<!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Archiving and Interchange DTD v1.0 20120330//EN" "JATS-archivearticle1.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta>
      <journal-title-group>
        <journal-title>Workshop on the Quantum Information Technologies, April</journal-title>
      </journal-title-group>
    </journal-meta>
    <article-meta>
      <title-group>
        <article-title>Analysis of metrological support of nano-measurements</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Volodymyr Kvasnikov</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Mariia Kataieva</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Victor Kobylyansky</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>National Aviation University</institution>
          ,
          <addr-line>1 Lubomyr Husar Ave., Kyiv, 03058</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <pub-date>
        <year>2021</year>
      </pub-date>
      <volume>11</volume>
      <issue>2021</issue>
      <fpage>110</fpage>
      <lpage>120</lpage>
      <abstract>
        <p>The article analyzes the existing methods and means of measuring objects in the nanometer range and develops their classification based on the main principles of use. The main parameters on which each described method is based are considered and the conditions for their most efective application are determined. It is proved that the chemical and electrical sets of properties of the nanomaterial can change when the particle size decreases to the nanometer size, which requires the inclusion of additional chemical and electrical tests in existing methods. Based on the analysis, it was determined that the most functional and universal in solving a wide range of problems is the method of scanning probe microscopy. The classification of existing methods of scanning probe microscopy based on the nature of their applications is developed. The main information parameters on which each described method is based are considered, and the conditions of their most efective application are determined. To increase the accuracy of nanomeasurements, a methodology based on the principle of integration of information provided by diferent methods has been developed. The use of the diferential-digital method is proposed, which includes the use of an additional information parameter in the mathematical model. An algorithm for including additional (a priory) information in the conditions for measuring the nanostructures has been developed, which leads the problem to the correct one according to the method of the control link, which characterizes the deviation of the parameters of measuring nanoobjects from their nominal values. It is proved that increasing the number of measurement methods used in the metrological analysis of nanoobjects will increase the reliability and accuracy of measurement results, and each method will provide additional information parameters to create a computerized method of calculating the control link. The main condition for correct comparison of the result is knowledge of the specific parameters on which each method is based.</p>
      </abstract>
      <kwd-group>
        <kwd>eol&gt;nanotechnology</kwd>
        <kwd>nanomeasurement</kwd>
        <kwd>metrology</kwd>
        <kwd>methods and means of measurement</kwd>
        <kwd>nanomaterials</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>
        In recent years, the study of submicron, nano-, and cluster materials has developed rapidly in
many fields of science and technology [
        <xref ref-type="bibr" rid="ref1 ref2 ref3">1, 2, 3</xref>
        ]. For several decades, almost all developed
countries in various sectors of the economy have seen rapid progress in the field of nanotechnology.
      </p>
      <p>Improving production eficiency and product quality, development of electronic equipment
and biomedical devices, as well as the creation of new nanostructured materials with special
properties are largely determined by the accuracy and precision of metrological support. It
should be noted that research aimed at improving the instrumentation of nanotechnology has
reached a new progressive level. Of course, large-scale development of the nanoindustry is
impossible without appropriate metrological (MS) and software support.</p>
      <p>
        Most of the theoretical and applied studies of new measurement methods with a minimum
error have no practical application. The existing methods [
        <xref ref-type="bibr" rid="ref4 ref5">4, 5</xref>
        ] are unproductive, have low
accuracy, noise immunity, reliability and cannot be used as part of flexible computerized
measuring systems. These methods do not provide the required measurement accuracy for
nanoobjects with complex, pronounced topography and do not meet modern requirements for the
accuracy and speed of measurements.
      </p>
      <p>In this regard, the problem of improving existing and developing new automated methods for
measuring and evaluating the physical and mechanical properties of nanoobjects is relevant.</p>
      <p>Therefore, the aim of the work is a thorough analysis of existing methods and measuring
instruments in the nanometer range, their classification, and determination of the main
characteristics. The analysis is carried out to create a new unified computer program for automatic
correction of nano-measurements errors online.</p>
    </sec>
    <sec id="sec-2">
      <title>2. Results</title>
      <p>
        The essence of nano-measurements is to work at the molecular level, to study structures with
fundamentally new properties. One of the main problems when working with nano-objects
and nanostructures is associated with ultra-low signal levels. Another problem [
        <xref ref-type="bibr" rid="ref6">6</xref>
        ] is the wide
range of behavior that objects and components can exhibit when measured, associated with
the influence of destabilizing factors.
