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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Robust diagnostics of dark counts for quantum networks</article-title>
      </title-group>
      <contrib-group>
        <aff id="aff0">
          <label>0</label>
          <institution>Kazan National Research Technical University n.a. A.N. Tupolev</institution>
          ,
          <addr-line>Kazan</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>N.S. Perminov</institution>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>Zavoisky Physical-Technical Institute, FRC Kazan Scientific Center of RAS</institution>
          ,
          <addr-line>Kazan</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
        <aff id="aff3">
          <label>3</label>
          <institution>KAZAN QUANTUM COMMUNICATION» LLC</institution>
          ,
          <addr-line>Kazan</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>In this work, we study timestamps when registering counts of single-photon detectors in quantum communications. Post-pulse counts are analyzed based on several approaches. Explicit statistical accounting of the noise of quantum detectors allows you to most correctly select the mode of use of the detectors to realize the most efficient quantum communication with the highest signal to noise ratio. Direct statistical analysis and robust diagnostics of the noise of quantum detectors can be done by ranging the time's tags of quantum keys that are available for the online diagnostic system and analysis a significant amount of information about the quantum communication performance (the amount of dark noise and post-pulse counts, line interference, etc.). The conclusion is made about the proportion of dark noise and post-pulse counts in the total noise, and the limits of applicability of the theory are shown using a sequence of the ranged amplitudes. We offer non-parametric robust diagnostic of times tags in keys to increase the security of quantum networks, and also discuss the prospects of commercializing quantum-classical cloud-based security services.</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>
        Robust diagnostics of the working complexes of
quantum communication (QC) [
        <xref ref-type="bibr" rid="ref1">1</xref>
        ] is crucial for the
implementation of quantum networks capable of working
in both urban and trunk standard fiber-optic
communication lines. At the same time, from the point of
view of communication systems, trunk quantum networks
(TQN) with lines of more than 100 km and losses between
nodes of more than 25 dB, where the signal-to-noise ratio
cannot be considered large, are particularly difficult to
implement [
        <xref ref-type="bibr" rid="ref2">2</xref>
        ]. From the point of view of fundamental
statistics, the fundamental difficulty here lies in the fact
that despite the relatively low average percentage of errors,
the magnitude of the error span and the variance of errors
can be extremely large, which entails low reliability of
diagnosing errors when performing continuous tests of the
TQN and especially large-scale TQN with a large number
of nodes.
      </p>
      <p>The necessary solution for a similar problem in
communication theory is the use of prognostic monitoring
tools and error filtering, which will increase the reliability
of security parameters for inter-city QC in continuous use.
We also note that due to large errors for the limit passport
operating modes of QC complexes, the security of the
communication complex should be determined by a
special diagnostic system that is different from the
diagnostic system for operating passport modes. This
difference in diagnosis is also due to the fact that the
reliability of error determination in the limiting mode
effectively depends on a significantly larger number of
physical factors, which are not always easy to track within
the framework of a single structurally finished product.
That is, a more powerful specialized diagnostic system
should be delivered with the QC complex as a separate
product and be able to work in the background of the TQN
to track the entire history of changes in the line
performance even with the QC complex in the node
disabled. In addition, such a system should be able to track
additional performance factors associated with the
statistics of quantum and classical noise.</p>
      <p>In large-scale TQN, according to the theory of
reliability, control requirements should be higher than for
conventional QC due to the large number of elements and
a high level of noise that cannot be eliminated for
longrange QC. A significant part of the noise in the TQN is due
to various factors arising from the registration of single
photons by highly sensitive single-photon detectors.
Therefore, explicit statistical accounting of the noise of
quantum detectors allows you to most correctly select the
mode of use of the detectors to realize the most efficient
quantum coupling with the highest signal to noise ratio.
Direct statistical analysis and robust diagnostics of the
noise of quantum detectors can be performed by
distributing the time stamps of quantum keys, which are
available for the online diagnostic system and, in our
opinion, carry a significant amount of information about
the QC operability and the level of quantum-classical
security of QC complexes as a whole.</p>
      <p>In this work, we study timestamps when registering
counts of single-photon detectors in QC. Post-pulse counts
are analyzed based on several approaches. The conclusion
is made about the proportion of dark noise and post-pulse
counts in the total noise, and the limits of applicability of
the theory are shown using a sequence of the ranged
amplitudes. We offer non-parametric robust diagnostic of
times tags in keys to increase the security of quantum
networks, and also discuss the prospects of
commercializing quantum-classical cloud-based security
services.
