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A2000 Component Analyzer Family
Swept Wavelength Systems for PMD, PDL, IL Analysis
2006
All-Parameter-JME for Accurate
PMD/DGD-Characterization
Müller Method for Accurate PDL-
Characterization
T
T
he well-known Jones-Matrix-Eigenanalysis
(JME) has become the standard method for
measuring Polarization Mode Dispersion (PMD)
or differential group delay (DGD) of optical
devices.
Adaptif PHOTONICS pushes the limits with its
:
:
PMD/DGD, PDL, Insertion Loss, 2nd-
order PMD (Depolarization + PCD),
TE/TM Insertion Loss
:
Full specified performance across C-
and L-band within a single sweep.
Typical update rate: < 8 seconds.
:
Accurate results even when operating
in harsh environment. Taping patch
cords to the table is not required.
he Müller Method is an established tool for
measuring polarization dependent loss
(PDL) with high accuracy. A very similar
approach is taken by the All-Parameter-JME
using the same data originally collected for the
DGD measurement. Therefore, only a single
sweep is needed to measure PDL and DGD with
excellent accuracy.
All-Parameter-JME
Single-sweep measurement of
Faster measurement speed
Robust against fiber movements
and drifts
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Key Benefits:
Applications:
Support of Common Tunable Laser
Sources:
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High-throughput in production test
systems
High-accuracy component
characterization
Passive component testing:
filters, isolators, circulators, fibers,
ROADMs, etc. (no length limitation)
Active component testing:
EDFAs, SOAs, VOAs
Intra-channel PMD/PDL
measurement
Agilent 816XX/819XX Series
NetTest Tunics Series
Yokogawa AQ4321, AQ2200-136
NewFocus Velocity 6300 Series
PMD/PDL-MEASUREMENT
Product Highlights:
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High-Speed Acquisition of PMD, PDL
and Power/Loss using Jones Matrix
Eigenanalysis (JME) method
High repeatability due to optical self-
calibration
Covers S-, C-, L-band and 1.3um
window
Robust - No moving parts
Contains full function set of our High
Speed Polarization Analyzer and
Polarization Controller
Remote control via Ethernet
PC software package provided:
polarizationNAVIGATOR
Software drivers available for
LabView, MATLAB, VBA, Python
Versions with integrated
touchscreen/computer available
(B3 and R3 options)
Displayless versions available
(external computer required, BT and
R2 options)
TM
Instrument Setup
The A2000 instrument contains a Lithium
Niobate polarization controller and a
polarimetric receiving unit, as shown in the figure
on the right. An internal optical switch provides
self-calibration capabilities and guarantees
always highly precise and repeatable
measurements.
The SOP of the laser input signal is switched by
the polarization controller to a defined set of
polarization states and launched into the Device
under Test (DUT). The DUT output signal is
received by the internal polarimeter unit.
Algorithms implemented on either the internal
(B3 and R3 option) or external computer (BT and
R2 option) provide the desired parameters.
Polarization
Controller
Microcontroller unit
GPIB, USB, Ethernet, RS232
Trigger in
Trigger out
Power
Laser Input OutputPolarimeter
Input
Polari-
meter
DUT
Reference switch
A2000 Component Analyzer Instrument Setup
A2000-B3 Component Analyzer with
Integrated Industry PC and Touchscreen
Flexible Form Factors
The A2000 Component Analyzer family
includes models for benchtop use as well as
for rack-mount. Depending on the customer’s
preference, the instruments are controlled by an
external computer (BT and R2 options) or an
internal industry PC with touchscreen (B3 and R3
option). All instruments include a GPIB-master
port to directly control the third-party laser
sources.
Resolving TE/TM Insertion Loss
The TE/TM-function allows accurate
determination of the minimum and
maximum loss of the DUT at each wavelength.
Due to birefringence, optical filters tend to show
different transmission functions depending on
the polarization state. As shown in the figure
above, these functions are typically shifted in
wavelength depending on the amount of
birefringence.
Wavelength [nm]
Insert
ion
Loss
[dB
]
1559 1560 1561-50
-40
-30
-20
-10
0
Wavelength [nm]
TE
/TM
Loss
[dB
]
1521.2 1521.3 1521.4 1521.5-30
-20
-10
0
Wavelength [nm]
Insert
ion
Loss
[dB
]
Long-Term Measurements
The capability of performing quick PMD-
m e a s u r e m e n t s m a k e s t h i s
measurement system well-suited for
collecting long-term PMD data. The
polarization NAVIGATOR software allows
to continuously collect the spectral PMD
data and store it on the hard disc. The data
can then be visualized as pseudo-color plot
(see figure).
