Research on Phase-Control Technology of Recovery Terminal by
Two-Way Optical Fiber Time Frequency Transfer Method
Cheng Ma
a
, Ming Ma
b
, Hang Gong, Jing Peng, Wenchi Zang and Ting Liu
College of Electronic Science, National University of Defense Technology, Changsha, China
Keywords: Time Frequency Transmission, Phase Control, Two-Way Time Comparison.
Abstract: Optical fiber time-frequency transmission technology is one of the key technologies of satellite navigation
system for global service. With the application background of the construction of time-frequency system in
satellite navigation field, the phase consistency control technology of two-way time-frequency transmission
of optical fiber is studied, and the experimental analysis is carried out. The results show that the phase
consistency control accuracy is better than 100ps when the optical fiber transmission distance is within 10km,
which provides a solution for engineering application of remote time-frequency technology with high
precision.
1 INTRODUCTION
Global Navigation Satellite System (GNSS) is new
generation of radio navigation system, which has the
advantages of global, all-day and all-weather
navigation, positioning, timing and speed
measurement to meet supply urgent demand for
space-time information in many fields in today's
information society
(Gang Xie, 2013). Due to the
complex structure and signal propagation
environment of the satellite navigation system and
scattered locations (Rong Qiang, 2011)
,
It is very
important to realize the high-fidelity time-frequency
signal transmission between the front-end equipment
and the terminal equipment during the time-
frequency signal transmission between the ground
stations of the large-scale satellite navigation system,
which requires the time-frequency signal transmitted
to the terminal to achieve impedance matching within
a long distance and provide a low amplitude Degree
loss, low noise insertion loss, maintain high fidelity
signal quality, especially the demand for signal phase
consistency and time signal synchronization
accuracy.
Optical fiber two-way time-frequency
transmission technology is an ideal transmission
means because of its small transmission attenuation,
a
Male, Master degree candidateEngaged in GNSS
Time-frequency reference transmission and
measurement technology research.
less stability insertion loss, low implementation cost,
simple configuration, convenient and flexible (Zhu X,
2015). According to the relevant literature (Schnatz H
- Lopez O), it can be seen that the current optical fiber
frequency transmission method can reach or exceed
the stability of 1×10
-14
/s, 2×10
-16
/day, and the phase
noise of -120dBc/Hz@1Hz, and the accuracy of
frequency transmission can maintain the same order
of magnitude as the input. However, for the
requirement of phase consistency, this index (Schnatz
H - Lopez O), is not mentioned in the relevant
literature of optical fiber time-frequency transmission
method at present, and there is a lack of engineering
application guidance, so it is difficult to achieve and
needs to be analyzed and studied.
Optical fiber two-way time-frequency
transmission technology needs to solve the phase
synchronization problem of terminal recovery signal.
At the end of the signal recovery, phase noise
purification and distribution after amplification, the
phase between all signals is arbitrary, which is to
obtain the time difference between them and the
front-end signal through phase measurement
technology, and control them to maintain phase
consistency with the front-end signal through phase
adjustment.
Aiming at the difficulty of restoring terminal
phase consistency control by optical fiber time-
b
Corresponding author, Male, PhD, Engaged in satellite
navigation time frequency system technology research
520
Ma, C., Ma, M., Gong, H., Peng, J., Zang, W. and Liu, T.
Research on Phase-Control Technology of Recovery Terminal by Two-Way Optical Fiber Time Frequency Transfer Method.
DOI: 10.5220/0012286900003807
Paper published under CC license (CC BY-NC-ND 4.0)
In Proceedings of the 2nd International Seminar on Artificial Intelligence, Networking and Information Technology (ANIT 2023), pages 520-525
ISBN: 978-989-758-677-4
Proceedings Copyright © 2024 by SCITEPRESS Science and Technology Publications, Lda.
frequency transmission method, this paper proposes
and discusses the design and implementation of a
phase consistency control method for optical fiber
time-frequency signal transmission, and verifies its
feasibility and performance through experimental
analysis.
2 BASIC PRINCIPLE OF FIBER
TWO-WAY TRANSMISSION
METHOD
Optical fiber time-frequency transmission technology
has been studied in foreign countries for more than 30
years. From the initial unidirectional time-frequency
transmission method to the widely used optical fiber
two-way time-frequency transmission method
(Xiaohui LI, 2010), the synchronization accuracy has
entered the sub-nanosecond order, which is an
important means to realize time synchronization
between stations.
