Abstract: A method of scanning a sample with a scanning probe system, the scanning probe system comprising a probe comprising a cantilever extending from a base to a free end, and a probe tip carried by the free end of the cantilever, the method comprising using the probe to measure an electrostatic interaction between the sample and the probe; and after measuring the electrostatic interaction between the sample and the probe, scanning the sample with the probe while simultaneously applying a bias voltage to the scanning probe system, the applied bias voltage based on the measured electrostatic interaction between the sample and the probe.

Abstract: A method for optimizing loop gain of an atomic force microscope (AFM) apparatus includes determining a change in gain of the physical system and adjusting a controller frequency response of the controller in an AFM loop to compensate for the determined change in gain. The AFM loop has a corresponding loop response that includes the product of the controller frequency response and a physical system response of the physical system.

Abstract: Height control systems and/or methods are implemented for dynamic force tunneling microscopy and single electron tunneling force spectroscopy to improve their accuracy.

Abstract: The present invention relates to a method for controlling a scanning probe microscope having a probe (2) with a tip (21) for interacting with a sample (4), and a nanoscanner (1) for retaining the sample (4) or the probe (2), comprising the steps of monitoring the extension of the piezo element (1) along a first direction (R) along which the tip (21) is moved towards the sample (4), and adjusting the level of the probe (2) along the first direction (R) by means of an additional actuator (3), when the nanoscanner (1) exhibits an extension below or above a threshold value. The invention further relates to a device (100) for controlling a scanning probe microscope.

Abstract: A probe alignment tool (10) for scanning probe microscopes utilizes an attached relay optics to view the scanning probe microscope probe tip (40) and align its image in the center of the field of view of an optical microscope (36). Adjustments to optical microscope motorized stages (50) and (60) along with adjustments of scanning probe microscope stages (44), (46) and (58) allow determination of a path and distance from the center of the field of view to the probe tip (40). From such determination a target area to be examined by the scanning probe microscope may be positioned precisely and accurately under the probe tip (40). Replacement of a scanning probe microscope probe tip (40) in an atomic force microscope unit (42) may be accomplished without the loss of alignment measurements.

Abstract: A technique for actively damping internal vibrations in a scanning probe microscope is disclosed. The excitation of various mechanical movements, including resonances, in the mechanical assembly of an SPM can adversely effect its performance, especially for high speed applications. An actuator is used to compensate for the movements. The actuator may operate in only the z direction, or may operate in other directions. The actuator(s) may be located at positions of antinodes.

Abstract: An atomic force microscope (AFM) system comprises a cantilever arm attached to a probe tip. The system controls a height of the cantilever arm to press the probe tip against a sample and then separate the probe tip from the sample, to detect a disturbance of the cantilever arm after the separation of the probe tip from the surface, and to engage active damping of the cantilever arm to suppress the disturbance.

Abstract: During a measurement in KFM mode of the surface potential of a material (P), a detection point (1) is arranged above a surface (S) of the material. Two piezoelectric actuators (2, 5) are used to monitor a mean distance of the detection point relative to the surface of the material and a mechanical oscillation of said point. During the measurement, a control voltage is applied between control electrodes (2a, 2b) of the piezoelectric actuator (2) which is dedicated to the mechanical oscillation of the detection point (1), said control voltage not having an alternative component to an angular frequency of electrical energization of said detection point. A result of the KFM measurement is therefore separate from operating parameters such as a projection angle used to perform closed-loop control and a value of the angular frequency of electrical energization. The invention thus provides absolute measurements of surface potentials.

Abstract: A control system 32, 75 is for use with a scanning probe microscope of a type in which measurement data is collected at positions within a scan pattern described as a probe and sample are moved relative to each other. The control system is used in conjunction with a position detection system 34 that measures the position of at least one of the probe and sample such that their relative spatial location (x, y) is determined. Measurement data may then be correlated with empirically-determined spatial locations in constructing an image. The use of empirical location data means that image quality is not limited by the ability of a microscope scanning system to control mechanically the relative location of probe and sample.

Abstract: An apparatus is provided and includes a cantilever having a tip at a distal end thereof disposed with the tip positioned an initial distance from a sample and a circuit electrically coupled to a substrate on which the sample is layered and the cantilever to simultaneously apply direct and alternating currents to deflect the cantilever and to cause the tip to oscillate about a point at a second distance from the sample, which is shorter than the initial distance, between first positions, at which the tip contacts the sample, and second positions, at which the tip is displaced from the sample.

