WO2009093284A1 - 走査型プローブ顕微鏡 - Google Patents
走査型プローブ顕微鏡 Download PDFInfo
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- WO2009093284A1 WO2009093284A1 PCT/JP2008/000078 JP2008000078W WO2009093284A1 WO 2009093284 A1 WO2009093284 A1 WO 2009093284A1 JP 2008000078 W JP2008000078 W JP 2008000078W WO 2009093284 A1 WO2009093284 A1 WO 2009093284A1
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01Q—SCANNING-PROBE TECHNIQUES OR APPARATUS; APPLICATIONS OF SCANNING-PROBE TECHNIQUES, e.g. SCANNING PROBE MICROSCOPY [SPM]
- G01Q20/00—Monitoring the movement or position of the probe
- G01Q20/02—Monitoring the movement or position of the probe by optical means
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01Q—SCANNING-PROBE TECHNIQUES OR APPARATUS; APPLICATIONS OF SCANNING-PROBE TECHNIQUES, e.g. SCANNING PROBE MICROSCOPY [SPM]
- G01Q30/00—Auxiliary means serving to assist or improve the scanning probe techniques or apparatus, e.g. display or data processing devices
- G01Q30/04—Display or data processing devices
- G01Q30/06—Display or data processing devices for error compensation
Definitions
- the present invention relates to a scanning probe microscope, and more particularly to a scanning probe microscope provided with a displacement detection means for optically detecting a mechanical displacement of a cantilever provided with a probe.
- An atomic force microscope Atomic
- Force Microscope typified by Force Microscope.
- a cantilever equipped with a probe is vibrated near its resonance point, and the interaction between the sample surface acting on the probe in that state is cantilever.
- a method called a non-contact mode or a dynamic mode is used in which the vibration is converted into a change in amplitude, phase, or frequency.
- FIG. 5 is a configuration diagram of a main part of a conventionally known scanning probe microscope described in, for example, Patent Document 1.
- a sample 1 to be observed is held on a sample table 2 provided on a scanner 3 having a substantially cylindrical shape.
- the scanner 3 includes an XY scanner 3a that scans the sample 1 in two directions of X and Y orthogonal to each other, and a Z scanner 3b that finely moves the sample 1 in the Z-axis direction orthogonal to the X and Y axes.
- the drive source is a piezoelectric element that is displaced by an applied voltage.
- a cantilever 4 having a probe 5 at its tip is disposed above the sample 1, and this cantilever 4 is vibrated by an excitation unit including a piezoelectric element (not shown).
- an optical displacement detector 10 including a laser light source 11, mirrors 13 and 14, and a photodetector 15 is provided above the cantilever 4.
- the laser light emitted from the laser light source 11 is reflected substantially vertically by the mirror 13 and is irradiated near the tip of the cantilever 4.
- the light reflected by the cantilever 4 is detected by the photodetector 15 via the mirror 14.
- the photodetector 15 has a light receiving surface divided into a plurality (usually two) in the displacement direction (Z axis direction) of the cantilever 4, or has a light receiving surface divided into four in the Z axis direction and the Y axis direction.
- the amount of displacement of the cantilever 4 can be calculated by calculating a detection signal corresponding to the plurality of received light amounts. .
- the measurement operation in the non-contact mode in the scanning probe microscope having the above configuration will be briefly described.
- the cantilever 4 is vibrated in the Z-axis direction at a frequency near the resonance point by an excitation unit (not shown).
- an attractive force or a repulsive force acts between the probe 5 and the surface of the sample 1
- the vibration amplitude of the cantilever 4 changes.
- a small change amount of the vibration amplitude is detected by a detection signal from the photodetector 15, and the sample 1 is moved in the Z-axis direction so that the change amount is zero, that is, the vibration amplitude is kept constant.
- the piezoelectric element of the scanner 3b is feedback controlled.
- the emission angle (emission direction) of the laser light emitted from the laser light source 11 may slightly change due to the influence of temperature change in the characteristics of the laser oscillation circuit.
- the variation in the emission angle of the laser beam occurs as described above, the following problem occurs.
- FIG. 6 is a diagram schematically showing a normal operation of the optical displacement detector 10.
- the probe 5 is scanning the flat surface on the sample 1
- a spot of the reflected light from the cantilever 4 is located at a position indicated by P on the light receiving surface of the photodetector 15 as shown in FIG. can get.