2.</p>
    </sec>
    <sec id="sec-2">
      <title>Modern diagnostic methods</title>
      <p>One of the modern statistical diagnostic methods is a
sequence of the ranged amplitudes (SRA), which is a
sequence of numbers obtained from the original sequence
by ordering numbers in descending (or ascending) order of
their values. SRA are often used in histogram construction
algorithms. The SRA sequences themselves are practically
not analyzed, although they are very interesting, since
when constructing them, there is no loss of information
about specific values of the source data, as, for example,
using the histogram method. It also gives the advantage of
using much less data for statistical analysis. Analytical
analysis of SRA is the essence of the so-called SRA
method
 + 1 −  (  ),

where N is the total number of points in the sample. In
some
cases, knowing the
analytical form
for the
distribution function F(x), one can find an analytical
expression for the SRA of the form that can be actively
used in the SRA method to quickly find the statistical
parameters of the initial sample. Next, we consider two
versions of expressions for SRA that describe random
readings of a single-photon detector. The first one
considers samples caused only by random Poisson sources
(the probability of post-pulse counts is zero). The second
one considers counts caused by post-pulse counts.</p>
    </sec>
    <sec id="sec-3">
      <title>3. Dark counts of detectors</title>
      <p>
        Light sources, as well as dark noise, corresponding to
Poisson processes, correspond to the probability density
for the time intervals
between
samples,
which is
approximately described by a decaying exponent [
        <xref ref-type="bibr" rid="ref8 ref9">8,9</xref>
        ]:
 
 
=  (  ) =   −   ,
  =

1
.
where λ is the average frequency of avalanche events, and
xn are the time intervals between samples. From (1) and
(2) can be obtained in form [
        <xref ref-type="bibr" rid="ref6 ref9">6,9</xref>
        ]:
      </p>
      <p>In gallium arsenide avalanche photodiodes used in QC
quantum detectors, the exponential model for dark counts
is violated due to post-pulse counts. The effect of
postpulse counts is the process of re-emission of charges
captured by the avalanche diode traps during the previous
avalanche event. The traps inside the diode are not due to
the ideality of the detector and its
manufacturing
technology.</p>
      <p>
        The first models describing post-pulse counts were
constructed on the
basis
of a
simple
exponential
dependence of the probability density on the inter-pulse
interval [
        <xref ref-type="bibr" rid="ref10 ref11">10,11</xref>
        ]. This expression depends on the amplitude
of the probability and the decay time. However, this
expression describes well the processes in the "free-run"
mode and does not accurately describe the readings of
devices operating in the "gating" mode. In [
        <xref ref-type="bibr" rid="ref10">10</xref>
        ], it was
shown that in this mode, post-pulse counts are well
described by a power function of the form
      </p>
      <p>=    ,
where C and α are positive parameters, t is time in counts.
In this paper, it is assumed that a possible reason for this
dependence is the wide distribution of trap energy in the
used semiconductor avalanche diode.</p>
      <p>Moreover, the
values of the parameters C and α depend on the shape of
the density function of the energy distribution of the traps.
(4)
(1)
(2)
(3)</p>
      <p>
        The characteristic value of the parameter α for InGaAs/InP
detectors is 1.2 ± 0.2 [
        <xref ref-type="bibr" rid="ref10">10</xref>
        ].
      </p>
      <p>
        Expression (4) describes with high accuracy the
statistics of post-pulse readings. The reasons for this are
that the charge traps in the avalanche photodiode have a
wide energy distribution. This circumstance does not
allow us to describe the statistics of readings by a single
decaying exponent, which determines a single Arrhenia
relaxation process. Of course, it is possible to improve the
degree of fitting by choosing as the fitting function the sum
of exponentials with different decay times, however, the
number of exponents is not a fixed parameter and the
physical meaning of the parameters obtained is not clear.
It is important to note that each value of the probability
distribution function in (2) and (4) is obtained by
calculating a statistically suitable number of experimental
points in a small time interval. Thus, to obtain the
dependence of the probability distribution function that is
suitable for analysis on the inter-pulse intervals, a large
number of experimental values are required (of the order
of 106 values [
        <xref ref-type="bibr" rid="ref11">11</xref>
        ]).
      </p>
      <p>For the data obtained in the experiment, we test
statistical hypotheses of the form
(2), (4)
with an
additional factor introduced for testing flexibility. In
addition, we are testing a new hypothesis for a probability
of the form P=A/(1-e-Bt), which is a solution of a nonlinear
equation
of
the
form
dP/dt=aP+bP2,
potentially
corresponding to possible strong nonlinear effects on
microscopic level of description of quantum detectors. The
results of quantitative parametrization of dark samples
with a small number of post-pulse counts for a working
QC system are shown in Fig. 1.</p>
      <p>
        We see that for the new hypothesis and Poisson theory
[
        <xref ref-type="bibr" rid="ref7">7</xref>
        ], the results of estimating noise in the region of small
times t&lt;3 us are more accurate than for Itzler's theory [
        <xref ref-type="bibr" rid="ref10">10</xref>
        ].