The basic principle of fiber two-way time
frequency transmission technology is: station A and
station B send and receive time signals each other
(such as 1PPS), signals generally through
multiplexing technology coupled in A fiber
transmission, because station A and station B send
and receive signals at the same time, two-way
transmission path is basically the same, its
propagation delay can be effectively cancelled; In
addition, if station B can't independently generate the
time-frequency reference, it can also be combined
with one-way time-frequency transmission method to
pass the frequency reference of station A to station B.
Its implementation principle block diagram is shown
as Figure 1:
Figure 1: Principle of fiber optic two-way time frequency
transmission method.
The time of station A is denoted as T
M
, the time of
station B is denoted as T
S
, the comparison and
measurement result of station A is
t
M
, and the
comparison and measurement result of station B is
t
S
. It is assumed that the delay of the transmitting
device at station A is τ
1
, the delay of the receiving
device at station A is τ
2
, and the delay of the
transmitting device at station B is τ'
1
, the delay of the
receiving device at station B is τ'
2
, the optical fiber
path transmission delay is τ, then:
t
M
= T
M
–(T
S
+τ'
1
+τ+τ
2
)
(1)
t
S
= T
S
–(T
M
+τ'
2
+τ+τ
1
)
(2)
let station A and station B use the same
transmitting and receiving technology, it is
considered that τ
1
,= τ'
1
, τ
2
,= τ'
2
, then the time
difference between station A and station B is:
T
M
-T
S
= (
t
M
+
t
S
)
/2
(3)
In formula (3), the circuit delay of station A and
station B at the receiving and transmitting ends is not
equal, and the delay of the device must be measured
and calibrated. At this time, the time difference
between station A and station B is:
2
'
221
'
1
ττττ
++ΔΔ
=
SM
SM
tt
T
T
(4)
In Formula (4), station A and station B use high-
precision phase measurement technology to measure
Δt
M
and Δt
S
, and adjust the time-frequency reference
of the recovery terminal of station B using high-
precision phase control technology according to the
comparison measurement results, so as to realize the
time-frequency transmission and time
synchronization of station A and station B.
3 PHASE CONTROL METHOD
OF OPTICAL FIBER
RECOVERY TERMINAL
When the time frequency signal of the optical fiber
time frequency transmission recovery terminal is
recovered, multiple types of local time frequency
signals will be generated, and the delay of multiple
PLL and frequency division circuit will be
inconsistent in the design, and each time the device is
started, reset or PLL relock will cause large delay
uncertainty, resulting in non-synchronization
between multiple types of time frequency signals.
Therefore, a local high-resolution phase regulation
method is needed to regulate the local signal
according to the time difference between stations
calculated by the two-way time and frequency
transmission method of optical fiber, so that the phase
consistency of the multi-class time and frequency
signals generated locally in real time is constrained
within a reasonable index range, and high-precision
Research on Phase-Control Technology of Recovery Terminal by Two-Way Optical Fiber Time Frequency Transfer Method
521
services are provided for the back-end time-used
frequency equipment.
3.1 Principle of High-Precision Phase
Adjustment Method
High-precision phase adjustment can be achieved by
controlling the output phase of the frequency
synthesizer. PLL (Phase Locked Loop) based on DDS
(Direct Digital Synthesis) The frequency synthesis
technology of Loop is a high-precision phase
adjustment method, which has the advantages of
simple structure, convenient control, high phase
control accuracy and resolution (<lps), unrestricted
phase control range, and low cost. The principle of
the specific design and implementation method is
shown as figure 2:
out
ϕ
ref
ϕ
R1
ϕ
N1
ϕ
Figure 2: A high-precision phase adjustment method for
PLL based on DDS.
Figure 2 PLL high-precision phase adjustment
method of DDS schematic block diagram. The above
is a closed-loop phase negative feedback control
system. In the basic PLL structure shown in the
schematic diagram, PLL is used to realize frequency
synthesis. In order to ensure the phase noise index of
the output frequency signal, OCXO is selected as
VCO; Loop phase is automatically controlled by DDS
negative feedback, PLL loop output phase is realized
by controlling 1N in the output phase of DDS, and at
the same time, the N frequency divider is matched
with the input reference R frequency divider for phase
identification: PLL output is used as the clock of the
post-stage time-frequency reference regeneration.
