡掃描方法相關。 The present invention relates to an atomic force microscope scanning method, and more particularly to an atomic force microscope scanning method using a dual probe for scanning.

近年來,奈米技術(Nanotechnology)成為科技發展的重心之一,主要是因物質在尺度劇減後的物理性質常會產生變化,在了解這些物質在奈米尺度下所擁有的量子和表面現象之後,始可為其另闢蹊徑,應用獲得新材料或新器械。因此,必不可或缺的是可達原子尺度解析度的觀測工具,原子力顯微鏡(Atomic force microscopy)即為其中一選擇。 In recent years, Nanotechnology has become one of the focuses of the development of science and technology, mainly because the physical properties of substances after the scale reduction are often changed, after understanding the quantum and surface phenomena possessed by these substances at the nanometer scale. It can be used to find new ways to apply new materials or new equipment. Therefore, what is indispensable is the observation tool that can reach the atomic scale resolution. Atomic force microscopy is one of the choices.

原子力顯微鏡的原理是藉由其內特製的微小探針得針尖與試片間的原子作用力,在掃描試片中使懸臂樑產生微細位移,以測得試片表面的微結構形狀,對導體及絕緣體均有三維空間的顯影能力。不僅如此,原子力顯微鏡還可偵測出探針與試片表面之間的某種交互作用,如穿隧電流、原子力、磁力、近場電磁波等等微特性,而可應用於探索奈米尺度下微觀的物性(光、力、電、磁)量測。 The principle of atomic force microscopy is to make the cantilever beam slightly displaced in the scanning test piece by the atomic force between the tip and the test piece by the special micro-probe inside it, to measure the microstructure shape of the test piece surface, and the conductor And the insulator has a three-dimensional development capability. Moreover, the atomic force microscope can detect some interaction between the probe and the surface of the test piece, such as tunneling current, atomic force, magnetic force, near-field electromagnetic wave, etc., and can be applied to explore the nanometer scale. Microscopic physical properties (light, force, electricity, magnetism) measurements.

然而,習知的原子力顯微鏡因為其探針的傾斜角度是一固定角度,無法統一適用於不同厚薄、輪廓的試片,而常會受到試片自身的特性影響其輸出數據的準確性,為研究過程另添變數。 However, the conventional atomic force microscope is not suitable for different thickness and contour test pieces because the tilt angle of the probe is a fixed angle, and often the accuracy of the output data is affected by the characteristics of the test piece itself. Add another variable.

本發明之一目的係在提供一種原子力顯微鏡掃描方法,透過控制雙探針在適於特定試片的傾角上掃描試片,並依據掃描進行時的配置合併兩探針的掃描資料,而能準確獲得該試片上的表面微結構形狀或微特性。 An object of the present invention is to provide an atomic force microscope scanning method for scanning a test piece by controlling a double probe on a tilt angle suitable for a specific test piece, and combining the scan data of the two probes according to the configuration at the time of scanning, which can be accurately The surface microstructure shape or microfeatures on the test piece were obtained.

依據本發明,提供一種原子力顯微鏡掃描方法,適用於一具有雙探針之原子力顯微鏡,包括:將該些探針進行對位;分別調整該些探針的一傾角適於掃描一試片;分別以一探針掃描該試片以取得一筆掃描資料;及合併該兩筆掃描資料,以獲得該試片上的表面微結構形狀或微特性。 According to the present invention, there is provided an atomic force microscope scanning method, which is suitable for an atomic force microscope with dual probes, comprising: aligning the probes; respectively adjusting an inclination angle of the probes to scan a test piece; The test piece is scanned with a probe to obtain a scan data; and the two scan data are combined to obtain a surface microstructure shape or micro-characteristic on the test piece.

由上述中可以得知,本發明之原子力顯微鏡掃描方法,透過控制雙探針的傾角及合併掃描資料等設計,以獲得該試片上的表面微結構形狀或微特性,並有效提升原子力顯微鏡的準確性。 It can be known from the above that the atomic force microscope scanning method of the present invention is designed to obtain the surface microstructure or micro-characteristics on the test piece by controlling the inclination angle of the double probe and combining scanning data, and effectively improving the accuracy of the atomic force microscope. Sex.

