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  <front>
    <journal-meta>
      <journal-title-group>
        <journal-title>hierarchical compression,” Computer Optics</journal-title>
      </journal-title-group>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.18287/2412-6179-2016-40-4-543-551</article-id>
      <title-group>
        <article-title>On the need to use the median signal filtering method to improve the metrological characteristics of the rubidium frequency standard during processing and transmitting large data arrays</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Anton Valov</string-name>
          <email>tony.valov2015@yandex.ru</email>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Vadim Davydov</string-name>
          <email>davydov_vadim66@mail</email>
          <email>davydov_vadim66@mail. ru</email>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Vasiliy Rud</string-name>
          <email>rudvas.spb@gmail.com</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Nikita Lukashev</string-name>
          <email>n-lukash@list.ru</email>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>All-Russian Research Institute of Phytopathology</institution>
          ,
          <addr-line>Moscow Region</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Bonch-Bruevich Saint Petersburg State University of</institution>
          ,
          <addr-line>Telecommunications, Saint-Petersburg</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>Peter the Great Saint Petersburg Polytechnic University</institution>
          ,
          <addr-line>Saint-Petersburg</addr-line>
          ,
          <country country="RU">Russia</country>
          ,
          <institution>All-Russian Research Institute of Phytopatholog</institution>
          ,
          <addr-line>Moscow</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
      </contrib-group>
      <pub-date>
        <year>2016</year>
      </pub-date>
      <volume>40</volume>
      <issue>4</issue>
      <fpage>102</fpage>
      <lpage>105</lpage>
      <abstract>
        <p>-The article describes the construction of the rubidium - 87 quantum frequency standard for satellite infocommunication and navigation systems for various purposes. The necessity of improving the metrological characteristics of the quantum frequency standard for longterm transmission of large amounts of data is substantiated. A new algorithm is proposed for processing data of a large amount of data about the error signal using the median filtering method to improve the short-term and long-term stability of the frequency standard. The results of experimental studies of the metrological characteristics of the quantum frequency standard are presented. The improvement in longterm frequency stability was found to be 7%, which reduces the number of bit errors during long-term transmission of information by at least 3%.</p>
      </abstract>
      <kwd-group>
        <kwd>quantum frequency standard</kwd>
        <kwd>signals processing</kwd>
        <kwd>information transfer</kwd>
        <kwd>data arrays</kwd>
        <kwd>Allan's deviations</kwd>
        <kwd>median filtering method</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>I. INTRODUCTION</title>
      <p>
        In the modern world, accurate measurement of time and
frequency is necessary to solve various problems in the
fields of science and technology [
        <xref ref-type="bibr" rid="ref1 ref2 ref3 ref4 ref5 ref6 ref7">1-7</xref>
        ]. One of the most
complex of them is ensuring the uninterrupted operation of
satellite communication systems, navigation, Earth surface
research and spacecraft control from orbit [
        <xref ref-type="bibr" rid="ref1 ref10 ref11 ref12 ref13 ref14 ref15 ref16 ref17 ref3 ref8 ref9">1, 3, 8-17</xref>
        ]. A
special place among the devices for determining the
frequency and time is occupied by quantum frequency
standards (QFS) [
        <xref ref-type="bibr" rid="ref8 ref9">8, 9, 18-22</xref>
        ]. Currently, global satellite
constellations for various purposes use only QFS [9.18-20,
23-25]. The main advantage of QFS over other devices is
the use for stable operation of stabilization systems for the
frequency of laser radiation and optical elements [
        <xref ref-type="bibr" rid="ref20 ref21 ref22 ref23 ref24 ref3 ref8">3, 8, 19,
20, 25-29</xref>
        ]. Other devices cannot provide the necessary
accuracy in determining the frequency and long-term
stability of its nominal value in conditions of large
overloads. A slight deviation of the frequency from the
nominal value leads to large errors, especially when
transmitting large data streams.
      </p>
      <p>
        One of the main problems of a satellite system is the
mutual synchronization of satellite timelines to nanoseconds
or less [
        <xref ref-type="bibr" rid="ref25 ref26 ref27 ref9">9, 18-20, 30-32</xref>
        ]. For example, the error of the
navigation signals emitted by different satellites during a
temporary mismatch of 10 ns causes an additional error in
determining the location of an object of 10-15 meters.