Considering the phase control relationship of PLL, in
the PLL loop, the phase discriminator thinks that the
output phase of the N divider is the output phase of
the VCO, that is, the final output phase of the PLL
loop. When the VCO output phase changes, the N
frequency divider phase changes, the phase
discriminator output adjustment voltage control VCO
to adjust the phase, and finally the phase
discriminator two input phase equal to reach a steady
state. R divider and N divider will introduce phase
delay when realizing frequency division, respectively
recorded as IR and IN, loop steady state phase divider
R divider and N divider output phase equal, then PLL
output phase 0out and reference input phase n has the
following relationship:
NRrefout 11
ϕϕϕϕ
+=
(5)
According to formula (5), the PLL output phase is
determined by the phase delay of the R divider and
the N divider. Changing the phase delay of the N/R
divider will also change the output phase of the PLL,
and then realize the delay adjustment of the back-end
time-frequency reference signal. In this scheme,
phase adjustment is carried out by changing the N
frequency divider of DDS. The formula of res of DDS
phase control resolution can be obtained by referring
to (
Gong Hang, 2008):
DDSclk
D
NN
DDSout
res
f
N
T
pp
,
,
2
1
2
==
ϕ
(6)
In formula (6), where N is the phase control word
length and f
clk,DDS
is the DDS output frequency. As
can be seen, the resolution is not only related to the
phase control word length, but also directly related to
the output frequency of DDS, the greater N, the
higher f
clk,DDS
, the higher resolution.
3.2 Local Time-Frequency Signal
Phase Control Method
For the phase alignment of local time-frequency
signal, a phase control method of local time-
frequency signal based on optical fiber two-way
comparison measurement data, DDS phase lock
adjustment and ARM automatic control is proposed.
The implementation principle is shown in FIG3. Set
the reference input signal f, the measured signal f is
also the feedback signal of the local output time-
frequency signal, and fou is the local output time-
frequency signal.
If f
r
is completely synchronized with station A
through the method in Section 2, then when f
r
is
aligned with the phase of f
out
, the phase comparison
result measured by the external high-precision phase
comparator (PCO) is T
r,
assuming that the time delay
between the two measuring channels of PCO is equal
to the cable time delay, then T
r,
≈0,
It can be considered that the phase of the recovery
terminal time-frequency signal at station B has been
completely synchronized with that at station A. Set
the real-time phase difference of the measurement of
two-way comparison at this time to
T, then through
real-time monitoring of the difference between the
measurement value of two-way comparison and the
zero value
t=
T-T
1
you can achieve real-time
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522
control and alignment of the phase of the local time-
frequency signal, set the threshold of real-time phase
adjustment toΦ, then:
onturn
offturn
Φ
Δτ=ΔΤ- Τ
Φ
Δτ=ΔΤ- Τ
1
1
(7)
Through the real-time monitoring of formula (7)
decision conditions by ARM microprocessor, the
phase of the local time-frequency signal can be
aligned in real-time self-closed loop phase to achieve
local phase consistency control.
1
τ
2
τ
1
T
T
Δ
tΔ
0
τ
Figure 3: Principle of local time-frequency signal phase
alignment method.
The method principle of phase consistency
control of local time-frequency signal by using
optical fiber two-way comparison of real-time
measurement data and initial calibration zero value is
discussed above. The implementation process is
shown as figure 4:
Figure 4: Phase alignment method implementation flow
chart Specific.
Implementation steps are:
1) When measuring for the first time, calibrate
the zero value
T of the output time-
frequency signal by the local reference time-
frequency reference, and store the initial
calibration zero value in the phase control
register;
2) the optical fiber time ratio is compared with
the phase comparison result T
1
of real-time
measurement and the zero value
T, and the
result is
t;
3) When
t exceeds the threshold, turn on the
output signal Real-time phase adjustment of
f
out
;
4) Stop real-time phase alignment when
t
reaches within the threshold.
4 TEST ANALYSIS
4.1 The Design of Test
Test scheme combined with the phase control method
of the optical fiber recovery terminal in the upper
section, the two-way optical fiber two-way
comparison method and DDS phase modulation
technology were used to verify the method through
the test design, and the test design scheme was
connected with the block diagram is shown as figure
5:
Figure 5: Block diagram of the test design scheme.
The time-frequency reference in the figure above
is a hydrogen atom clock. The homologous hydrogen
clock in the reference source of the test and
verification system has passed the metrological
inspection, proving that its indicators are accurate and
reliable; The time-frequency transmission terminal
and time-frequency recovery terminal are self-
developed prototypes; The test system is composed of
phase noise analyzer, time interval tester and other
measuring equipment, and the test fiber is 10km. The
temperature control box is used for temperature
regulation and constant temperature control of the test
optical fiber.