- the cantilever 4 bends upward as shown in FIG. 5B, and the spot position P of the reflected light on the light receiving surface of the photodetector 15 is downward. It is displaced to. Due to such displacement, the detection signal from the photodetector 15 changes, and information reflecting the height of the convex portion 1a and the like is obtained.
- FIG. 7 is a diagram schematically showing the operation when the emission direction of the laser light from the laser light source 11 is inclined upward.
- FIG. 7A when there is no inclination (shift) in the laser beam emission direction (in this example, the laser beam is emitted in the X-axis direction), the position indicated by P on the light receiving surface of the photodetector 15 A spot of reflected light from the cantilever 4 is obtained.
- the emission direction of the laser beam is slightly inclined upward due to the change in ambient temperature, the incident angle of the irradiation light Lm to the cantilever 4 also changes.
- the spot position P of the reflected light on the light receiving surface of the photodetector 15 is displaced downward, even though the probe 5 is scanning the flat surface on the sample 1. That is, on the light receiving surface of the photodetector 15, the state is the same as when the convex portion 1a is present on the surface of the sample 1 as shown in FIG. Therefore, when the laser beam emission direction (emission angle) changes as described above, it is erroneously recognized that there is a convex portion or a concave portion on the surface of the sample 1.
- the laser light source 11 that suppresses the change in the emission angle with respect to the temperature or the like is adopted, or a temperature control device that maintains the ambient temperature of the laser light source 11 constant is provided.
- a temperature control device that maintains the ambient temperature of the laser light source 11 constant is provided.
- the present invention has been made to solve the above-mentioned problems, and the object of the present invention is that even when a change occurs in the emission angle of the laser beam from the laser light source, it is unevenness on the sample surface.
- An object of the present invention is to provide a scanning probe microscope that can prevent erroneous recognition.
- the first invention made to solve the above-mentioned problems is a flexible cantilever provided with a probe, a light source unit for irradiating light to the cantilever, and the cantilever for the irradiated light.
- a scanning detector that detects the displacement of the cantilever based on positional information of the reflected light obtained by the photodetector when the probe scans the surface of the sample.
- the easiest way for the compensation means to control the light source unit is to change the posture (tilt) of the light source unit.
- An actuator such as a piezoelectric element can be used as a drive source for such changes.
- the second invention made to solve the above-mentioned problems is a flexible cantilever provided with a probe, a light source unit for irradiating light to the cantilever, and the cantilever for the irradiated light.
- a light detector for detecting reflected light from the probe, and when the probe scans the surface of the sample, scanning for obtaining displacement of the cantilever based on positional information of the reflected light obtained by the light detector
- Type probe microscope a) a light splitting unit that splits and extracts a light beam on the optical path of the irradiation light from the light source unit to the cantilever; b) Compensation light detection means for detecting the arrival position of the light split and extracted by the light splitting means; c) Recognizing a change in the emission angle of the light emitted from the light source unit according to the information obtained by the compensation light detection means, so that the influence of the change is reduced in the position information of the reflected light Compensation means for controlling the optical element inserted in the optical path of the i
- the optical element can be, for example, a single lens or a lens mechanism in which a plurality of lenses are combined, and the compensation means can control the position and angle of the lens mechanism.
- the compensation means can control the position and angle of the lens mechanism.
- an optical element capable of electrically changing optical characteristics can also be used.
- a third aspect of the present invention made to solve the above-described problems is a flexible cantilever provided with a probe, a light source unit for irradiating light to the cantilever, and the cantilever for the irradiated light.
- a light detector for detecting reflected light from the probe, and when the probe scans the surface of the sample, scanning for obtaining displacement of the cantilever based on positional information of the reflected light obtained by the light detector
- Type probe microscope a) a light splitting unit that splits and extracts a light beam on the optical path of the irradiation light from the light source unit to the cantilever; b) Compensation light detection means for detecting the arrival position of the light split and extracted by the light splitting means; c) moving means for moving at least one of the sample and the cantilever to change a relative distance; d) Recognizing a change in the emission angle of the light emitted from the light source unit according to the information obtained by the compensation light detection means, so that the influence of the change is
- the moving means can be, for example, a scanner that moves a sample and uses a piezoelectric element as a drive source.
