High Precision Analysis of Beam Quality and Spatial Power Distribution
Single Stand-Alone Measurement Head
For Continuous and Pulsed Laser Beams
Variable Scanning Speed
Power Meter Integrated (not calibrated)
High Dynamic Range
Low Noise Amplifier
Gaussian Fit Function
2D or Pseudo 3D Diagrams
Average and Max-Hold Functions
Powerful GUI: Separate X and Y Profiles
Fast USB 2.0 Interface to PC, Live Data Readout Via TCP/IP to a DataSocket Server
Item #
BP10x-UV
BP10x-VIS
BP10x-IR
BP10x-IR2
Wavelength Range (nm)
200 - 1100
400 - 1100
700 - 1800
1000 - 2700
Detector Type
Si - UV Enhanced
Si
Ge
Extended InGaAs
Aperture Diameter
4 mm (BP104-xx), 9 mm (BP109-xx)
Slit Size
2.5 µm (BP104-xx), 5 µm (BP109-xx)
Min Beam Diameter
10 µm (BP104-xx), 20 µm (BP109-xx)
Thorlabs' dual scanning slit Beam Profiler is easy to align and features fast simultaneous measurement of both the X and Y profiles with a large dynamic range of 72 dB. The beam diameter is measured in accordance with the ISO11146 standard. The diameter of the beam can be displayed using a number of industry standard clip levels such as 1/e2 (13.5%) and 50% or an arbitrary clip level input. Please see the User Interface tab above for more details on the functionality of the software.
The system is available in 4 wavelength ranges: UV 200-1100 nm, VIS 400-1100 nm, IR 700-1800 nm, and IR 1000-2700 nm. Additionally, two slit and aperture sizes are offered: BP104 models have a physical aperture diameter of 4 mm and can accommodate beam diameters as small as 10 µm (1/e2), while BP109 models have a physical aperture diameter of 9 mm and accommodate beam diameters as small as 20 µm (1/e2). The operating principles are detailed on the tab provided above and labeled "Operation."
A variable scan rate of up to 20 Hz allows for real time optical system alignment. Both beam parameters and spatial power distribution can be monitored in dynamically changing systems. To obtain absolute optical power measurements, the user can perform a calibration using the integrated power meter and software and applying a calibration measurement at the wavelength of interest.
The Beam Profiler can work directly with a connected PC with no additional hardware or power supply required. For ease of use, Thorlabs utilizes a Hi-Speed USB2.0 interface to connect the measurement head with user supplied PC. Flexible data export options and the readout option via TCP/IP to standart data socket servers ease the integration into customized data processing environments.
Pulsed Laser Beams
The beam profile of pulsed laser sources with repetition rates of 10 Hz or higher and of any pulse widths can be measured. Several scans of the XY slit pairs are used to reconstruct the complete beam shape. Synchronization is done by manually adjusting the scanning speed to very close to an integer fraction of the laser’s repetition frequency. See Operations Manual for a detailed description. For M² measurements the minimum pulse repetition rate is >= 300 kHz.
Each Beamprofiler comes with the following parts:
BP100 Series Profiler Head
USB 2.0 Connection Cable, 2 m
Beam Profiler Software CD ROM with GUI software package and LabVIEW™ and LabWINDOWS™ /CVI Driver Set
Printed Operation Manual
Item #
BP104-UV
BP104-VIS
BP104-IR
BP104-IR2
BP109-UV
BP109-VIS
BP109-IR
BP109-IR2
Sensor
Wavelength Range (nm)
200 - 1100
400 - 1100
700 - 1800
1000 - 2700
200 - 1100
400 - 1100
700 - 1800
1000 - 2700
Detector Type
Si - UV Enhanced
Si
Ge
Extended InGaAs
Si - UV Enhanced
Si
Ge
Extended InGaAs
Aperture Diameter
4 mm
9 mm
Scan Method
Scanning Slits
Slit Size
2.5 µm
5 µm
Min Beam Diameter
10 µm
20 µm
Max Beam Diameter
4 mm
9 mm*
Scan Rate
1.0 - 20.0 per s (continuously variable)
Sampling Resolution
0.5 - 38 µm (depending on scan rate)
1.1 - 38 µm (depending on scan rate)
Power Range
10 nW - 10 W (depending on beam diameter and model)
Amplifier Bandwidth
10 to 150 kHz in 10 kHz Steps (@ -1 dB)
Sample Frequency
0.0625 - 1.0 MHz
Dynamic Range
72 dB (Amplifier Switchable)
Signal Digitization
16 bit
Head Size
Ø 80 mm x 60 mm (including rotation mount)
Minimum Pulse Rate
10 Hz (300 kHz if using the M² Option)
Software
Displayed Parameters/Features
X-Y-Profile, Centroid Position, Peak Position, Pseudo 3D Profile, Beam Width Clip Level/Second Moment (4σ), Gaussian Fit Applicable, Colored Pass/Fail Test
Compliant to Norm
ISO 11146 (Beam Widths, Divergence Angle and Beam Propagation Factor)
General System Requirements
Windows™ 2000/XP/Vista or later, USB2.0 port recommended, 120 MB HD, 512 MB RAM
* BP109-UV, -VIS, -IR: beam diameter error <10% at 9 mm beam diameter, BP109-IR2: beam diameter error <20% at 9 mm beam diameter for beam divergence <5° ** Using one of the M² Options
The upper limit on optical power with respect to the instruments' saturation level is related to the intensity (power per unit area). Therefore, the maximum power acceptable to the device is dependent on the width of the beam being measured. As depicted below, the measurable power range depends on both the model used (slit size and sensor type) as well as the width of the beam measured.