1‧‧‧原子力顯微鏡 1‧‧‧Atomic Force Microscope

2‧‧‧試片 2‧‧‧ test strips

10‧‧‧測量單元 10‧‧‧Measurement unit

11、12‧‧‧探針 11, 12 ‧ ‧ probe

13‧‧‧鏡台 13‧‧‧Mirror

20‧‧‧第一掃描單元 20‧‧‧First scanning unit

30‧‧‧第二掃描單元 30‧‧‧Second scanning unit

40‧‧‧資料處理單元 40‧‧‧Data Processing Unit

50‧‧‧軌跡產生單元 50‧‧‧Track generation unit

60‧‧‧光學顯微鏡 60‧‧‧Light microscope

第1圖顯示依據本發明所適用之原子力顯微鏡之一系統結構示意圖。 Figure 1 is a schematic view showing the structure of a system of an atomic force microscope to which the present invention is applied.

第2圖顯示的是其一探針與一試片之間位置關係示意圖。 Figure 2 shows a schematic diagram of the positional relationship between a probe and a test piece.

為進一步說明各實施例,本發明乃提供有圖式。此些圖式乃為本發明揭露內容之一部分,其主要係用以說明實施例,並可配合說明書之相關描述來解釋實施例的運作原理。配合參考這些內容,本領域具有通常知識者應能理解其他可能的實施方式以及本發明之優點。圖中的元件並未按比例繪製,而類似的元件符號通常用來表示類似的元件。 To further illustrate the various embodiments, the invention is provided with the drawings. The drawings are a part of the disclosure of the present invention, and are mainly used to explain the embodiments, and the operation of the embodiments may be explained in conjunction with the related description of the specification. With reference to such content, those of ordinary skill in the art should be able to understand other possible embodiments and advantages of the present invention. Elements in the figures are not drawn to scale, and similar elements are generally used to represent similar elements.

首先,請先參考第1圖,其顯示依據本發明所適用之原子力 顯微鏡之一系統結構示意圖。請注意,在此說明的原子力顯微鏡乃是本發明所適用之其中一種實施態樣,本發明並不以此為限。如第1圖中所示,原子力顯微鏡1主要包括一測量單元10、一第一掃描單元20、一第二掃描單元30及一資料處理單元40。測量單元10包括兩個探針11、12,針頭分別指向鏡台13上的試片2。 First, please refer to Figure 1 first, which shows the atomic force applied in accordance with the present invention. A schematic diagram of one of the microscope systems. Please note that the atomic force microscope described herein is one of the embodiments to which the present invention is applicable, and the present invention is not limited thereto. As shown in FIG. 1, the atomic force microscope 1 mainly includes a measuring unit 10, a first scanning unit 20, a second scanning unit 30, and a data processing unit 40. The measuring unit 10 comprises two probes 11, 12 which are respectively directed to the test strip 2 on the stage 13.

第一掃描單元20及第二掃描單元30分別連接至探針11、12,並且可調整探針11、12的位置,舉例來說,第一掃描單元20或第二掃描單元30之任一內可設置一XY-壓電位移元件控制探針11/12在XY平面上的移動並且設置一Z-壓電位移元件控制探針11/12在Z軸上的高度,另一例為第一掃描單元20或第二掃描單元30之任一內可設置一XYZ-壓電位移元件控制探針11/12在XYZ三軸上的位置,或者是利用其他形式驅動而可調整探針11/12位置的元件及其他設置結構,並不限於此。在本實施例中,本實施例的架構是以同一個軌跡產生單元50發出正源及負源輸出訊號,分別控制第一掃描單元20及第二掃描單元30,第一掃描單元20內設置一XY-壓電位移元件控制探針11在XY平面上的移動並且設置一Z-壓電位移元件控制探針11在Z軸上的高度,第二掃描單元30內設置一XYZ-壓電位移元件控制探針12在XYZ三軸上的位置,這乃是因為探針12在Z軸上的高度調整幅度相較於其在XY平面上的移動來得小很多,然而本發明並不限於以此方式建構出雙探針架構,亦可以其他方式達成。 The first scanning unit 20 and the second scanning unit 30 are respectively connected to the probes 11, 12, and the positions of the probes 11, 12 can be adjusted, for example, within either the first scanning unit 20 or the second scanning unit 30. An XY-piezoelectric displacement element can be provided to control the movement of the probe 11/12 in the XY plane and to set a Z-piezoelectric displacement element to control the height of the probe 11/12 on the Z axis, and another example is the first scanning unit. The position of the XYZ-piezoelectric displacement element control probe 11/12 on the XYZ triaxial axis may be set in either of the 20 or the second scanning unit 30, or the position of the probe 11/12 may be adjusted by other forms of driving. The components and other setting structures are not limited thereto. In this embodiment, the architecture of the embodiment is that the same trajectory generating unit 50 sends out positive and negative source output signals, and controls the first scanning unit 20 and the second scanning unit 30 respectively, and the first scanning unit 20 is provided with a The XY-piezoelectric displacement element controls the movement of the probe 11 in the XY plane and sets a Z-piezoelectric displacement element to control the height of the probe 11 on the Z axis, and an XYZ-piezoelectric displacement element is disposed in the second scanning unit 30. The position of the probe 12 on the XYZ triaxial is controlled because the height adjustment amplitude of the probe 12 on the Z axis is much smaller than its movement in the XY plane, but the invention is not limited in this way. Constructing a dual probe architecture can also be achieved in other ways.