- a fourth aspect of the present invention made to solve the above-described problems includes a flexible cantilever provided with a probe, a light source unit for irradiating light to the cantilever, and the cantilever for the irradiated light.
- a light detector for detecting reflected light from the probe, and when the probe scans the surface of the sample, scanning for obtaining displacement of the cantilever based on positional information of the reflected light obtained by the light detector
- Type probe microscope a) a light splitting unit that splits and extracts a light beam on the optical path of the irradiation light from the light source unit to the cantilever; b) Compensation light detection means for detecting the arrival position of the light split and extracted by the light splitting means; c) Recognizing a change in the emission angle of light emitted from the light source unit according to the information obtained by the compensation light detection means, and depending on the amount of change, the position information of the reflected light or the position information Compensation means for correcting data reflecting the irregularities and physical properties of
- a beam splitter such as a half mirror can be used as the light splitting means.
- a light detector such as a photodiode having a light receiving surface divided into a plurality of light receiving surfaces such as 2, 4 can be used.
- the said light source part is a laser light source normally.
- the incident angle of the irradiation light to the cantilever also changes.
- the arrival position of the light divided and extracted by the light dividing means changes on the light receiving surface of the compensation light detecting means, and the amount of change corresponds to the change in the emission angle.
- the light reception of the photodetector for detecting the displacement of the cantilever by correcting the change in the optical path due to the change in the emission angle of the emission light from the light source unit.
- the spot position of the reflected light obtained on the surface is prevented from shifting. In this case, by performing feedback control based on information obtained by the compensation light detection means, it is possible to eliminate the influence of fluctuations in the emission angle in almost real time.
- the amount of movement of the moving means that is feedback-controlled according to the change in the spot position of the reflected light on the light receiving surface of the photodetector is set. , Based on the information obtained by the compensation light detection means. Therefore, although the optical path of the light irradiated to the cantilever does not change, the influence of the variation of the emission angle of the emitted light does not appear in the spot position of the reflected light on the light receiving surface of the photodetector.
- the optical path of the irradiation light hitting the cantilever and the distance between the sample and the cantilever are not particularly changed.
- the change in the angle appears as it is as the change in the spot position of the reflected light on the light receiving surface of the photodetector. That is, the position information of the reflected light obtained by the photodetector at this time includes the influence of the change in the outgoing angle of the outgoing light.
- the degree of the influence can be quantitatively grasped based on the information obtained by the light detection means, for example, after the data reflecting the unevenness and physical properties of the sample surface is calculated, the change in the emission angle of the emitted light Correct the data according to the amount.
- the scanning probe microscope According to the scanning probe microscope according to the first to fourth inventions, even when the emission angle of light emitted from the light source unit varies due to factors such as changes in ambient temperature, the variation is caused by unevenness on the sample surface. It is no longer erroneously recognized as being present, and it is possible to create a surface image of the sample and measure the surface roughness with high accuracy. Further, as compared with the case where the temperature dependency of the emission angle is improved by the light source unit itself or the temperature of the light source unit is controlled, the cost can be suppressed and the effect is more certain. Furthermore, the same effect can be obtained even with respect to changes in the emission angle due to factors such as changes with time other than temperature.
- FIG. 1 is a configuration diagram of a main part of a scanning probe microscope according to the first embodiment.
- the same components as those already described in FIG. 5 are denoted by the same reference numerals and description thereof is omitted.
- a half mirror 20 corresponding to the light splitting means in the present invention is provided in the optical displacement detection unit 10 in place of the conventional mirror 13.
- the emitted light is divided into irradiation light Lm and monitor light Ls directed to the cantilever 4.
- the light receiving surface is divided into four along the two axis directions of the Y axis and the Z axis, which corresponds to the compensation light detection means in the present invention.
- An optical detector 21 is disposed.
- the laser light source 11 can be rotated within a predetermined angle range in the rotation direction around the Y axis and the rotation direction around the Z axis by an actuator 23 composed of a piezoelectric element or the like. Detection signals from the four light receiving surfaces 21a, 21b, 21c, and 21d of the photodetector 21 are input to the drive amount calculation unit 22, and the drive amount calculation unit 22 calculates the drive amount in the rotation direction around the Y axis and the Z axis. Then, the actuator 23 is controlled.