      </p>
      <p>
        The essence of nano-measurements is to work at the molecular level, to study structures with
fundamentally new properties. One of the main problems when working with nanoobjects and
nanostructures is related to ultra-low signal levels. Another problem [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ] is the wide range of
behaviors that measuring objects and components can exhibit.
      </p>
      <p>
        For example [
        <xref ref-type="bibr" rid="ref8">8</xref>
        ], measuring objects made of polymeric materials may have a resistance of
more than one GM. However, being drawn into fibers with a diameter of less than 100 nm and
doped with various nanoparticles, the polymer can be transformed from an excellent insulator
into a high-conductivity wire. The result is an extremely wide range of test signals.
Highsensitivity, high-resolution instruments are required to detect weak electrical signals at the
bottom of the range.
      </p>
      <p>
        Also, a prominent aspect is that DC measurements may require the characterization of some
devices and structures by radio frequency signals. This requires a strict design of measuring
instruments with reliable RF connections with low losses of the measuring head and a special
electronic circuit for each signal path [
        <xref ref-type="bibr" rid="ref9">9</xref>
        ]. Otherwise, it will not be possible to achieve the
resolution required for precision re-measurements. Therefore, measurement methods and tools
should minimize noise and other sources of error that may interfere with the signal. No less
important is the fact that metrological means of nano measurement should be easy to use and
economical.
      </p>
      <p>Nowadays, raster electron microscopy (SEM), transmission electron microscopy (TEM), atomic
force microscopy (AFM), scanning tunneling microscopy (STM), microscopy, and focusing on
microscopy have become the most widespread. mass spectrometry, Auger spectroscopy, etc.
From the point of view of research of the relief and physical properties of structures with high
lateral resolution (less than 10 nm), one of the most perspectives is scanning probe microscopy
(SPM).</p>
      <p>
        The size and structure of the nanoobject have a great influence on the type of technique and
the characteristics of the measurement methods used [
        <xref ref-type="bibr" rid="ref10">10</xref>
        ]. It is proved that optical microscopes
are the most suitable for the study of macroscopic materials, for nanoscopic materials with a
particle size less than 200 nanometers it is better to use STM, AFM, or combined methods of
scanning probe microscopy.
      </p>
      <p>SPM, STM, AFM methods are especially useful for the structures of crystalline nanoparticles.
Figure 1 shows the atomic structures for some typical crystals of well-known shapes, such as
a simple cube, a volume-centered cube, and a border-centered cube. Knowing the location of
atoms in these structures helps to predict the properties of particles.</p>
      <p>
        However [
        <xref ref-type="bibr" rid="ref11 ref12">11, 12</xref>
        ], on a nanoscopic scale, it is the particle size that radically changes the
physics of its behavior and dictates the need to use other measurement methods.
      </p>
      <p>Importantly, the chemical and electrical sets of properties of the nanomaterial can change as
the particle size decreases to nanometer size. Therefore, in practice, additional chemical and
electrical tests are required to determine the characteristics of most of these materials, which
also afects the choice of the measurement method. Depending on the means of measurement,
methods of analysis of nanomaterials can be divided into two main groups: discrete and
ensemble methods of measurement.</p>
      <p>
        Discrete methods of measuring nanoobjects typically use powerful microscopes, such as
scanning electron microscopy (SEM), transmission electron microscopy (TEM), electron
microscopy (SEM), atomic force microscopy (AFM), and scanning probe microscopy (SPM). EM
and SPM are fairly simple methods and reflect particle shapes, but are insuficient in terms of
statistics [
        <xref ref-type="bibr" rid="ref13 ref14">13, 14</xref>
        ].
      </p>
      <p>These methods have a resolution much higher than optical microscopy and can detect and
measure discrete particles by scattering a high-energy electron beam (SEM and TEM), or by
detecting through a probe attached to a slightly sprung console (AFM). In figure 2 shows a
comparison of discrete methods of nano measurement concerning the indicators of the speed
of obtaining results and price.</p>
      <p>Ensemble methods are usually indirect methods when information from many nanoparticles
is obtained simultaneously. The methods of this group make it possible to establish the average
size of nanoparticles as low-angle X-ray scattering (SAXS) and to detect photon interference.</p>
      <p>One of the most frequently used and user-friendly methods for determining the size of
nanoobjects in this group is the method of dynamic light scattering (DRS), which is based
on the principles of coherence of light waves, and metrological characteristics are obtained by
determining the phase diference of these waves after interaction with nanoparticles.</p>
      <p>One method that potentially combines the advantages of a group of discrete methods and
an ensemble approach is the nanoparticle tracking method, which involves determining the
position of particles suspended in a liquid by detecting the light they scatter when irradiated
by a laser source and viewing the suspension by using a camera with a charged connected
device.</p>
      <p>In figure 3 presents the ratio of the main methods of research of nanomaterials with diferent
relief characteristics of nanoobjects.</p>
      <p>
        Based on the analysis, it was determined that the most functional and universal in solving
a wide range of problems is the method of scanning probe microscopy. SPM, in turn, covers
several diferent experimental methods for studying the structure and properties of the surface,
both at the micro-level and the level of individual molecules and atoms [
        <xref ref-type="bibr" rid="ref4">4, 15</xref>
        ].