在使用原子力顯微鏡1進行掃描時,首先需將探針11、12進行對位。本實施例是以粗調跟細調兩步驟完成對位,在粗調時,是以一光學顯微鏡60藉由顯示探針11、12針尖的一影像,並控制第一掃描單元20及第 二掃描單元30使探針11、12針尖移動至一定範圍之內,以粗調該些探針針尖的相對位置。接著在細調時,是以探針11、12其中之一探針11/12的針尖掃描另一探針12/11,如:以探針11掃描探針12的針尖,獲得兩探針11、12之間的相對位置關係,以便細部調動探針11、12針尖的相對位置或供後續判讀資料時使用。 When scanning with the atomic force microscope 1, it is first necessary to align the probes 11, 12. In this embodiment, the alignment is performed in two steps of coarse adjustment and fine adjustment. In the coarse adjustment, an image of the probes 11 and 12 is displayed by an optical microscope 60, and the first scanning unit 20 and the first control unit are controlled. The two scanning unit 30 moves the tips of the probes 11, 12 to a certain range to coarsely adjust the relative positions of the probe tips. Then, in the fine adjustment, the other probe 12/11 is scanned with the tip of one of the probes 11 and 12, for example, the tip of the probe 12 is scanned by the probe 11, and the two probes 11 are obtained. The relative positional relationship between 12, so that the relative position of the tip of the probe 11, 12 can be mobilized or used for subsequent interpretation of the data.

接著,分別調整兩探針11、12的一傾角適於掃描一試片2。請參考第2圖,其顯示的是其一探針,舉例來說是探針11與一試片2之間位置關係示意圖。從第2圖中可知,探針11的傾角最佳是使得探針針尖的側面貼合於試片2的側壁,即,使得圖中的ψ角度為零。第2圖顯示的其他參數尚有:σ為試片2的一側壁傾角、α為探針11的針尖半頂角、1為探針11的長度、針尖β為探針11的旋轉角度、h為試片2厚度、而p為試片2上的表面微結構形狀之圖形寬距。探針傾角Φ滿足下列關係:Φ=σ+α+β-π,此時可使得探針針尖的側面貼合於試片2的一側壁,如此可增加探針針尖有效掃描的範圍。以第2圖之示例來說,滿足前述關係式可使得探針針尖掃描至試片2右側壁與底部交接處時,使得探針11的針尖右側是貼合於試片2右側壁。另一探針12較佳地是往探針11相對方向傾斜,如往第2圖中的左側傾斜,較佳是滿足前述關係式而傾斜至使探針針尖掃描至試片2左側壁與底部交接處時,探針12的針尖左側是貼合於試片2左側壁。 Next, adjusting an inclination angle of the two probes 11, 12 respectively is suitable for scanning a test piece 2. Please refer to FIG. 2, which shows a probe thereof, for example, a schematic diagram of the positional relationship between the probe 11 and a test strip 2. As can be seen from Fig. 2, the inclination angle of the probe 11 is preferably such that the side surface of the probe tip is attached to the side wall of the test piece 2, i.e., the ψ angle in the figure is zero. The other parameters shown in Fig. 2 are: σ is the side wall inclination angle of the test piece 2, α is the tip half angle of the probe 11, 1 is the length of the probe 11, the needle tip β is the rotation angle of the probe 11, h It is the thickness of the test piece 2, and p is the graphic width of the surface microstructure shape on the test piece 2. The probe tilt angle Φ satisfies the following relationship: Φ = σ + α + β - π, in which case the side of the probe tip can be attached to one side wall of the test strip 2, which can increase the effective scanning range of the probe tip. In the example of FIG. 2, the above relationship is satisfied such that the probe tip is scanned to the intersection of the right side wall and the bottom of the test piece 2 such that the right side of the tip of the probe 11 is attached to the right side wall of the test piece 2. The other probe 12 is preferably inclined to the opposite direction of the probe 11, as inclined to the left side in FIG. 2, preferably to satisfy the aforementioned relationship and tilted so that the probe tip is scanned to the left side wall and the bottom of the test piece 2. At the junction, the left side of the tip of the probe 12 is attached to the left side wall of the test piece 2.