- the drive amount calculation unit 22 sets the drive amount to zero, and the actuator 23 does not operate.
- the position of the light spot Q by the monitor light Ls on the light receiving surface of the photodetector 21 is, for example, It moves as shown in FIG.
- the amount of movement of the light spot Q at this time corresponds to the magnitude of the inclination in the light emission direction, and the movement direction corresponds to the direction of inclination. Therefore, the drive amount calculation unit 22 calculates the drive amount that recognizes the magnitude and direction of the inclination of the light emission direction and can cancel the result by calculating the four detection signals.
- a drive signal corresponding to the obtained drive amount is sent to the actuator 23 to control the displacement amount of the actuator 23.
- the attitude of the laser light source 11 changes due to the displacement of the actuator 23, and the direction of the emitted light from the laser light source 11 approaches the X-axis direction.
- the position of the light spot Q of the monitor light Ls on the light receiving surface of the photodetector 21 approaches the state shown in FIG. In this state, if there is an error from the state of FIG. 8A, the driving amount is further corrected, and the light spot Q is adjusted to the state of FIG. 8A.
- the light emission direction from the laser light source 11 can be made to coincide with the X-axis direction. Thereby, the influence of the inclination of the light emission direction from the laser light source 11 is eliminated.
- the photodetector 21 with the light receiving surface divided into four parts is used as described above, the inclination of the emitted light in any direction can be detected.
- the direction of the inclination is limited due to the characteristics of the laser light source 11.
- a light detector 21 having a light receiving surface divided into two can be used.
- FIG. 2 is a configuration diagram of a main part of a scanning probe microscope according to the second embodiment.
- the same components as those already described in FIGS. 1 and 5 are denoted by the same reference numerals, and description thereof is omitted.
- the deviation (tilt) of the emission direction of the emitted light is compensated by controlling the attitude of the laser light source 11 itself.
- the laser light source 11 is fixed.
- the lens 25 inserted in the optical path between the laser light source 11 and the half mirror 20 can be moved by the actuator 24 in the Y-axis and Z-axis directions.
- the lens 25 may be a single lens, but if a lens group is formed by combining a plurality of lenses and one to a few lenses are moved, the direction of the emitted light from the laser light source 11 is X. Even when tilted from the axial direction, it becomes easy to correct the tilt and make it incident on the half mirror 20 along the X-axis direction.
- the lens 25 may be rotated as in the first embodiment.
- FIG. 3 is a configuration diagram of a main part of a scanning probe microscope according to the third embodiment.
- the same components as those already described in FIGS. 1 and 5 are denoted by the same reference numerals, and description thereof is omitted.
- the drive amount calculation unit 16 obtains a minute change amount of the vibration amplitude of the cantilever 4 based on the detection signal from the photodetector 15, and obtains a drive amount Ka that makes this change amount zero, that is, keeps the vibration amplitude constant. .
- the driving unit 17 feedback-controls the piezoelectric element of the Z scanner 3b so as to move the sample 1 in the Z-axis direction according to the driving amount Ka.
- the drive amount calculation unit 30 calculates the deviation amount of the outgoing angle of the outgoing light in the Z-axis direction based on the four detection signals of the photodetector 21, and calculates it.
- a compensation driving amount Kb that cancels out is calculated.
- the adder 31 subtracts the compensation drive amount Kb from the drive amount Ka, and the drive unit 17 drives the piezoelectric element of the Z scanner 3b with the drive amount Ka-Kb.
- the amount of displacement of the sample 1 in the Z-axis direction by the Z scanner 3b changes so as to reduce the influence of the tilt in the direction of light emission from the laser light source 11.
- the feedback control is performed in the same manner as in the first and second embodiments, so that the influence of the inclination of the direction of light emission from the laser light source 11 can be minimized.
- control responsiveness is poor.
- the change in the direction of light emission from the laser light source 11 occurs gradually, it is possible to sufficiently follow such a slow change.
- FIG. 4 is a configuration diagram of a main part of a scanning probe microscope according to the fourth embodiment.
- the same components as those already described in FIGS. 1 and 5 are denoted by the same reference numerals, and description thereof is omitted.
- the feedback control as in the first to third embodiments is not performed, and an error amount corresponding to the change in the direction of the light emitted from the laser light source 11 is considered in data processing. It is corrected with. That is, the detection signal of the photodetector 15 is converted into digital data by the A / D converter 40 and input to the unevenness data calculation processing unit 43 included in the data processing unit 42.