Abstract: An electronic control device for a local probe with a piezoelectric resonator and preamplification and processing of its signals, the probe being configured for local measurement of physical properties of a sample in an environment with a particle beam directed towards the probe, in which an excitation voltage generated by an excitation mechanism is applied to the piezoelectric resonator through a first galvanic isolation transformer, and a current for measurement of mechanical oscillations of the piezoelectric resonator is applied through a second galvanic isolation transformer to a preamplification device on the output side.

Abstract: A system includes a displacement sensor, an actuator connected to the displacement sensor, and a feedback unit. The displacement sensor is configured to measure at least one of a relative position and a relative orientation between the displacement sensor and the target object. The feedback unit receives a signal from the displacement sensor related to the measured relative position or relative orientation and controls the actuator to move the displacement sensor on the basis of variations in the received signal arising due to a change in environmental conditions.

Abstract: An optimal input design method and apparatus to achieve rapid broadband nanomechanical measurements of soft materials using the indentation-based method for the investigation of fast evolving phenomenon, such as the crystallization process of polymers, the nanomechanical measurement of live cell during cell movement, and force volume mapping of nonhomogeneous materials, are presented. The indentation-based nanomechanical measurement provides unique quantification of material properties at specified locations. Particularly, an input force profile with discrete spectrum is optimized to maximize the Fisher information matrix of the linear compliance model of the soft material.

Abstract: A probe detection system (74) for use with a scanning probe microscope comprises both a height detection system (88) and deflection detection system (28). As a sample surface is scanned, light reflected from a microscope probe (16) is separated into two components. A first component (84) is analysed by the deflection detection system (28) and is used in a feedback system that maintains the average probe deflection substantially constant during the scan. The second component (86) is analysed by the height detection system (88) from which an indication of the height of the probe above a fixed reference point, and thereby an image of the sample surface, is obtained. Such a dual detection system is particularly suited for use in fast scanning applications in which the feedback system is unable to respond at the rate required to adjust probe height between pixel positions.

Abstract: It has been difficult to highly accurately measure the profiles of samples using scanning probe microscopes at the time when scanning is performed due to scanning mechanism fluctuations in the non drive direction, i.e., vertical direction. The present invention is provided with, on the rear side of a sample stage, a high-accuracy displacement gauge for measuring fluctuation in the non drive direction, i.e., vertical direction, at the time when the sample stage is being scanned in the horizontal directions, and as a result, highly accurate planarity evaluation with accuracy of sample nm-order or less is made possible by correcting sample surface shape measurement results obtained using a probe.

Abstract: A dynamic probe detection system (29,32) is for use with a scanning probe microscope of the type that includes a probe (18) that is moved repeatedly towards and away from a sample surface. As a sample surface is scanned, an interferometer (88) generates an output height signal indicative of a path difference between light reflected from the probe (80a,80b,80c) and a height reference beam. Signal processing apparatus monitors the height signal and derives a measurement for each oscillation cycle that is indicative of the height of the probe. This enables extraction of a measurement that represents the height of the sample, without recourse to averaging or filtering, that may be used to form an image of the sample. The detection system may also include a feedback mechanism that is operable to maintain the average value of a feedback parameter at a set level.

Abstract: Methods and apparatus are described for scanning probe microscopy. A method includes generating a band excitation (BE) signal having finite and predefined amplitude and phase spectrum in at least a first predefined frequency band; exciting a probe using the band excitation signal; obtaining data by measuring a response of the probe in at least a second predefined frequency band; and extracting at least one relevant dynamic parameter of the response of the probe in a predefined range including analyzing the obtained data. The BE signal can be synthesized prior to imaging (static band excitation), or adjusted at each pixel or spectroscopy step to accommodate changes in sample properties (adaptive band excitation).

Abstract: An atomic force microscope (AFM) comprises a physical system and a controller comprising a plurality of digital filters and configured to control the physical system. The AFM is tuned by performing automatic loop shaping on a loop response defined by a frequency response of the physical system and a frequency response of the controller, and adjusting a gain of the controller according to a peak in a magnitude of the loop response.

Abstract: Provided are an AFM measuring method and a system thereof. The tip of a cantilever is provided to a plurality of points on a substrate, to which incident light is radiated from a light source. Scattered light is generated between the tip of the cantilever and the substrate by the incident light and the intensity of the scattered light is measured. The measured intensity of the scattered light is input to a data processing unit so as to find a point where the intensity of the incident is highest. The tip of the cantilever is moved to the point where the intensity of the incident light is highest.