然而,考量到有些試片2可能易碎或者具有重複的微結構設置在其上,若以大角度傾斜探針11、12,其針尖可能在掃描過程中撞到附近密集排列的微結構而產生損壞。為了避免發生這樣的情況,先以β-α-tan-1(h/(hcot(σ)+p))≦σ+α+β-π之關係式判斷前述關係式得到的探針傾 角Φ是否大於β-α-tan-1(h/(hcot(σ)+p)),若是,則設定探針11/12的傾角為β-α-tan-1(h/(hcot(σ)+p)),而非σ+α+β-π。因此,透過此步驟調整探針傾角後,探針11、12即適於掃描該特定之試片2。 However, it is considered that some of the test pieces 2 may be fragile or have a repeating microstructure disposed thereon. If the probes 11, 12 are tilted at a large angle, the tip of the probe may collide with a densely arranged microstructure in the vicinity during scanning. damage. In order to avoid such a situation, first determine whether the probe tilt angle Φ obtained by the above relation is obtained by the relationship of β-α-tan -1 (h/(hcot(σ)+p))≦σ+α+β-π Greater than β-α-tan -1 (h/(hcot(σ)+p)), and if so, set the inclination of the probe 11/12 to β-α-tan -1 (h/(hcot(σ)+p )) instead of σ+α+β-π. Therefore, after adjusting the probe tilt angle by this step, the probes 11, 12 are adapted to scan the particular test strip 2.

接著,分別以一探針11/12掃描試片2以取得一筆掃描資料。在本實施例中,輪流移動探針11、12之一,以相反方向掃描試片2,其中對探針傾角為銳角之探針,使其由一側至對向側掃描試片2,對探針傾角為鈍角之另一探針,使其由該對向側至該一側掃描試片2。舉例來說,使第2圖所示的探針11由左至右掃描試片2,使探針12由右至左掃描試片2,在掃描完畢之後,資料處理單元40收到分別由探針11、12獲得的掃描資料。 Next, the test piece 2 is scanned by a probe 11/12 to obtain a scanned data. In this embodiment, one of the probes 11, 12 is rotated to scan the test strip 2 in the opposite direction, wherein the probe is tilted at an acute angle to scan the test strip 2 from one side to the opposite side, The other probe having an angle of inclination of the probe is an obtuse angle, and the test piece 2 is scanned from the opposite side to the one side. For example, the probe 11 shown in FIG. 2 is scanned from left to right, and the probe 12 is scanned from right to left. After the scanning is completed, the data processing unit 40 receives the probe. Scanned data obtained by needles 11, 12.