- the unevenness data calculation processing unit 43 included in the data processing unit 42.
- data reflecting the unevenness of the surface of the sample 1 is calculated, but when the direction of the light emitted from the laser light source 11 changes, an error is included with the change.
- the detection signal of the photodetector 21 is converted into digital data by the A / D converter 41 and input to the emission angle data calculation processing unit 44 included in the data processing unit 42.
- the emission angle data calculation processing unit 44 calculates error data associated with a change in direction of light emitted from the laser light source 11. Therefore, for example, as shown in FIG. 8A, when there is no change in the emission angle, the error data calculated by the emission angle data calculation processing unit 44 is zero.
- the correction processing unit 45 subtracts the error data from the data obtained by the concavo-convex data calculation processing unit 43 to perform the correction to remove the influence of the direction change of the emitted light, and outputs the corrected data to obtain the accuracy.
- a high sample surface image is displayed on the display unit 46.
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Abstract
Description
a)前記光源部から前記カンチレバーまでの照射光の光路上で光束を分割して取り出す光分割手段と、
b)前記光分割手段により分割して取り出された光の到達位置を検出する補償用光検出手段と、
c)前記補償用光検出手段により得られる情報に応じて前記光源部から出射される光の出射角の変化を認識し、前記反射光の位置情報において前記変化の影響が軽減されるように前記光源部を制御する補償手段と、
を備えることを特徴としている。
a)前記光源部から前記カンチレバーまでの照射光の光路上で光束を分割して取り出す光分割手段と、
b)前記光分割手段により分割して取り出された光の到達位置を検出する補償用光検出手段と、
c)前記補償用光検出手段により得られる情報に応じて前記光源部から出射される光の出射角の変化を認識し、前記反射光の位置情報において前記変化の影響が軽減されるように前記照射光の光路中に挿入された光学素子を制御する補償手段と、
を備えることを特徴としている。
a)前記光源部から前記カンチレバーまでの照射光の光路上で光束を分割して取り出す光分割手段と、
b)前記光分割手段により分割して取り出された光の到達位置を検出する補償用光検出手段と、
c)前記試料と前記カンチレバーとの相対的な距離を変化させるべく少なくともいずれか一方を移動させる移動手段と、
d)前記補償用光検出手段により得られる情報に応じて前記光源部から出射される光の出射角の変化を認識し、前記反射光の位置情報において前記変化の影響が軽減されるように前記移動手段を制御する補償手段と、
を備えることを特徴としている。
a)前記光源部から前記カンチレバーまでの照射光の光路上で光束を分割して取り出す光分割手段と、
b)前記光分割手段により分割して取り出された光の到達位置を検出する補償用光検出手段と、
c)前記補償用光検出手段により得られる情報に応じて前記光源部から出射される光の出射角の変化を認識し、その変化量に応じて、前記反射光の位置情報又は該位置情報に基づいて得られる試料表面の凹凸や物性を反映したデータを補正する補償手段と、
を備えることを特徴としている。
2…試料台
3…スキャナ
3a…XYスキャナ
3b…Zスキャナ
4…カンチレバー
5…探針
10…光学的変位検出部
11…レーザ光源
14…ミラー
15…光検出器
17…駆動部
20…ハーフミラー
21…補償用光検出器
21a、21b、21c、21d…受光面
16、22、30…駆動量演算部
23、24…アクチュエータ
31…加算部
40、41…A/D変換器
42…データ処理部
43…凹凸データ算出処理部
44…出射角データ算出処理部
45…補正処理部
46…表示部
まず第1発明の一実施例(第1実施例)である走査型プローブ顕微鏡について、図面を参照して具体的に説明する。図1は第1実施例による走査型プローブ顕微鏡の要部の構成図である。既に説明した図5中に記載の構成要素と同一の構成要素には同一の符号を付して説明を略す。
次に第2発明の一実施例(第2実施例)である走査型プローブ顕微鏡について、図面を参照して具体的に説明する。図2は第2実施例による走査型プローブ顕微鏡の要部の構成図である。既に説明した図1、図5中に記載の構成要素と同一の構成要素には同一の符号を付して説明を略す。
