OZ OPTICS DTS0144 Adjustable Polarization Insensitive Variable Bandwidth Tunable Filters Owner’s Manual
- June 3, 2024
- OZ Optics
Table of Contents
- OZ OPTICS DTS0144 Adjustable Polarization Insensitive Variable Bandwidth
- PRELIMINARY SPECIFICATIONS
- Product Description
- Ordering Information for Standard Parts
- Ordering Example for Standard Parts
- **Part Number
- Frequently Asked Questions (FAQs)
- Application Notes
- References
- Read User Manual Online (PDF format)
- Download This Manual (PDF format)
OZ OPTICS DTS0144 Adjustable Polarization Insensitive Variable Bandwidth
Tunable Filters
PRELIMINARY SPECIFICATIONS
Features
- 45 nm tunable wavelength range
- 1 to 18 nm continuously adjustable bandwidth
- Independently tunable both wavelength and bandwidth
- Flat-top filter shape
- Available for wavelengths from 1100 nm to 1650 nm
- Polarization insensitive
- High r esolution
- Singlemode, polarization maintaining, and multimode fiber versions
- High out-of-band suppression
- High input power handling
Applications
- WDM channel filtering
- High-speed transmission testing
- Signal f iltering
- Laser pulse shaping
- ASE light noise suppression
- Tunable light sources
- Spectral analysis
- Fiber optic component manufacturing
- Quality control and measurement
- Product development
Product Description
The manually adjustable variable bandwidth tunable filter is a pig-tailed
component with adjustment knobs that allow both the wave-length and bandwidth
of the filter to be controlled. The device con-tains two independently
variable tunable bandpass filters in series. With the two filters tuned to
cover slightly different wavelength ranges, the overall passband becomes the
region where the two individual passbands overlap. The amount of overlap
determines the width of the filter. Since each filter can be tuned over a
range of wavelengths, both the center frequency and width of the passband can
be controlled. Each individual filter consists of a multi-layer thin film band
pass filter, designed to give a flat top pass band, with steep roll-off
shapes.
The center wavelength of the filters is adjusted by changing the angle of
incidence of the light as it impinges upon the filter. In the Variable
Bandwidth Tunable Filter, each filter is independently rotated relative to the
incoming light, in order to change the passband. OZ Optics uses a special
technique to minimize polarization dependencies, allowing PDL effects to be
kept below 0.3 dB, and making the spectral response virtually polarization
independent. This feature makes it ideal for today’s DWDM system applications.
Variable bandwidth tunable filters using singlemode, and Polarization
Maintaining (PM) fibers are offered. In general, OZ Optics uses polarization
maintaining fibers based on the PANDA fiber structure when building
polarization maintaining components and patch cords. However, OZ Optics can
construct devices using other PM fiber structures. We do carry some
alternative fiber types in stock, so please contact our sales department for
availability. If necessary, we are willing to use customer-supplied fibers to
build devices.
Ordering Information for Standard Parts
Standard Parts
Bar Code | Part Number | Description |
---|
56160
| ****
BTF-11-11-1525/1565-9/125-S-60-3S3S-1-1-1/18
| Polarization insensitive manual variable bandwidth tunable filter for 1525–1565 nm with 1 meter long, 1mm OD jacketed 9/125 SM fiber pigtails, 60dB return loss, super FC/PC connectors, and 1–18 nm variable FWHM Fabry Perot filter.
Standard Product Specifications
Part Number | BTF-11-11-1525/1565-9/125-S-60-3S3S-1-1-1/18 |
---|---|
Wavelength Range | 1525 – 1565 nm; Other ranges available on request |
Bandwidth (FWHM) | 1 – 18 nm |
Wavelength Resolution | 0.1 nm |
Filter Edge Roll Off Slope | 10 dB/nm |
Insertion Loss | 3 dB for complete device over full tuning range |
Polarization Dependent Loss (PDL) | Typically less than 0.3 dB |
Transmission Shape | Flat-top |
Wavelength/Temperature Sensitivity | 0.002 nm/°C |
Power Handling | Up to 200 mW for standard package |
Fiber Type | SMF-28 (or SMF-28e) |
Operating Temperature | -10° to 55°C |
Storage Temperature | -30° to 70°C |
1 Typical values. Tested at 23°C.
Ordering Example for Standard Parts
A customer wants a manual variable bandwidth tunable filter to filter ASE
light noise from the transmitted advanced modulation format light signals, in
order to test their characteristics at different DWDM channel frequencies.
Those different modulation format signals have different spectral bandwidths
and spectral shapes that are dependent on the modulation formats. The
transmitted signal light is tapped out from the monitoring port with FC/PC
receptacles and the wavelength regions of interest for the signals under test
(SUT) are throughout the C-band. The transmitted light signals are polarized
with random states of polarization (SOPs), and have different spectral
bandwidths. Therefore, the filter required for the test should be polarization
insensitive with an adjustable filter bandwidth,tunable across the entire
C-band.
With this filter connected to the monitoring fiber from the DWDM network, the
ASE noise light level can be reduced to a minimum for any spectral bandwidth
signals without decreasing the signal intensity, i.e. to achieve a best OSNR
for the transmitted light signals.
These requirements can be met with the part identified below:
Bar Code | Part Number | Description |
---|
56160
|
BTF-11-11-1525/1565-9/125-S-60-3S3S-1-1-1/18
| Polarization insensitive manual bandwidth variable tunable filter for 1525–1565 nm with 1 meter long, 1mm OD jacketed 9/125 SM fiber pigtails, 60 dB return loss, super FC/PC connectors, and 1–18 nm adjustable FWHM Fabry Perot filter.