The graph shows the power ranges, indicated on the vertical axis of the graph that can be measured as a function of the specific model number (four colored lines), and the 1/e² beam width indicated on the horizontal axis of the graph.
Please note that the maximum average power needs to be limited to below 1W to prevent thermally damaging the measurement head. Levels up to 10W are acceptable for short term analysis only.
BP100 Series Operating Ranges
With the included GUI software, one can view the measurement results as either 3D, 2D, or single axis (X or Y) beam shapes. In addition, the beam profiler also extracts and displays: X & Y peak power and peak position, X & Y centroid position and beam width (at variable clip level), and total power and beam ellipticity. Each of the latter can be presented numerically or in a bar graph display.
BP100 Beam Profiler Series Graphical User Interface: Pseudo 3D Beam Profile
BP100 Beam Profiler Series Graphical User Interface: Separate X- and Y- Axis 2D-Profile with Gaussian Fit
Our BP100 Beam Profiler series is based on a scanning slit technology.
A narrow slit scans the beam at two defined orthogonal directions. This method allows a wide range of power and beam diameters to be analyzed without the need of attenuators or lenses.
To determine the beam's quality and spatial characteristics, the passing light is sampled by the detector in two directions and the overall power distribution is calculated. From the resulting power distributions in the X and Y directions, appropriate beam characteristics are analyzed. These parameters include: beam diameter, ellipticity, centroid location, 3D profile and the beam power distribution. These parameters, as well as the 2D and 3 -plots, and a Gaussian fit of the scanned profiles are then displayed.
The direction of X and Y is manually set by a rotation mount. A variable average function provides adjustable noise reduction and increases the measurement accuracy. The maximum-hold function allows analysis of pulsed laser sources, while the automatic or manual gain control enables the user to adapt to different beam powers. The power meter readouts in mW or dBm can be calibrated by the user. The provided GUI shows all parameters as digital or bar graph readouts, and parameter drifts can be visualized by a trend indicator. All resulting data can be exported as text or spreadsheet files.
Rotation mount The rotation mount is essential for measurement of the beam's ellipticity. For example, since the major and minor axis of an elliptical beam may have arbitrary position in space, the scan axes of the Beam Profiler needs to be oriented to these axes in order to measure the real ellipticity. Without scan axes alignment, the Beam Profiler will measure erroneous beam ellipticities. The BP104/BP109 Beam Profiler is an external optical beam measurement sensor and was designed for applications with an open beam.
The BP104/BP109 comes with a rotation mount, which enables you to rotate the scan axis X and Y up to +/- 60° manually. Simply take the plug on the top and move it to the left or right (while keeping the mount fixed); the Beam Profiler rotates within its mount. To get the desired angle, use the short markers set every 10° and the long markers set at 0° and 45° on the rotation mount in order to measure your beam profile at different directions easily.
The available software is organized into the following categories:
Applications: Standard application software packages and graphical user interfaces. This is what most users need to operate the device for typical applications.
Drivers: Instrument drivers for the National Instruments™, LabWindows™/CVI and LabVIEW™ development environments. These are intended for developers who want to extend or adapt the functionality of the device to their special requirements.
Loading...
Posted Comments:
Poster: klee
Posted Date: 2009-12-14 16:37:36.0
A response from Ken at Thorlabs to aditya.suresh: The beam profiler itself does not measure the M2 values. You should take a look at our Complete M2 Analysis Sets (M2SET-VIS or M2SET-IR) instead. You can click on the "Beam Quality Analyzer" under the Related Products above.