次に第3発明の一実施例(第3実施例)である走査型プローブ顕微鏡について、図面を参照して具体的に説明する。図3は第3実施例による走査型プローブ顕微鏡の要部の構成図である。既に説明した図1、図5中に記載の構成要素と同一の構成要素には同一の符号を付して説明を略す。
次に第4発明の一実施例(第4実施例)である走査型プローブ顕微鏡について、図面を参照して具体的に説明する。図4は第4実施例による走査型プローブ顕微鏡の要部の構成図である。既に説明した図1、図5中に記載の構成要素と同一の構成要素には同一の符号を付して説明を略す。
Claims (4)
- 探針が設けられた可撓性を有するカンチレバーと、前記カンチレバーに対し光を照射するための光源部と、その照射光に対する前記カンチレバーからの反射光を検出する検出器と、を具備し、前記探針が試料表面を走査する際に、前記検出器により得られる反射光の位置情報に基づいて前記カンチレバーの変位を求める走査型プローブ顕微鏡において、
a)前記光源部から前記カンチレバーまでの照射光の光路上で光束を分割して取り出す光分割手段と、
b)前記光分割手段により分割して取り出された光の到達位置を検出する光検出手段と、
c)前記光検出手段により得られる情報に応じて前記光源部から出射される光の出射角の変化を認識し、前記反射光の位置情報における前記変化の影響が軽減されるように前記光源部を制御する補償手段と、
を備えることを特徴とする走査型プローブ顕微鏡。 - 探針が設けられた可撓性を有するカンチレバーと、前記カンチレバーに対し光を照射するための光源部と、その照射光に対する前記カンチレバーからの反射光を検出する検出器と、を具備し、前記探針が試料表面を走査する際に、前記検出器により得られる反射光の位置情報に基づいて前記カンチレバーの変位を求める走査型プローブ顕微鏡において、
a)前記光源部から前記カンチレバーまでの照射光の光路上で光束を分割して取り出す光分割手段と、
b)前記光分割手段により分割して取り出された光の到達位置を検出する光検出手段と、
c)前記光検出手段により得られる情報に応じて前記光源部から出射される光の出射角の変化を認識し、前記反射光の位置情報における前記変化の影響が軽減されるように前記照射光の光路中に挿入された光学素子を制御する補償手段と、
を備えることを特徴とする走査型プローブ顕微鏡。 - 探針が設けられた可撓性を有するカンチレバーと、前記カンチレバーに対し光を照射するための光源部と、その照射光に対する前記カンチレバーからの反射光を検出する検出器と、を具備し、前記探針が試料表面を走査する際に、前記検出器により得られる反射光の位置情報に基づいて前記カンチレバーの変位を求める走査型プローブ顕微鏡において、
a)前記光源部から前記カンチレバーまでの照射光の光路上で光束を分割して取り出す光分割手段と、
b)前記光分割手段により分割して取り出された光の到達位置を検出する光検出手段と、
c)前記試料と前記カンチレバーとの相対的な距離を変化させるべく少なくともいずれか一方を移動させる移動手段と、
d)前記光検出手段により得られる情報に応じて前記光源部から出射される光の出射角の変化を認識し、前記反射光の位置情報における前記変化の影響が軽減されるように前記移動手段を制御する補償手段と、
を備えることを特徴とする走査型プローブ顕微鏡。 - 探針が設けられた可撓性を有するカンチレバーと、前記カンチレバーに対し光を照射するための光源部と、その照射光に対する前記カンチレバーからの反射光を検出する検出器と、を具備し、前記探針が試料表面を走査する際に、前記検出器により得られる反射光の位置情報に基づいて前記カンチレバーの変位を求める走査型プローブ顕微鏡において、
a)前記光源部から前記カンチレバーまでの照射光の光路上で光束を分割して取り出す光分割手段と、
b)前記光分割手段により分割して取り出された光の到達位置を検出する光検出手段と、
c)前記光検出手段により得られる情報に応じて前記光源部から出射される光の出射角の変化を認識し、その変化量に応じて、前記反射光の位置情報又は該位置情報に基づいて得られる試料表面の凹凸や物性を反映したデータを補正する補償手段と、
を備えることを特徴とする走査型プローブ顕微鏡。
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CN2008801255068A CN101952706B (zh) | 2008-01-24 | 2008-01-24 | 扫描探针显微镜 |
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Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN103454454A (zh) * | 2013-08-30 | 2013-12-18 | 哈尔滨工业大学 | 用于双探针原子力显微镜的激光测力系统 |
Families Citing this family (21)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP5931537B2 (ja) * | 2012-03-28 | 2016-06-08 | 東レエンジニアリング株式会社 | レーザの光軸アライメント方法およびそれを用いたレーザ加工装置 |
JP2016520216A (ja) * | 2013-05-23 | 2016-07-11 | アプライド マテリアルズ イスラエル リミテッド | 評価システムおよび基板を評価する方法 |
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JP2016128788A (ja) * | 2015-01-09 | 2016-07-14 | キヤノン株式会社 | プローブ変位計測装置、およびそれを有するイオン化装置、質量分析装置、情報取得システム |