資料處理單元40接著合併來自探針11、12的該兩筆掃描資料,以經過資料判讀之後,獲得該試片2上的表面微結構形狀或微特性。在本實施例中,考量到探針11、12的傾斜角度不同、掃描方向不同,使其對於不同斜率的微結構形狀有著不同的表現。舉例來說,探針11之傾角為銳角且其掃描方向為由左至右,其對以負斜率下降的微結構形狀的判斷效果不佳,相反地,其對以正斜率上升的微結構形狀,就能精準地判斷。因此,當連續兩掃描點之間為正斜率時,擷取傾角為銳角且其掃描方向為由左至右之探針11取得的該筆掃描資料為供分析其表面微結構形狀或微特性,然而當連續兩掃描點之間為負斜率時,擷取傾角為鈍角且其掃描方向為由右至左之探針12取得的該筆掃描資料為供分析其表面微結構形狀或微特性。下式為資料合併關係式: P m (t k )為該兩筆掃描資料之一合併結果,S i (t k )為兩掃描點之間的斜率,k=0,1,....,m,...,i為該些探針的編號,i=1或2,分別代表探針11和探針12。 The data processing unit 40 then combines the two pieces of scanned data from the probes 11, 12 to obtain the surface microstructure shape or micro-characteristics on the test piece 2 after the data has been interpreted. In the present embodiment, it is considered that the inclination angles of the probes 11, 12 are different and the scanning directions are different, so that they have different performances for the microstructure shapes of different slopes. For example, the tilt angle of the probe 11 is an acute angle and its scanning direction is from left to right, which has a poor judgment effect on the shape of the microstructure falling with a negative slope, and conversely, it is a shape of the microstructure that rises with a positive slope. , can be judged accurately. Therefore, when there is a positive slope between two consecutive scanning points, the scanning data obtained by the probe 11 having an acute angle and whose scanning direction is left to right is for analyzing the surface microstructure shape or micro characteristics. However, when there is a negative slope between successive two scanning points, the scanning data obtained by the right-to-left probe 12 is taken as an obtuse angle and its scanning direction is for analyzing the surface microstructure shape or micro-characteristic. The following formula is the data merge relationship: P m ( t k ) is the combined result of one of the two scanning data, S i ( t k ) is the slope between the two scanning points, k =0,1,...., m ,...,i For the numbering of these probes, i = 1 or 2, respectively, represents probe 11 and probe 12.

由上述中可以得知,本發明之原子力顯微鏡掃描方法,透過控制雙探針的傾角及合併掃描資料等設計,以獲得該試片上的表面微結構形狀或微特性,並有效提升原子力顯微鏡的準確性。 It can be known from the above that the atomic force microscope scanning method of the present invention is designed to obtain the surface microstructure or micro-characteristics on the test piece by controlling the inclination angle of the double probe and combining scanning data, and effectively improving the accuracy of the atomic force microscope. Sex.

以上敍述依據本發明多個不同實施例,其中各項特徵可以單一或不同結合方式實施。因此,本發明實施方式之揭露為闡明本發明原則之具體實施例,應不拘限本發明於所揭示的實施例。進一步言之,先前敍述及其附圖僅為本發明示範之用,並不受其限囿。其他元件之變化或組合皆可能,且不悖于本發明之精神與範圍。 The above description is based on a number of different embodiments of the invention, wherein the features may be implemented in a single or different combination. Therefore, the disclosure of the embodiments of the present invention is intended to be illustrative of the embodiments of the invention. Further, the foregoing description and the accompanying drawings are merely illustrative of the invention and are not limited. Variations or combinations of other elements are possible and are not intended to limit the spirit and scope of the invention.

Claims (6)