      </p>
      <p>The expanding of the tasks number for which the
satellite navigation systems are used, the accuracy is
required of increase of determining the object position to 0.5
m. On the other hand, a development of scientific and
technological progress is changing the composition of the
used electronic equipment. All this requires constant
modernization of satellite navigation systems, including
quantum frequency standards.</p>
      <p>
        The development and commissioning of new QFS
models is a very lengthy and expensive process. In most
cases, there is no time and sufficient funds for its
implementation. Therefore, in most cases, for the specific
problems it is better to perform the modernization of the
rubidium – 87 QFS and caesium - 133 QFS, which are in
operation on satellite systems [
        <xref ref-type="bibr" rid="ref18 ref19 ref20 ref27 ref28 ref29 ref30">18-20, 23-25, 32-35</xref>
        ].
      </p>
      <p>The process of modernizing frequency standards
includes various directions: changing weight and
dimensions, reducing energy consumption, improving
metrological characteristics. The quantum frequency
standards are characterized by the fact that modernization
may not be for its entire structure, but only for individual
nodes or blocks. In our work, we are considering one of
such directions for improving the metrological characteristic
of the rubidium-87 quantum frequency standard.</p>
      <p>II. THE CONTROL ALGORITHM FOR FREQUENCY ADJUSTING OF</p>
      <p>THE QUANTUM STANDARD</p>
      <p>
        During the period of operation of rubidium – 87 QFS,
the structural schemes of its various QFS models did not
undergo fundamental changes in comparison with their
classical representation [
        <xref ref-type="bibr" rid="ref25 ref26 ref8 ref9">8, 9, 18-20, 30, 31</xref>
        ]. In the design of
the QFS, individual elements or blocks, as well as control
systems for various parameters, are mainly changed to
improve the metrological characteristics of the standard. On
fig. 1 is shown the structural diagram of the rubidium – 87
QFS.
      </p>
      <p>In this design the method developed by us for improving
the microwave signal parameters to improve the
metrological characteristics of the standard is implemented.</p>
      <p>
        The operation of the rubidium – 87 QFS is based on the
principle of tuning a highly stable voltage-controlled quartz
oscillator 10 to the quantum-frequency transition of
rubidium–87 atoms [
        <xref ref-type="bibr" rid="ref18 ref19 ref30 ref8">8, 18, 23, 24, 35</xref>
        ]. To implement the
noted frequency adjustment of the quartz oscillator, a
microwave signal from a frequency synthesizer (FS) 11 is
supplied to a vacuum cell 6 filled with rubidium-87 atoms
and a buffer gas 11. When the frequency of the microwave
signal coincides with the quantum transition frequency of
the excited rubidium – 87 atoms, the signal detected by the
photodetector has maximum signal to noise ratio (S/N). If
the frequency of the microwave signal fmw leaves the value
of the frequency of the resonant transition, the S/N ratio
decreases and an error signal is generated by the electronic
circuit 9. This signal is used to adjust the frequency of the
crystal oscillator 10. Therefore, one of the key points in the
operation of the QFS on rubidium atoms is 87, is the
formation of a microwave signal taking into account its
various features. The process of generating a microwave
signal is carried out in the midrange 11. It is necessary that
the output of the midrange provide high accuracy of the
output frequency, high suppression of the side amplitude
components in the spectrum of the output signal, low
dependence of the frequency and amplitude of the output
signal on temperature.
      </p>
      <p>
        The method of generating a microwave signal in a
frequency synthesizer discussed in detail in [
        <xref ref-type="bibr" rid="ref1 ref2">1, 2, 20</xref>
        ] has
one significant drawback. The spectrum of the output signal
with a frequency of 5.3125 MHz, which is obtained at the
output of one of the FS balanced mixers (BM) 11 [20],
contains lateral amplitude components. If one of the side
components coincides with the frequency of any Zeeman
transition, then this will lead to transitions of atoms at these
levels and an error in establishing the actual value of the
frequency of the output signal of the QFS. To suppress the
side components, a quartz filter is used, which has a high
temperature dependence. For reliable operation of the quartz
filter, high temperature stabilization is required. This is
extremely difficult to achieve, especially in conditions of a
long flight of the satellite.