      </p>
      <p>The indisputable advantage of this method is the fact that with the help of SPM you can get
information directly from a relatively large area of the surface, which allows you to use this
method on-line. Therefore, it is not surprising that they are now widely used for the research,
diagnosis, and modification of surfaces.</p>
      <p>Common to all methods is the presence of a pointed probe as a tool for working with the
surface of the samples. There are contact, semi-contact, and non-contact modes of operation, as
well as various modes of operation, including tunnel mode, atomic force mode, spectroscopy
mode, Kelvin probe method, electric power, magnetic force, near field, optical, confocal
microscopy, etc.</p>
      <p>With these methods, you can measure not only the topology of the structure but also many
special properties, such as modulus of elasticity, distribution of various substances on the
surface, the degree of surface roughness, static charge distribution, the orientation of magnetic
domains, etc. [16].</p>
      <p>Based on the nature of the applications of existing methods in SPM, they can be classified as
follows (figure 4).</p>
      <p>Despite the variety of types and applications of modern scanning microscopes, their work
is based on similar principles, and their designs difer little from each other.</p>
      <p>Another common feature that unites not only sounding instruments, but also other
measuring equipment presented in the article for measuring in the nanomaterial range is their
increased sensitivity to external destabilizing factors, such as the composition and properties
of the environment, lighting, potential diference, and magnetic field, temperature, etc.
Because the properties of certain nanomaterials are diferent from conventional ones, the efect
of destabilizing factors on the measurement results can be completely unpredictable.</p>
      <p>Therefore, when choosing an existing or developing a new measurement method, the
features of the kinetics and mechanism of the interaction of the measuring nanoobject with the
environment should be thoroughly studied, the properties of nanostructures, process
parameters, and the model of their mathematical description should be determined.</p>
      <p>A necessary condition for the choice of measurement conditions, such assessments, and
subsequent interpretation of the data is the reproducibility of the results and the invariance of
the sample for a set of properties.</p>
      <p>When changing the size can change not only the values of certain values but also the nature
of their dependencies on properties, environments, and influences.</p>
      <p>The main directions of creation and use of methods of measurement of micro- and
nanosystems are defined:
• creation of model representations of connections of topological characteristics and
reaction of the object to external influences
• establishing links between the properties of the element or system and the topology of
the composition, structure, charges, and fields
• establishing links between technological factors, the kinetics of formation, and the
properties of nanostructures
• creation of models that link the functional parameters of devices with the properties of
structures that are determined during their manufacture
Therefore, to obtain more reliable results, the method of nano measurements should take into
account the efects of external destabilizing factors on the nanoobject and ensure the possibility
of correcting the deviations caused by them.</p>
    </sec>
    <sec id="sec-3">
      <title>3. Discussion</title>
      <p>Based on the analysis, a method for measuring nanoobjects in static and dynamic modes is
proposed. This method will take into account the influence of destabilizing factors for
nanostructures of diferent types. The method consists of the continuous determination of the
coordinates of the points on the surface of the nanoobject, their processing, and presented in the
form of a three-dimensional image. A cluster is introduced to determine the compensating link
that corresponds to the tolerance field according to the spectrum of the color image.</p>
      <p>The color value of the discrete points of the digital image forms the area, which is represented
as isolines. Mathematical software includes geometric parameters of the reference
nanostructure. As a result, a region of the color image is formed, which corresponds to the deviations
from the shape and location of the surfaces and difers from each other in color (figure 5).</p>
      <p>In addition to measuring flat nanostructures, a big task is to determine the topographic
features of the surface and the angle of rotation of the plane of the nanoobject. This dependence
is formed in the form of a three-dimensional array, in which one column occupies the angle of
inclination of the plane, the second – the topographic features of the surface, the third – the
coordinate. When scanning the surface of the part, a function based on a mathematical model
of the process of traversing the measuring object is used.</p>