一種原子力顯微鏡掃描方法,適用於一具有雙探針之原子力顯微鏡,包括:將該些探針進行對位;分別調整該些探針的一傾角Φ適於掃描一試片,並藉由一光學顯微鏡顯示該些探針及試片之影像進行對位;分別以一探針掃描該試片以取得一筆掃描資料;及合併該兩筆掃描資料,以獲得該試片上的表面微結構形狀或微特性,包括下列步驟:當連續兩掃描點之間為正斜率時,擷取該些探針之該傾角Φ為銳角且其掃描方向為由左至右之該探針取得的該掃描資料為供分析其表面微結構形狀或微特性;及當連續兩掃描點之間為負斜率時,擷取該些探針之該傾角Φ為鈍角且其掃描方向為由右至左之該探針取得的該掃描資料為供分析其表面微結構形狀或微特性。 An atomic force microscope scanning method suitable for an atomic force microscope with dual probes, comprising: aligning the probes; respectively adjusting an inclination angle Φ of the probes for scanning a test piece, and by using an optical The microscope displays the images of the probes and the test strips for alignment; respectively, scanning the test strips with a probe to obtain a scan data; and combining the two scan data to obtain a surface microstructure shape or micro on the test strip The characteristic includes the following steps: when there is a positive slope between two consecutive scanning points, the inclination angle Φ of the probes is taken as an acute angle and the scanning direction is the scanning data obtained by the probe from left to right. Analyzing the surface microstructure shape or micro-characteristics; and when the two consecutive scanning points have a negative slope, the inclination angle Φ of the probes is obtuse and the scanning direction is obtained from the right-to-left probe. The scanned data is for analysis of its surface microstructure shape or micro-characteristics. 如申請專利範圍第1項所述的原子力顯微鏡掃描方法,其中該傾角Φ是以下列關係獲得:該探針之該傾角Φ滿足Φ=σ+α+β-π,σ為該試片的一側壁傾角,α為該探針的針尖半頂角,且β為該探針的旋轉角度。 The atomic force microscope scanning method according to claim 1, wherein the inclination angle Φ is obtained by the following relationship: the inclination angle Φ of the probe satisfies Φ=σ+α+β-π, and σ is one of the test pieces. The side wall inclination angle, α is the tip half angle of the probe, and β is the rotation angle of the probe. 如申請專利範圍第1項所述的原子力顯微鏡掃描方法,其中該傾角Φ是以下列關係獲得:若β-α-tan-1(h/(hcot(σ)+p))≦σ+α+β-π,則設定該探針的該傾角Φ等於β-α-tan-1(h/(hcot(σ)+p)),否則,該探針的該傾角Φ為σ+α+β-π,σ為該試片的一側壁傾角,α為該探針的針尖半頂角,β為該探針的旋轉角度,且p為該試片上的表面微結構形狀之圖形寬距。 The atomic force microscope scanning method according to claim 1, wherein the inclination angle Φ is obtained in the following relationship: if β-α-tan -1 (h/(hcot(σ)+p))≦σ+α+ Β-π, the inclination angle Φ of the probe is set to be equal to β-α-tan -1 (h/(hcot(σ)+p)), otherwise, the inclination angle Φ of the probe is σ+α+β- π, σ is the inclination angle of one side wall of the test piece, α is the tip half angle of the probe, β is the rotation angle of the probe, and p is the graphic width of the surface microstructure shape on the test piece. 如申請專利範圍第1項所述的原子力顯微鏡掃描方法,其中將該些探針進行對位的該步驟更包括:藉由顯示該些探針針尖的一影像,以粗調該些探針針尖的相對位置;及以該些探針之其一探針掃描另一探針的針尖,獲得該些探針之間的相對位置關係,以細調該些探針針尖的相對位置。 The AFM scanning method of claim 1, wherein the step of aligning the probes further comprises: coarsely adjusting the probe tips by displaying an image of the probe tips The relative positions of the probes are scanned by the probes of the other probes to obtain the relative positional relationship between the probes to finely adjust the relative positions of the probe tips. 如申請專利範圍第1項所述的原子力顯微鏡掃描方法,其中分別以一探針掃描該試片以取得一筆掃描資料的該步驟更包括:輪流移動該些探針之一,以相反方向掃描該試片。 The AFM scanning method of claim 1, wherein the step of scanning the test piece with a probe to obtain a piece of scanned data further comprises: moving one of the probes in turn to scan the opposite direction Audition. 如申請專利範圍第5項所述的原子力顯微鏡掃描方法,其中合併該兩筆掃描資料,以獲得該試片上的表面微結構形狀或微特性的該步驟是依據下列關係式進行: 為該兩筆掃描資料之一合併結果,S i (t k )為兩掃描點之間的斜率,k=0,1,....,m,...,i為該些探針的編號,i=1或2。 The atomic force microscope scanning method according to claim 5, wherein the step of combining the two scanning materials to obtain the surface microstructure shape or micro-characteristics on the test piece is performed according to the following relationship: For the result of combining the two scan data, S i ( t k ) is the slope between the two scan points, k =0, 1, . . . , m, . . . , i is the probe Number, i=1 or 2.
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TW348260B (en) * 1996-05-20 1998-12-21 Ohara Tetsuo Apparatus for and method of real-time nanometer-scale position measurement of the sensor of a scanning tunneling microscope
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