Abstract: The present invention provides a fast-operating and stable scanning probe microscope configured to detect the interaction between a probe and a sample to avoid generation of a harmonic component. An oscillation circuit (31) generates an excitation phase signal indicative of the phase of an excitation signal. An excitation signal generation circuit (33) generates an excitation signal from the excitation phase signal. A complex signal generation circuit (35) generates a complex signal from a displacement signal. A vector calculation circuit (37) calculates the argument of the complex signal. A subtracting phase comparator (39) compares the argument with the phase of the excitation phase signal by subtraction. The amount of the interaction between a probe device and a sample is obtained using the subtracting phase comparator (39). The result of the comparison carried out by the subtracting phase comparator (39) may be output as a difference in phase between the displacement signal and the excitation signal.

Abstract: The invention relates to a method and to a device for examining a test sample using a scanning probe microscope. According to the method a first and a second measurement using a scanning probe microscope are carried out on the test sample using a measuring probe system in which a measuring probe and another measuring probe are formed on a common measuring probe receptacle. During the first measurement, in relation to the test sample, the measuring probe is held in a first measurement position and the other measuring probe is held in another non-measurement position, and the test sample is examined with the measuring probe using a scanning probe microscope. After the first measurement, by displacing in relation to the test sample, the measuring probe is displaced from the measurement position into a non-measurement position and the other measuring probe from the other non-measurement position into another measurement position.

Abstract: A control system 32, 75 is for use with a scanning probe microscope of a type in which measurement data is collected at positions within a scan pattern described as a probe and sample are moved relative to each other. The control system is used in conjunction with a position detection system 34 that measures the position of at least one of the probe and sample such that their relative spatial location (x, y) is determined. Measurement data may then be correlated with empirically-determined spatial locations in constructing an image. The use of empirical location data means that image quality is not limited by the ability of a microscope scanning system to control mechanically the relative location of probe and sample.

Abstract: A method includes generating, using a sensor, a data signal. The data signal includes a first component based on a motion in a first direction of an actuator configured to provide motion between a sample and a probe in the first direction, the first direction substantially in the plane of the sample; and a second component based on at least one of topographic variations of the sample in a second direction, and a materials property of the sample. The method further includes generating, using a processor, a compensatory signal based on the first component of the data signal generated by the sensor; and providing the compensatory signal to the actuator.

Abstract: A portion of light emitted from a laser source (11) for detecting a displacement of a cantilever (4) is extracted by a half mirror (20) and guided onto a photodetector (21) having a light-receiving surface divided into four sections. When the direction of the emitted light is inclined due to a change in the ambient temperature or other factors, the light spot formed on the light-receiving surface of the photodetector (21) moves. Accordingly, the amount and direction of the inclination of the emission direction can be recognized from the amount and direction of the movement of the light spot. A drive amount calculator (22) calculates a drive amount according to the amount and direction of the inclination, and operates an actuator (23) to rotate the laser source (11) around each of the Y and Z axes. This operation compensates for the inclination of the direction of the emitted light and thereby prevents the inclination from being falsely recognized as an irregularity on the sample surface.

Abstract: An atomic force microscopy (AFM) method includes a scanning probe that scans a surface of a structure to produce a first structure image. The structure is then rotated by 90° with respect to the scanning probe. The scanning probe scans the surface of the structure again to produce a second structure image. The first and second structure images are combined to produce best fit image of the surface area of the structure. The same method is used to produce the best fit image of a flat standard. The best fit image of the flat standard is subtracted from the best fit image of the structure to obtain a true topographical image in which Z direction run out error is substantially reduced or eliminated.

Abstract: An apparatus for atomic force microscopy (AFM) comprises a first actuator configured to move a cantilever along an axis; a second actuator configured to move the cantilever along the axis; an amplifier; and a crossover network connected between the amplifier, and the first actuator and the second actuator. The crossover network is adapted to provide a first drive signal to the first actuator over a first frequency range and to provide a second drive signal to the second actuator over a second frequency range.

Abstract: A method, system, device, and software for automatically determining PI feedback parameters in a scanning probe microscopy application setup using an iterative feedback tuning process.

Abstract: Incident light 19 emitted from a laser light source 18 is reflected on an upper surface of a cantilever 13, so that reflected light 19a enters light detection means 20. Since the incident light 19 and the reflected light 19a are in a plane not including a long axis of the cantilever 13, movements of the reflected light 19a due to change in a deflection amount ? of the cantilever 13 and due to change in a fine vertical movement amount z thereof are different in direction on the light detection means 20. This enables the change in the deflection amount ? of the cantilever 13 and the change in the fine vertical movement amount z thereof to be separated from output of the light detection means 20.