In the two-way time comparison method, the
positive pseudo-code ranging result is
t
M
,,the
positive pseudo-code ranging result is Ats, the time of
the main station is recorded as T
M,
the terminal time
is recorded as T
S
, the link delay of optical fiber
transmission is τ, the time difference between the
central node IPPS and the distribution node 1PPS is
T
MS=
T
M,
-T
S
,and according to formula (1) and formula
(2), then:
Research on Phase-Control Technology of Recovery Terminal by Two-Way Optical Fiber Time Frequency Transfer Method
523
==+=Δ
==+=Δ
τττ
τττ
MS
T
s
T
M
T
M
T
S
T
S
t
MS
T
s
T
M
T
S
T
M
T
M
t
-)()(
-)()(
(8)
For the control of the phase consistency between
the central node 1PPS and the distributed node 1PPS,
the phase difference that the distributed node 1PPS
needs to compensate is T
MS
, and the phase consistency
can be regarded as that the amplitude of T
MS
, T
MS
can
be controlled within the range of the phase
consistency index by compensating T
MS
in real time.
4.2 Analysis of Results
During the test and verification, the output phase
consistency under two typical application scenarios is
analyzed.
1) When the central node is the same origin as the
distributed node, and the link delay t has no
fluctuation and is A constant, then:
==Δ
==Δ
=
=
A
MS
T
S
t
A
MS
T
M
t
A
MS
T
τ
τ
τ
0
(9)
Formula (9) can be understood as that under ideal
conditions, the delay of one-way frequency
transmission is fixed, and the clock difference of two-
way time comparison is about zero. At this time, for
distributed nodes, it is necessary to compensate the
fixed zero value of the frequency transmission system
and align the internal phase to realize the phase
consistency control between stations A and B. The
test results in this scenario are shown as figure 6:.
Figure 6: 1PPS phase difference between Station A and
Station B(S1).
2) When the central node is the same origin as the
distributed node, the link delay rfluctuates and is a
variable value, then:
==Δ
==Δ
=
ττ
ττ
MS
T
S
t
MS
T
M
t
MS
T 0
(10)
Formula (10) can be understood as the real-time
phase alignment adjustment is enabled when the
optical fiber is subjected to the temperature regulation
delay fluctuation in the temperature control box, the
delay fluctuation of one-way frequency transmission
is effectively compensated, and the forward delay and
reverse delay change laws of two-way comparison are
consistent. At this time, the delay fluctuation of the
time frequency transmission of the recovery terminal
of station B is dynamically compensated, and the
fixed zero value of the system is also compensated to
realize the phase consistency control of station A and
station B. The test results in this scenario are shown
as figure 7:
Figure 7: 1PPS phase difference between Station A and
Station B(S2).
4.3 Test Summary
In the two test groups, due to the homology test, the
clock difference between station A and station B is
zero, and the 1PPS phase difference between station
A and station B is significantly affected by the
fluctuation of link delay. The T
MS
values of the two
scenarios were statistically analyzed, and the
maximum value of each group of TMs in the table
was defined as the phase consistency measurement
results of the group of experiments. Details are
shown as Table 1:
Table 1: Statistics of phase consistency test results.
Experimental
Scenario
Phase difference consistency
control results
S1 0.05ns(50ps)
S2 0.09ns(90ps)
0 5 10 15 20 25
-0.08
-0.06
-0.04
-0.02
0
0.02
0.04
0.06
0.08
time (h)
T
MS
(ns)
0 5 10 15 20 25
-0.08
-0.06
-0.04
-0.02
0
0.02
0.04
0.06
0.08
time (h)
T
MS
(ns)
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524
Based on the above analysis, under the condition
of 10km indoor optical fiber, the phase-consistency
control accuracy of the time-frequency signal
transmission method designed in this paper is less
than 100ps.
5 CONCLUSION
In summary, we have come to the following
conclusion:
1) High precision time-synchronization within
and between stations can be achieved.
Using fiber two-way time-frequency transmission
can effectively eliminate the asymmetric error of
delay, but the accuracy of two-way comparison with
drastic change of delay is worse than that of stable
change of delay. Through the phase control of
terminal recovery signal, the phase synchronization
accuracy of recovery signal can reach sub-
nanosecond or even higher.
2) It is completely feasible to use the
measurement data of optical fiber two-way time
frequency method to carry out phase consistency
control on the recovery terminal.
The phase consistency test of two-way optical
fiber comparison under different scenarios is
analyzed. The results show that the phase consistency
control method of optical fiber time-frequency signal
transmission designed in this paper, by realizing
phase consistency control, recovers the phase
consistency control of the time-frequency signal
output by the terminal (station B) and the 1PPS signal
output by the main station (station A). At the
transmission distance of 10km optical fiber, the time
comparison measurement accuracy of the two
scenarios is better than 100ps, which is further
verified the proposed phase control method of optical
fiber recovery terminal is feasible in engineering
application.
ACKNOWLEDGMENTS
National Natural Science Foundation of Hunan
(2021RC3073).
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