However, the asymptotic behavior of the curves on a
logarithmic scale indicates the need for a more competent
account of the distribution tails in the region of large times
t&gt;3 us, which is not so simple to do in the framework of
one consistent physical theory [
        <xref ref-type="bibr" rid="ref10">10</xref>
        ]. Here we see the
imperfection of theoretical models, which is difficult to
overcome within the framework of theoretical models of
noise analysis with a small finite number of parameters,
but it is easy to overcome within the framework of
nonparametric statistical criteria for noise analysis, such as
SRA.
density of dark counts for the working QC system
      </p>
    </sec>
    <sec id="sec-4">
      <title>4. SRA analysis of dark noise</title>
      <p>Expression (4) we will base the model of post-pulse
counts based on SRA. In the case when the samples
dominated by the counts due to the effect of post-pulses,
we can substitute (4) in (1) and get:</p>
      <p>xn= xmin (N/(n-1))1/(α-1), (5)
where xmin is the minimum time value equal to the dead
time Tho, N is the number of points in the sample. Eq. (5)
has only one adjustable parameter α.</p>
      <p>
        Note that Eq. (3) and (5) contain each experimental
value. Thus, in this case, to obtain a dependence suitable
for analysis, a much smaller number of experimental
values (of the order of 103–104 are required in comparison
with the probability distribution functions obtained from
the histograms. In Fig. 2 shows the parametrization of dark
noise with a sufficient proportion of post-pulse samples
based on formula (5) with an additional factor for testing
flexibility, which corresponds to Itzler's theory [
        <xref ref-type="bibr" rid="ref10">10</xref>
        ].
      </p>
      <p>In Fig. 2 on a logarithmic scale, we clearly see that
starting from t&gt; 24 us, Itzler's theory ceases to work. Thus,
in addition to fast parametrization of noise by theoretical
models, we can also quantify the applicability limits of
models using non-parametric analysis of the tails of the
distribution of SRA.</p>
    </sec>
    <sec id="sec-5">
      <title>5. Relative SRA for different operating modes of QC</title>
      <p>
        Explicit statistical accounting of the noise of quantum
detectors allows you to most correctly select the mode of
use of the detectors to realize the most efficient quantum
communication with the highest signal to noise ratio.
Direct statistical analysis and robust diagnostics of the
noise of quantum detectors can be done by distributing the
times tags of quantum keys that are available for the online
diagnostic system and a significant amount of information
about the QC performance (the amount of dark noise and
post-pulse counts, line interference, etc.). Moreover, a
joint statistical analysis of the dynamics of bit errors in
keys and key times tags can become the new standard of
quantum-classical security of quantum communication
complexes as a whole due to the high predictive power of
nonparametric statistical criteria [
        <xref ref-type="bibr" rid="ref3 ref4 ref5 ref6 ref7">3-7</xref>
        ].
      </p>
      <p>In Fig. 3 shows the dependence of
SRA[Constructive]SRA[Dark] on SRA[Dark] for precise distinguishing
between constructive and destructive interference using
times tags within in key for continuous diagnosis of
changes in statistics.</p>
      <p>Unlike parametric criteria with 2-3 evaluation
parameters, the criterion described here is the entire
resulting dependence, that is, 1000 fitting parameters. In
this sense, the power of many advanced nonparametric
criteria is almost incomparable with conventional
parametrization methods. Therefore, despite the difficulty
in comparing nonparametric criteria with real physical
factors, they are hypersensitive even with small changes in
the systems under study and are able to work in the
absence of a priori information. Accordingly, such robust
nonparametric methods as SRA can be used as the basis
for quantum-classical diagnostics of QC.</p>
    </sec>
    <sec id="sec-6">
      <title>6. Conclusion</title>
      <p>Precise error diagnostics in QC depends on a large
number of physical factors that are difficult to track within
the framework of only one structurally finished product. In
our opinion, needed an expanded robust diagnostic
system, which should be supplied with the QC complex
and be able to conduct a joint statistical analysis of such
seemingly different parameters as the time stamps of keys
and the distribution of errors within the key. Such a
quantum-classical diagnostic subnet in the TQN, capable
of diagnosing even small noises in the network in the
absence of a priori information about the type of
interference, also opens up prospects for the
commercialization of quantum-classical cloud services for
robust information protection.</p>
    </sec>
    <sec id="sec-7">
      <title>Acknowledgments</title>
      <p>The work was carried out with partial financial support
in the framework of the topic of the laboratory "Integrated
quantum optics" of the Kazan quantum center
KNRTUKAI (the basic idea of nonparametric analysis and analysis
of results – NSP, AAL). Research in the field of statistics
of quantum detectors and quantum sensors was carried out
with the financial support of RFBR grant No. 19-32-80029
(idea of a microscopic approach to the dynamics of
postpulse counts and the basic statistical verification of this
hypothesis – MAS) and also grant of the Government of
the Russian Federation 14.Z50.31.0040, February 17,
2017 (experiments on the generation of quantum keys –
NSP, MAS, KSM, LRG, OIB, AAL). The work is also
partially supported in the framework of the budget theme
of the laboratory of Quantum Optics and Informatics of
Zavoisky Physical-Technical Institute FRC Kazan
Scientific Center of RAS (numerical modeling in quantum
informatics – NSP, DYT).</p>
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