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EP3324194B1 (en) * | 2016-11-22 | 2019-06-26 | Anton Paar GmbH | Imaging a gap between sample and probe of a scanning probe microscope in substantially horizontal side view |
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GB201705613D0 (en) * | 2017-04-07 | 2017-05-24 | Infinitesima Ltd | Scanning probe system |
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Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH07134132A (ja) * | 1993-11-10 | 1995-05-23 | Olympus Optical Co Ltd | 走査型プローブ顕微鏡 |
US5560244A (en) * | 1993-08-17 | 1996-10-01 | Digital Instruments, Inc. | Scanning stylus atomic force microscope with cantilever tracking and optical access |
JPH10104245A (ja) * | 1996-09-27 | 1998-04-24 | Nikon Corp | 微小変位測定装置 |
JPH1194854A (ja) * | 1997-07-24 | 1999-04-09 | Olympus Optical Co Ltd | 走査型プローブ顕微鏡 |
JP2005118815A (ja) * | 2003-10-16 | 2005-05-12 | Hitachi Via Mechanics Ltd | レーザ加工方法およびレーザ加工装置 |
Family Cites Families (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH05256641A (ja) * | 1992-03-11 | 1993-10-05 | Olympus Optical Co Ltd | カンチレバー変位検出装置 |
JP2936311B2 (ja) * | 1994-09-09 | 1999-08-23 | セイコーインスツルメンツ株式会社 | 液中観察機能付き走査型近視野原子間力顕微鏡 |
JP4658452B2 (ja) * | 2003-02-07 | 2011-03-23 | オリンパス株式会社 | 光学式エンコーダ |
JP2005233669A (ja) | 2004-02-17 | 2005-09-02 | Shimadzu Corp | 走査型プローブ顕微鏡 |
JP2006329973A (ja) * | 2005-04-28 | 2006-12-07 | Hitachi Ltd | 走査プローブ顕微鏡およびこれを用いた試料観察方法およびデバイス製造方法 |
-
2008
- 2008-01-24 CN CN2008801255068A patent/CN101952706B/zh not_active Expired - Fee Related
- 2008-01-24 JP JP2009550375A patent/JP4873081B2/ja not_active Expired - Fee Related
- 2008-01-24 WO PCT/JP2008/000078 patent/WO2009093284A1/ja active Application Filing
- 2008-01-24 US US12/864,491 patent/US8321960B2/en not_active Expired - Fee Related
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5560244A (en) * | 1993-08-17 | 1996-10-01 | Digital Instruments, Inc. | Scanning stylus atomic force microscope with cantilever tracking and optical access |
JPH07134132A (ja) * | 1993-11-10 | 1995-05-23 | Olympus Optical Co Ltd | 走査型プローブ顕微鏡 |
JPH10104245A (ja) * | 1996-09-27 | 1998-04-24 | Nikon Corp | 微小変位測定装置 |
JPH1194854A (ja) * | 1997-07-24 | 1999-04-09 | Olympus Optical Co Ltd | 走査型プローブ顕微鏡 |
JP2005118815A (ja) * | 2003-10-16 | 2005-05-12 | Hitachi Via Mechanics Ltd | レーザ加工方法およびレーザ加工装置 |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN103454454A (zh) * | 2013-08-30 | 2013-12-18 | 哈尔滨工业大学 | 用于双探针原子力显微镜的激光测力系统 |
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US8321960B2 (en) | 2012-11-27 |
US20110113515A1 (en) | 2011-05-12 |
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