Abstract: A The local probe microscopy apparatus (1) comprises a probe (3) with translation stages (5a, 5b) for controlling the position of the probe (3) relative to a sample surface. The probe (3) has a feedback mechanism (6, 5 7) for maintaining the deflection of the probe and a height measuring system (9) which includes means for compensating for environmental noise. The local probe microscopy apparatus is particularly suitable for use as a wafer inspection tool in a wafer fabrication plant where the inspection tool is liable to be exposed to significant mechanical vibration.

Abstract: A scanning probe microscope and method of operation for monitoring and assessing proper tracking between the tip and sample, as well as automating at least some aspects of AFM setup previously done manually. Preferably, local slopes corresponding to the acquired data are compared to determine a tracking metric that is self-normalizing.

Abstract: A control system (32, 75) is for use with a scanning probe microscope of a type in which measurement data is collected at positions within a scan pattern described as a probe and sample are moved relative to each other. The control system is used in conjunction with a position detection system (34) that measures the position of at least one of the probe and sample such that their relative spatial location (x, y) is determined. Measurement data may then be correlated with empirically-determined spatial locations in constructing an image. The use of empirical location data means that image quality is not limited by the ability of a microscope scanning system to control mechanically the relative location of probe and sample.

Abstract: Linear PID controllers have a transfer function that resembles the frequency response of a notch filter. The PID parameters, KP, KI, and KD (proportional, integral, and derivative gains, respectively) can be extracted from the parameters of a linear notch filter. The linearized modes of scanning probe microscope (SPM) actuators have frequency responses that resemble those of simple second order resonance. Reasonable feedback control can be achieved by an inverse dynamics model of the resonance. A properly parameterized notch filter can cancel the dynamics of a resonance to give good closed-loop response.

Abstract: There is provided a scanning probe microscope that allows active damping to be advantageously carried out. A Z scan control section functions as a driving control section to control a Z scanner that is a controlled object. Driving control is performed by supplying the controlled object with a driving signal processed by an adjustment function. The adjustment function adjusts the driving signal by using a simulated transfer function that simulates an actual transfer function indicative of an actual frequency characteristic of the controlled object so that executing processing of the simulated transfer function on the adjusted driving signal results in decrease of vibration of an output signal from the simulated transfer function.

Abstract: A scanning probe microscope is provided, which can be stably used for a long time even if excitation efficiency varies during scan. A cantilever (5) is excited, and the cantilever (5) and a sample are subjected to relative scanning. A second-harmonic component detection circuit (31) detects second-harmonic component amplitude of oscillation of the cantilever (5) as integral-multiple component amplitude. The second-harmonic component amplitude is amplitude of a second-harmonic component having a frequency twice as high as excitation frequency. An excitation intensity adjustment circuit (33) controls excitation intensity based on the detected second-harmonic component amplitude such that the second-harmonic component amplitude is kept constant.

Abstract: Disclosed herein are an automatic landing method for a scanning probe microscope and an automatic landing apparatus using the same. The method comprises irradiating light to a cantilever using a light source; collecting interference fringes generated by the light being diffracted from the edge of the cantilever and then being incident to a surface of the sample; driving the tip in the sample direction until the pattern of the interference fringes reaches a predetermined pattern region (first driving); and driving the tip in the sample direction after the interference fringe pattern reached the predetermined pattern region (second driving). The method in accordance with the present invention is very effective particularly for samples having a large surface area, because it enables automatic landing of a tip according to recognition and selection of an optimal time point for individual landing steps, irrespective of adverse changes in landing conditions, such as surface irregularities of samples.

Abstract: An actuator subsystem for use in a scanning probe microscope (SPM) system having a probe for measuring a sample comprises and actuator and an actuator driving circuit. The actuator operates in the SPM system to generate relative motion between the probe and the sample while the SPM system collects data indicative of a property of the sample. The relative motion includes a range of motion of at least 1 micron. The actuator driving circuit applies a drive signal to the actuator to cause the relative motion, and has a small signal bandwidth of at least 200 kHz with a phase lag of not more than 100 degrees within the small signal bandwidth.

Abstract: To realize to adapt to a shape of a surface, shorten a measurement time period and promote a measurement accuracy by setting a sampling interval in accordance with a slope of the shape of the surface and controlling a stylus in accordance with the interval, there is provided a scanning probe microscope, in which in scanning the stylus, an observation data immediately therebefore is stored as a history, the sampling interval in X or Y direction is set at each time based on a shape of the observation data, and the stylus is scanned to a successive sampling position.