      <p>The obtained values of the angle of inclination of the plane and topographic features, as well
as the values of the coordinates, are compared with the tolerance field, which is presented in
the color image (figure 6).</p>
      <p>The diferential-digital method makes it possible to study errors, determine the parameters
of the nanoobject and obtain cross-sections using the developed methods of algorithmic error
compensation, which provides zero ofsets for the operating conditions of the measurement
after the training procedure to obtain a statistical result. The development of the
diferentialdigital method involves the use of an additional information parameter in the mathematical
model in the form of a compensating link. The introduction of additional (a priori) information
leads the problem to the correct according to the method of regularization for the functional
Ω(,  ) = |</p>
      <p>−  |2 +  | −  0|,
where →− ∞,  0 – is the a priori solution vector that coincides with the regularization
coeficient.</p>
      <p>Using this approach to the problem of determining the geometric parameters of the
aviation part of a complex spatial surface in small segments, using Delaunay triangulation, using
the operation of minimizing the sum of the squares of the deviation, we obtain the following
expression:</p>
      <p>( =1)</p>
      <p>2
Φ( ) = ∑   + 
(,  ),
part; 
constructed surface; 
(,</p>
      <p>)
the geometric parameter and the regularization coeficient  :</p>
      <p>=  0,  1, . . . ,   , . . . ,  
where ∑( =1)  2 – the sum of the squares of the deviation of n measured points, then from the</p>
      <p>– the required geometric parameters of the aviation
- regulatory member, which includes information about the nominal value of
 (,  ) = 
∑ (  −    ) .</p>
      <p>2</p>
      <p>Thus, we obtain the problem of the regularizing link, which characterizes the deviation of the
parameters of nanoobjects from their nominal values, we can obtain a clear point of minimum
in the minimization function. The obtained results were stable and satisfied the value of the
tolerance field of the measuring part.</p>
      <p>( =1)</p>
    </sec>
    <sec id="sec-4">
      <title>4. Conclusions</title>
      <p>There are many advantages and disadvantages in choosing a specific measurement method to
measure the topography of non-objects. There is no best general method. The use of
integration of information provided by diferent methods is proposed, but the results of diferent
methods may be contradictory in some cases, namely:
1. Each method is based on the need to study the diferent properties of nanoobjects
2. The steps of sample preparation can modify the results by further unintentional
movements of the particles in the matrix, changing the average diameter detected by the SPM
3. Uncertainty that is not taken into account may also afect the final measurements
4. The use of diferent weighing in determining the average diameter of the size
distribution. Comparing the results of diferent measurements of the same methodology will be
less problematic in this sense because the existing error is constant</p>
      <p>Comparing the results of diferent measurements of the same methodology will be less
problematic in this sense because the existing error is constant. Therefore, to test the method, the
error must be accurately measured, and the results must be consistent with other methods.
Therefore, increasing the number of measurement methods used in the metrological
analysis of nanoobjects will increase the reliability and accuracy of measurement results and each
method will provide additional information. The main condition for correct comparison of the
result is knowledge of the specific parameters on which each method is based. The analysis
was conducted to obtain the most complete information for the development of a computer
program based on a discrete-digital measurement method, which would take into account the
measurement information obtained by diferent measurement methods, taking into account
the impact of destabilizing factors.
in Theory, Practice and Applications (Cat. No. 98CH36190), volume 3, IEEE, 1998, pp.
1739–1746.
[15] M. Sitti, H. Hashimoto, Two-dimensional fine particle positioning under an optical
microscope using a piezoresistive cantilever as a manipulator, journal of Micromechatronics
1 (2000) 25–48.
[16] Digital Instruments, 2021. URL: https://www.digital-instruments.com/.</p>
    </sec>
  </body>
  <back>
    <ref-list>
      <ref id="ref1">
        <mixed-citation>
          [1]
          <string-name>
            <given-names>R.</given-names>
            <surname>Balabai</surname>
          </string-name>
          ,
          <article-title>Electronic properties of functionalized graphene nanoribbons</article-title>
          ,
          <source>Ukrainian Journal of Physics</source>
          <volume>58</volume>
          (
          <year>2013</year>
          )
          <fpage>389</fpage>
          -
          <lpage>397</lpage>
          . doi:
          <volume>10</volume>
          .15407/ujpe58.
          <fpage>04</fpage>
          .0389.