TM
DGD
Wavelength
Tim
e
DGD
DG
D
Wavelength
A2000-BT Component
Analyzer
PRODUCT FAMILY
MEASUREMENT EXAMPLES
Insertion Loss with High Dynamic
Particularly for characterizing optical filters,
the high dynamic range of the A2000 allows
accurate resolution of the filter’s sidelobes.
The internal reference path allows to measure
insertion loss spectra with excellent accuracy
minimizing the influence of the power
characteristics of the tunable laser source.
Excellent Spectral Resolution
Due to the excellent spectral resolution,
the A2000 is best suited for intra-
channel DGD/PDLcharacterization.
The All-Parameter-JME algorithm allows
flexible adjustments of the wavelength
resolution without the need to repeat the
measurement. This allows to easily find the
optimum trade-off between PDL/DGD
accuracy and wavelength resolution.
TE/TM Insertion Loss Function
of an Optical Filter Sidelobes of an Optical Filter 2.5 GHz DPSK Demodulator
Long Term DGD Spectra of Installed Fiber Links
A2000-R2 Component Test System
with Agilent Tunable Laser Source
1545 1546 1547 1548 1549-60
-40
-20
0
A1 A2 B C D
850-1000nm
950-1100nm
1260-1640nmWavelength Operating Range
Factory Calibration Range 980nm 980nm 1270-1375nm
1460 -1620nm
1270-1375nm,1460-1620nm
Resolution 50pm 1pmWavelength
Accuracy 100pm 15pm
Range 0-200ps 0-1000psPMD
Accuracy +/- (0.03ps + 2% of PMD value)
Range 0-10dB 0-10dBPDL
Accuracy +/- (0.01dB + 4% of PDL value)
Dynamic range >57dB
Input Power Range -35dBm
...+10dBm
-40dBm
...+10dBm
-50dBm ... +7dBm
Optical Connector FC or Multipurpose Adapter (FC, SC, ST, LC, DIN, E2000), straight/angled
Operating Temperature range +5 C ... +40 C
Interface Ethernet , GPIB, USB, RS232
Power 100V 240V
Physical R3: 19 wide, 5.25 high R2: 19 wide, 3.5 high BT: 12 x 10.6 x 2.75
adaptif PHOTONICS reserves the right to make product changes without notice. 2006 © adaptif PHOTONICS GmbH
CONTACT
adaptif PHOTONICS GmbH
Harburger Schlossstr. 6-12
21079 Hamburg, GERMANY
Phone +49-40 766 29 2160
Fax +49-40 766 29 2161
www.adaptif.de
Your local sales contact
ORDERING INFORMATION
A2000 - H H - X - M - Y - Z
Wavelength Range
A1 = 850nm - 1000nm
A2 = 950nm - 1100nm
B = 1270nm - 1375nm
C = 1460nm - 1620nm
D = 1270nm - 1375nm
1460nm - 1620nm
Model*)
BT = Benchtop Unit
R2 = 2U Rack Unit
B3 = 3U Benchtop Unit
with Touchscreen
R3 = 3U Rack Unit
with Touchscreen
DUT Ports
0 = straight
1 = angled
Connector Type
0 = FC
1 = Multipurpose
Adapter
Laser Port
0 = straight
1 = angled
For connector type “Multipurpose Adapter”, three
connector adapters are needed in addition:
CON - T T T T
Available Types:
FC, SC, DIN, ST, LC, E2000
CHARACTERISTICS
° °
“ “ “ “ “ “ “
(1)The wavelength range for passivecomponent test applications isdetermined by the overlap betweenthe wavelength range of the tunablelaser and the wavelength range of theselected A2000 instrument.
(2)
(3)
(4)
(5)
(6)
Other factory calibration wavelengthranges on request.
Typical values for operation with NewFocus Velocity 6300 series tunablelaser sources.
Valid for operation with Agilent familyof tunable lasers. Becausewavelength accuracy is determinedby the tunable laser, operation withother lasers may result in differentwavelength accuracy.
Average DGD value across 100nmwavelength range.
Only A2000-R3 and A2000-B3.
(1)
(2)
(4)
(4)
(5)
(6)
*) Note that a third-party laser source isrequired for operation.
The BT and R2 models require a standardpersonal computer with USB port orNational Instruments GPIB interface foroperation.
(3)
(3)
...
>35dB >40dB