Abstract: A method of operating a scanning probe microscope (SPM) includes scanning a sample as a probe of the SPM interacts with a sample, and collecting sample surface data in response to the scanning step. The method identifies a feature of the sample from the sample surface data and automatically performs a zoom-in scan of the feature based on the identifying step. The method operates to quickly identify and confirm the location of features of interest, such as nano-asperities, so as to facilitate performing a directed high resolution image of the feature.

Abstract: An system for the measurement, analysis, and imaging of objects and surfaces in a variety of sizes is provided. In the most general terms, the invention relates to a device capable of measuring an object using a combination of low-resolution optical, high-resolution optical, SPM/AFM and/or material analysis techniques. The data gathered at various resolutions is correlated to absolute locations on the object's surface, allowing selected regions of the object's surface to be analyzed to any desired degree of precision (down to atomic scale). In a specific embodiment of the present invention, a system for collecting measurement data regarding an object of interest is disclosed. The system includes a sample stage adapted to hold the object of interest. The system further includes an optical lens assembly disposed above the sample stage. The optical lens assembly is configured to capture an optical image of the object of interest.

Abstract: A method and apparatus of scanning a sample with a scanning probe microscope including scanning a surface of the sample according to at least one scan parameter to obtain data corresponding to the surface, and substantially automatically identifying a transition in the surface. Based on the identified transition, the sample is re-scanned. Preferably, the resultant data is amended with data obtained by re-scanning the transition.

Abstract: A scanning probe microscope capable of preventing contact between the probe and a sample and a method of operating this microscope. The scanning probe microscope measures the topography of a surface of the sample by scanning the probe relative to the surface of the sample. A scanning reference position in the heightwise direction is updated in response to a maximum value of the height of the surface of the sample on the scan lines scanned so far. A limit value is set for motion of the probe in the heightwise direction relative to the scanning reference position. After the update, the next scan line is scanned. In this way, scanning is carried out along the successive scan lines.

Abstract: The present invention is directed toward devices comprising carbon nanotubes that are capable of detecting displacement, impact, stress, and/or strain in materials, methods of making such devices, methods for sensing/detecting/monitoring displacement, impact, stress, and/or strain via carbon nanotubes, and various applications for such methods and devices. The devices and methods of the present invention all rely on mechanically-induced electronic perturbations within the carbon nanotubes to detect and quantify such stress/strain. Such detection and quantification can rely on techniques which include, but are not limited to, electrical conductivity/conductance and/or resistivity/resistance detection/measurements, thermal conductivity detection/measurements, electroluminescence detection/measurements, photoluminescence detection/measurements, and combinations thereof. All such techniques rely on an understanding of how such properties change in response to mechanical stress and/or strain.

Abstract: Provided is a scanning probe microscope (SPM), a probe of which can be automatically replaced and the replacement probe can be attached onto an exact position. The SPM includes a first scanner that has a carrier holder, and changes a position of the carrier holder in a straight line; a second scanner changing a position of a sample on a plane; and a tray being able to store a spare carrier and a spare probe attached to the spare carrier. The carrier holder includes a plurality of protrusions.

Abstract: A drive stage for a scanning probe apparatus includes a supporting member, a plurality of movable portions fixed to the supporting member, and a plurality of drive elements configured and positioned to drive the plurality of movable portions. The drive stage is driven in a direction in which inertial forces of the plurality of movable portions are mutually canceled during drive of the plurality of drive elements. The drive stage further includes an inertial force difference detection member configured and positioned to detect a difference in inertial force between the plurality of movable portions, and an inertial force adjustment member configured and positioned to effect inertial force adjustment so that the difference in inertial force between the plurality of movable portions is decreased on the basis of a detection output of the inertial force detection member.

Abstract: To be able to measure a value with regard to a dissipation, or a value in proportion to a dissipation energy without making a premise by being brought into a steady state. Exciting means 12 for carrying out an excitation by following a resonance frequency of a cantilever 2, a displacement detector 10 for detecting a displacement of a stylus at a tip of the cantilever 2, an amplitude detector 20 for successively providing an amplitude from a signal from the displacement detector 10, a difference value detector 21 for providing a time difference value of the amplitude, a divider 22 for providing a value of a quotient between the time difference values, a logarithmic converter 23 for providing a logarithmic value of the value of the quotient, and a second divider 24 for providing a value with regard to a dissipation by calculating a value constituted by dividing the logarithmic value by a difference time period are provided.

Abstract: A method of position control for scanning probe spectroscopy of a specimen. Probe positional error is determined by comparing images generated from a sequence of scans to identify differences between positions of at least a portion of a reference characteristic of the specimen in the images. A probe is moved to a target location for spectroscopic analysis, as a function of the determined probe positional error.