      </p>
      <p>
        It should also be noted that the frequency of the
microwave signal necessary for the operation of the QFS,
which corresponds to the frequency difference between the
two ultra-thin sublevels F = 2 and F = 1 [
        <xref ref-type="bibr" rid="ref8">8</xref>
        ], is formed at the
output of the balanced midrange mixer 11. The BM
operation can be described by the equation:
  = 21   ( 1 −  2) + 21  ( 1 +  2) , (1)
where  ( 1 −  2) is the difference and  ( 1 +  2)
is the total frequency.
      </p>
      <p>All side components, if they appear in the spectrum of
signals with frequencies ω1 and ω2 (for example, due to
temperature drift in a quartz filter), are converted to signals
with combination frequencies. These signals will create
additional errors. Therefore, during each communication
session of the satellite with the ground station, when
comparing the time scales in the QFS on the rubidium
atoms, 87 adjust the frequency. If for some reason the
communication session did not take place, then the satellite
can be suspended in the navigation system.</p>
      <p>
        Therefore, it is extremely important to develop a method
that, on the one hand, provides high accuracy of the output
frequency with its tuning in autonomous mode, regardless of
communication with the ground station. In the methods for
QFS considered in [
        <xref ref-type="bibr" rid="ref25 ref26 ref8">8, 18, 30, 31</xref>
        ], the frequency tuning step
is more than 1 Hz using a voltage setting of the
voltagecontrolled crystal oscillator 10.
      </p>
      <p>The frequency tuning of the crystal oscillator is
controlled by the AFC system 9, which includes a crystal
oscillator control unit (XOCU) and a control unit that
converts the signal from the quantum discriminator and
calculates the tuning code for further sending it to the
XOCU.</p>
      <p>In the previous version of the software for the QFS
control device, simple accumulation of all received data at
different frequencies was used with further calculation of
the value of the error signal of the microwave signal. In the
new version, it is proposed to use the median filtering
method as one of the data filtering methods.</p>
      <p>The median filtering method uses the ordering of several
elements received at the input of the control unit and the
subsequent selection of a value equally spaced from the
beginning and end of the ordered series of elements.
III. THE RESULTS OF EXPEREMENTAL INVESTIGATIONS AND</p>
      <p>DICUSSION</p>
      <p>
        During of the using of the optical light signals for
recording of resonance conditions on a photodetector, the
important characteristic is the spectral density Sφ [
        <xref ref-type="bibr" rid="ref8">8</xref>
        ]. The
value of Sφ has a significant effect on the S/N ratio. In fig. 2
shows the spectral densities of phase noises for two designs
of the QFS (the previously used design and a new). In new
design was used the method of improving the parameters of
the microwave signal.
      </p>
      <p>An analysis of the obtained results shows a significant
decrease in phase noise amplitude when using the median
filtering method.</p>
      <p>The spectral density of noise in the frequency range of
the tuning of the resonant frequency of the quantum
transition is presented on fig. 3.</p>
      <p>An analysis of the obtained results of experimental
investigations in fig. 3 showed that the use of the method
developed by us, as well as the use of a microcontroller for
control in the QFS, reduces the power of phase noise in the
output spectrum of the signal.</p>
      <p>All this made it possible to improve the short-term
frequency stability - Allan's deviation, as well as long-term
frequency stability. The results of the investigations of
Allan's deviation are presented on fig. 4.</p>
      <p>The analysis of the obtained results (fig. 4) shows that
the implemented technical solutions and the developed new
method for improving the parameters of the microwave
excitation signal during modernization of the standard
design made it possible to improve Allan deviation by 7 %.</p>
    </sec>
    <sec id="sec-2">
      <title>IV. CONCLUSION</title>
      <p>The obtained results have shown that the use of a new
method of filtering data in the automatic frequency
adjustment system of the microwave excitation signal
reduces one of the most important disturbing factors
(spectral noise density) that affects short-term frequency
stability.</p>
      <p>The experimental investigations of the metrological
characteristics of the rubidium – 87 QFS are showed the
improvement of the long-term frequency stability on 7 %.
The resulting improvements in short-term and long-term
frequency stability can improve the reliability of satellite
transmission systems of large amounts of information.
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frequency standard on a rubidium gas cell with pulsed optical
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scheme,” Measurement Techniques, vol. 59, no. 12 , pp. 1218-1224,
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