        </mixed-citation>
      </ref>
      <ref id="ref2">
        <mixed-citation>
          [2]
          <string-name>
            <given-names>E.</given-names>
            <surname>Glushko</surname>
          </string-name>
          ,
          <string-name>
            <given-names>A.</given-names>
            <surname>Stepanyuk</surname>
          </string-name>
          ,
          <article-title>Electromagnetic modes inside the island kind 2d photonic crystal resonator</article-title>
          ,
          <source>Springer Proceedings in Physics 195</source>
          (
          <year>2017</year>
          )
          <fpage>263</fpage>
          -
          <lpage>274</lpage>
          . doi:
          <volume>10</volume>
          .1007/ 978-3-
          <fpage>319</fpage>
          -56422-7_
          <fpage>18</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref3">
        <mixed-citation>
          [3]
          <string-name>
            <given-names>V.</given-names>
            <surname>Zenou</surname>
          </string-name>
          ,
          <string-name>
            <given-names>A.</given-names>
            <surname>Kiv</surname>
          </string-name>
          ,
          <string-name>
            <given-names>D.</given-names>
            <surname>Fuks</surname>
          </string-name>
          ,
          <string-name>
            <given-names>V.</given-names>
            <surname>Ezerski</surname>
          </string-name>
          ,
          <string-name>
            <given-names>N.</given-names>
            <surname>Moiseenko</surname>
          </string-name>
          ,
          <article-title>The microscopic mechanism of silicon precipitation in al/si system</article-title>
          ,
          <source>Materials Science and Engineering A</source>
          <volume>435</volume>
          -
          <fpage>436</fpage>
          (
          <year>2006</year>
          )
          <fpage>556</fpage>
          -
          <lpage>563</lpage>
          . doi:
          <volume>10</volume>
          .1016/j.msea.
          <year>2006</year>
          .
          <volume>07</volume>
          .095.
        </mixed-citation>
      </ref>
      <ref id="ref4">
        <mixed-citation>
          [4]
          <string-name>
            <given-names>P.</given-names>
            <surname>Todua</surname>
          </string-name>
          ,
          <article-title>Metrology and standardization in nanotechnologies and the nanoindustry</article-title>
          ,
          <source>Measurement Techniques</source>
          <volume>51</volume>
          (
          <year>2008</year>
          )
          <fpage>462</fpage>
          -
          <lpage>469</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref5">
        <mixed-citation>
          [5]
          <string-name>
            <given-names>J.</given-names>
            <surname>Garnaes</surname>
          </string-name>
          ,
          <string-name>
            <given-names>L.</given-names>
            <surname>Nielsen</surname>
          </string-name>
          ,
          <string-name>
            <given-names>K.</given-names>
            <surname>Dirscherl</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J.</given-names>
            <surname>Jørgensen</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J.</given-names>
            <surname>Rasmussen</surname>
          </string-name>
          ,
          <string-name>
            <given-names>P.</given-names>
            <surname>Lindelof</surname>
          </string-name>
          ,
          <string-name>
            <given-names>C.</given-names>
            <surname>Sørensen</surname>
          </string-name>
          ,
          <article-title>Two-dimensional nanometer-scale calibration based on one-dimensional gratings</article-title>
          ,
          <source>Applied Physics A</source>
          <volume>66</volume>
          (
          <year>1998</year>
          )
          <fpage>S831</fpage>
          -
          <lpage>S835</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref6">
        <mixed-citation>
          [6]
          <string-name>
            <given-names>W.</given-names>
            <surname>Fritzsche</surname>
          </string-name>
          ,
          <string-name>
            <given-names>L.</given-names>
            <surname>Takac</surname>
          </string-name>
          , E. Henderson,
          <article-title>Application of atomic force microscopy to visualization of dna, chromatin</article-title>
          , and chromosomes,
          <source>Critical Reviews™ in Eukaryotic Gene Expression</source>
          <volume>7</volume>
          (
          <year>1997</year>
          ).
        </mixed-citation>
      </ref>
      <ref id="ref7">
        <mixed-citation>
          [7]
          <string-name>
            <given-names>S.</given-names>
            <surname>Roth</surname>
          </string-name>
          ,
          <string-name>
            <given-names>L.</given-names>
            <surname>Dellmann</surname>
          </string-name>
          , G. Racine, N. De Rooij,
          <article-title>High aspect ratio uv photolithography for electroplated structures</article-title>
          ,
          <source>Journal of Micromechanics and Microengineering</source>
          <volume>9</volume>
          (
          <year>1999</year>
          )
          <fpage>105</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref8">
        <mixed-citation>
          [8]
          <string-name>
            <surname>AZOnano</surname>
          </string-name>
          ,
          <year>2021</year>
          . URL: https://www.azonano.com/.