Poster: aditya.suresh
Posted Date: 2009-12-10 18:31:48.0
can you let us know if we can use this system to measure M2 values for beam outputs from a fibre?
Thanks,
A
Poster: kenlee
Posted Date: 2009-12-10 11:58:30.0
A response from Juergen from Thorlabs to bear020121212:
1) You ask, if rotation speed of the drum with slits is influencing the m² result? No, it should not, if the BP10x device settings were made correct. Please explain more detailed, why you are asking that.
2)No, in the SW you can observe either 2D profiles (in real time) or you can watch the virtual (calculated) 3D profile - a slit scanning beam profiler cannot deliver a genuine 3D profile, becaúse the slits are scanning the beam under +45° and -45° angle simultaneously.
Poster: bear020121212
Posted Date: 2009-12-10 10:13:51.0
Is the rotating of slit influence the measurement result of the M square factor of the laser? Could I use this beam profile to observe the 3D or 2D beam distribution simultaneously?
Poster: jhartmann
Posted Date: 2009-11-12 17:46:20.0
A response from Juergen from Thorlabs to c.j.lee:
The BP10X beam profilers are based on a rotating drum with scanning slits. The source of electrical signal is a photodiode, locate behind the slits inside the drum.
As for this, X and Y 2D profiles are real time profiles, as they represent the photodiode current vs. time. The X and Y scans can be saved, which make sense of course only for Gaussian or close to Gaussian beam profiles.
A beam profile in 3D in this case can be calculated only, its not a real picture, but just a virtual image - this is the reason why 3D profile cannot be exported as a number or array of data: There is only 1 value changing in time, and this time is formed by human eye to a consistent picture while its actually only a sequence of dots. Analogy: old CRT TV images...
"quite messy beams" is clearly NOT a suitable application for any scanning slit beam profiler (not only made by Thorlabs). We offer a camera beam profiler, where the beam profile is represented in a real 3D picture, based on a CCD camera - pixel coordinate and its intensity.
The item # is BC106-VIS or -UV. Unfortunately, there is no IR version available due to a lack of IR sensitive CCD image sensors (Si is becoming transparent above 1000nm)
So, in order to resolve your issue, Id like to ask you about details on your laser:
- type of laser
- CW or pulsed?
- wavelength
- power?
- beam diameter?
- expected beam shape?
- what beam parameters you want to characterize?
Poster: c.j.lee
Posted Date: 2009-11-12 09:27:43.0
We have already purchased the IR version of the beam profiler, but the software has disappointed us somewhat. It appears to be impossible to extract a complete image as an array of values (or as an image, for that matter) from the program. Instead, the program produces a screen shot of the window.
I have read the manual and found nothing that looks appropriate. That is, to put it mildly, absolutely pathetic for any use other than generating publicity for Thorlabs.
It is especially useless if you are dealing with beams that are quite messy, because you cannot adequately control how the beam parameters are analyzed and the x-y center cuts might not be appropriate.
Is there someway to extract this data? Other than to cut out the appropriate part of each screen shot and run them through an image analysis program?
Poster: jens
Posted Date: 2009-06-02 20:27:02.0
A reply from Jens at Thorlabs: the issue here is that your repetition rate is in the same range as the drum scanning frequency. The example in the manual describes repetition rates of the light srouce in the kHz range. With that the drum will see several pulses while it is scanning which will allow it to calculate the beam shape. In your case a CCD based profiler will be the better option. I will contact you directly to discuss next steps and ask our development to add more details regarding the lower limit repition rate to the manual.
Poster: stcpe
Posted Date: 2009-06-02 10:22:11.0
Please, advise, how to synchronize BP109-UV with 10 Hz 18 ns laser. Reading users manual doesnt help, as its imposible to reach necessary parameters using provided software.
Poster: Tyler
Posted Date: 2009-04-13 14:46:46.0
A response from Tyler at Thorlabs to lok.eg: The beam profiler can be used to measure 60 fs pulses for repetition rates above 10 Hz. The damage threshold is dependent on the beam diameter. Because of the short pulse duration, the amplifier will only be sensitive to the average power of the beam, which should be kept below 1 W. Please see the specs tab for how the operating power range is dependent on the beam diameter. Thank you for considering the BP109-UV beam expander. As an alternative you may wish to consider our camera based beam profiler (BC106-UV).
Poster: lok.eg
Posted Date: 2009-04-03 05:11:13.0
Is it possible to use BP109-UV with 60 fs pulses? (10 Hz or single pulse; 266, 400, 800 nm; 4 mm) Whats the highest power allowed then?