Ordering Information for Custom Parts
OZ Optics welcomes the opportunity to provide custom designed products to meet
your application needs. As with most manufacturers, customized products do
take additional effort so please expect some differences in the pricing
compared to our standard parts list. In particular, we will need additional
time to prepare a comprehensive quotation, and lead times will be longer than
normal. In most cases non-recurring engineering (NRE) charges, lot charges,
and a 1 piece minimum order will be necessary. These points will be carefully
explained in your quotation, so your decision will be as well informed as
possible. We strongly recommend buying our standard products.
Questionnaire for Custom Parts
- What operation wavelength range are you interested in?
- What variable bandwidth range do you require?
- What type of fiber is being used? Singlemode, PM, or multimode fiber?
- Are you using a polarized or randomly polarized light source?
- What return losses are acceptable in your system?
- What connector types are you using?
- What fiber length and jacket diameter do you need?
**Part Number
**
Ordering Example for Custom Parts
A customer wants to reduce the ASE light noise for transmitted signals using
different spectral bandwidths, manually tuning the trans-mitted light
wavelength between the C and L bands, (1550 to 1600 nm), and manually
adjusting the transmitted light spectral linewidth from 1 nm to 18 nm.
A custom version of the manual variable bandwidth tunable filter will meet
this requirement, as shown below:
Bar Code | Part Number | Description |
---|
N/A
|
BTF-11-11-1550/1600-9/125-S-60-3U3U-1-1-1/18
| Polarization insensitive manual variable bandwidth tunable filter for 1550–1600 nm with 1 meter long, 1mm OD jacketed 9/125 SM fiber pigtails, 60dB return loss and ultra flat FC/PC connectors. Custom 1 – 18 nm FWHM Fabry Perot filter.
Frequently Asked Questions (FAQs)
Q: What is the filter bandwidth?
A: The standard variable bandwidth tunable filter has an adjustable bandwidth
(FWHM) from 1 nm to 18 nm, consisting of two tunable
bandpass Fabry-Perot type filters. This can be customized to suit the
customer’s requirements.
Q: What is the largest tuning range available?
A: The standard tuning range is 45 nm. However, the filter can be operated
over a wider range with some effects on the insertion loss
and polarization dependent loss in the shorter wavelength (high angle of
incidence) region.
Q: How do you define your bandwidths?
A: Standard filters are specified by their Full Width Half Maximum (FWHM).
This is the transmitted bandwidth at -3dB from the peak
transmission. For custom filters, bandwidths such as the passband at -1dB and
-25dB can be specified upon request.
Q: Is the shape of the transmission curve affected by the polarization?
A: No, OZ Optics tunable filters utilize an optical technique to control
Polarization Dependent Losses (PDL). This design reduces PDL
to a minimal level, while at the same time making the spectral response
polarization insensitive.
Q: How well does the filter block unwanted wavelengths?
A: For the standard filters the typical operation wavelength is in the C-band
(between 1530 nm and 1565 nm) with a light pass band width from 1 nm to 18 nm.
This type of filter is good for selecting any channel signals in a DWDM system
or cleaning up the ASE noise from a broadband light source in the C-band.
However, the filter may still transmit light at wavelengths significantly
outside the operating wavelength range. For custom applications that require
operation over different wavelength regions or different variable filter
bandwidths, please contact OZ Optics.
Q: Is the unit calibrated?
A: No, the manual variable bandwidth tunable filter is a low cost, flexible
solution to bandwidth adjustable tunable filter needs and is not calibrated
due to its manual use. However, OZ Optics does take great care in the
production of these units in order to meet or exceed the optical properties
required by the customers.
Application Notes
Introduction To Thin Film Filters:
In many fiber-optic applications we need to use light with a specific
frequency or wavelength (λ) and a specific linewidth. Although a laser may be
an excellent source of monochromatic radiation, we might still need a source
of light providing controlled, variable wave-length, and even variable
linewidth. Variable bandwidth filters provide an effective means of
transmitting a well-defined band of light while blocking unwanted wavelengths
emanating from a broadband source. This is useful when dealing with DWDM/
ROADM signals, or advanced modulation signals.
OZ Optics’ Variable Bandwidth Tunable Filter uses an innovative filter design
to tune both filter wavelength and linewidth at the same time (Figure 3). As
the angle of incidence changes, the range of wavelengths passing through each
filter changes. By controlling the angle of each filter relative to the
incoming light, the upper and lower limits of the passband can be controlled,
creating a tunable filter with an adjustable passband.
The typical output wavelength distribution is demonstrated in Figure 4. An adjustable linewidth is achieved by the light passing through common wavelength regions of the two bandpass filters. The spectral linewidth can be adjusted from 1 nm to 18 nm for a wavelength tunable range between 1525 and 1565 nm.
A big problem with typical variable bandwidth tunable filters that has been solved by OZ Optics is their polarization sensitivity. As the angle of incidence increases, the sensitivity to polarized light also increases. (See Figure 5) This is a very important point in optical systems as the separation of the S and P polarization states causing a large PDL can have detrimental effects on the system.
OZ Optics’ variable bandwidth tunable filters utilize an optical technique to control PDL making the spectral response polarization insen-sitive. The polarization insensitivity is accomplished through the precision alignment of optical components on both the input and output side of the filter. As demonstrated in Figure 6 below, the light is first split into its respective polarizations and then one of the polarizations is rotated such that the light incident on the filters is all the same polarization. After passing through the filters the other polarization is rotated and then the beams are combined for the final focusing and collection into the fiber. By rotating the light and having a common polarization pass through the filters the PDL effect of the filters at high angles of incidence is avoided. Therefore, the spectral response of S and P polarizations remain the same for increasing angles of incidence. See Figure 7.
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References
Read User Manual Online (PDF format)
Read User Manual Online (PDF format) >>