        </mixed-citation>
      </ref>
      <ref id="ref9">
        <mixed-citation>
          [9]
          <string-name>
            <given-names>R.</given-names>
            <surname>Said</surname>
          </string-name>
          ,
          <article-title>Microfabrication by localized electrochemical deposition: experimental investigation and theoretical modelling</article-title>
          ,
          <source>Nanotechnology</source>
          <volume>14</volume>
          (
          <year>2003</year>
          )
          <fpage>523</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref10">
        <mixed-citation>
          [10]
          <string-name>
            <given-names>H.</given-names>
            <surname>Iwasaki</surname>
          </string-name>
          ,
          <string-name>
            <given-names>T.</given-names>
            <surname>Yoshinobu</surname>
          </string-name>
          ,
          <string-name>
            <given-names>K.</given-names>
            <surname>Sudoh</surname>
          </string-name>
          ,
          <article-title>Nanolithography on sio2/si with a scanning tunnelling microscope</article-title>
          ,
          <source>Nanotechnology</source>
          <volume>14</volume>
          (
          <year>2003</year>
          )
          <article-title>R55</article-title>
          .
        </mixed-citation>
      </ref>
      <ref id="ref11">
        <mixed-citation>
          [11]
          <string-name>
            <given-names>A.</given-names>
            <surname>Majumdar</surname>
          </string-name>
          ,
          <string-name>
            <given-names>P.</given-names>
            <surname>Oden</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J.</given-names>
            <surname>Carrejo</surname>
          </string-name>
          ,
          <string-name>
            <given-names>L.</given-names>
            <surname>Nagahara</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J.</given-names>
            <surname>Graham</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J.</given-names>
            <surname>Alexander</surname>
          </string-name>
          ,
          <article-title>Nanometer-scale lithography using the atomic force microscope</article-title>
          ,
          <source>Applied Physics Letters</source>
          <volume>61</volume>
          (
          <year>1992</year>
          )
          <fpage>2293</fpage>
          -
          <lpage>2295</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref12">
        <mixed-citation>
          [12]
          <string-name>
            <given-names>C.</given-names>
            <surname>Hyon</surname>
          </string-name>
          ,
          <string-name>
            <given-names>S.</given-names>
            <surname>Choi</surname>
          </string-name>
          ,
          <string-name>
            <given-names>S.-H.</given-names>
            <surname>Song</surname>
          </string-name>
          ,
          <string-name>
            <given-names>S.</given-names>
            <surname>Hwang</surname>
          </string-name>
          ,
          <string-name>
            <given-names>M.</given-names>
            <surname>Son</surname>
          </string-name>
          ,
          <string-name>
            <given-names>D.</given-names>
            <surname>Ahn</surname>
          </string-name>
          ,
          <string-name>
            <given-names>Y.</given-names>
            <surname>Park</surname>
          </string-name>
          , E. Kim,
          <article-title>Application of atomic-force-microscope direct patterning to selective positioning of inas quantum dots on gaas</article-title>
          ,
          <source>Applied Physics Letters</source>
          <volume>77</volume>
          (
          <year>2000</year>
          )
          <fpage>2607</fpage>
          -
          <lpage>2609</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref13">
        <mixed-citation>
          [13]
          <string-name>
            <given-names>M.</given-names>
            <surname>Falvo</surname>
          </string-name>
          ,
          <article-title>The nanomanipulator: A teleoperator for manipulating materials at the nanometer scale</article-title>
          ,
          <source>in: Proc. Int. Symp. on the Science and Technology of Atomically Engineered Materials</source>
          ,
          <year>1995</year>
          , pp.
          <fpage>579</fpage>
          -
          <lpage>586</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref14">
        <mixed-citation>
          [14]
          <string-name>
            <given-names>M.</given-names>
            <surname>Sitti</surname>
          </string-name>
          ,
          <string-name>
            <given-names>H.</given-names>
            <surname>Hashimoto</surname>
          </string-name>
          ,
          <article-title>Tele-nanorobotics using atomic force microscope</article-title>
          ,
          <source>in: Proceedings. 1998 IEEE/RSJ International Conference on Intelligent Robots and Systems</source>
          . Innovations
        </mixed-citation>
      </ref>
    </ref-list>
  </back>
</article>