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USB Optical Bench Options
What makes the USB spectrometers (USB2000+ and
USB4000) so special are the
options that allow you to configure the bench for your application. Our
Applications Scientists can help you choose the optimum components, or you
can follow this guide to choose an entrance aperture size, detector
accessories, filters, a grating and more. The diagram below shows how
light moves through the asymmetrical crossed Czerny-Turner optical bench,
which has no moving parts that can wear or break; all components specified
are fixed in place at the time of manufacture.

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1 |
SMA 905 Connector |
Light from a fiber
enters the optical bench through the SMA 905 Connector. The SMA 905
bulkhead provides a precise locus for the end of the optical fiber,
fixed slit, absorbance filter and fiber clad mode aperture.
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2 |
Fixed Entrance Slit
(specify slit size) |
Light passes through
the installed slit, which acts as the entrance aperture. Slits come in
various widths from 5 µm to 200 µm. The slit is fixed in the SMA 905
bulkhead to sit against the end of a fiber. |
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3 |
Longpass Absorbing Filter
(optional) |
If selected, an
absorbance filter is installed between the slit and the clad mode
aperture in the SMA 905 bulkhead. The filter is used to block second-
and third-order effects or to balance color. |
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4 |
Collimating Mirror
(specify standard or SAG+) |
The collimating mirror
is matched to the 0.22 numerical aperture of our optical fiber. Light
reflects from this mirror, as a collimated beam, toward the grating.
You can opt to install a standard mirror or a UV absorbing SAG+
mirror. |
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5 |
Grating & Wavelength
Range
(specify grating & starting wavelength) |
We install the grating
on a platform that we then rotate to select the starting wavelength
you’ve specified. Then we permanently fix the grating in place to
eliminate mechanical shifts or drift. |
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6 |
Focusing Mirror
(specify standard or SAG+) |
This mirror focuses
first-order spectra on the detector plane. Both the collimating and
focusing mirrors are made in-house to guarantee the highest
reflectance and the lowest stray light possible. You can opt to
install a standard or SAG+ mirror. |
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7 |
L2 & L4 Detector Collection
Lenses
(optional) |
One of these cylindrical lenses,
made in-house to ensure aberration-free performance, is fixed to the
detector to focus the light from the tall slit onto the shorter
detector elements. It increases light-collection efficiency. The L2 is
for the USB2000+; the L4 is for the USB4000. |
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8 |
Detector |
For the USB2000+ we
offer the 2048-element Sony ILX511 linear CCD array detector.
For the USB4000, we offer the 3648-element
Toshiba TCD1304AP linear CCD array detector.
Each pixel responds to
the wavelength of light that strikes it. Electronics bring the
complete spectrum to the software. |
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9 |
OFLV Variable Longpass
Order-sorting Filter
(optional) |
Our proprietary filters
precisely block second- and third-order light from reaching specific
detector elements. |
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10 |
UV2 & UV4
Detector Upgrades
(optional) |
When selected, the
detector’s standard BK7 window is replaced with a quartz window to
enhance the performance of the spectrometer for applications <340 nm.
The UV2 is for the USB2000+; the UV4 is for the USB4000. |
A precision SMA 905 Connector aligns to the
spectrometer’s entrance slit and ensures concentricity of the fiber. For
an upgrade fee that includes the cost of the custom connector and labor,
we will replace the standard SMA 905 Connector with a different connector
of your choice. We also offer connector adapters, such as an SMA-to-ST
Adapter and an SMA-to-FC Adapter. Please call for details on custom
connectors and adapters.
Another option available with a USB4000 user-configured
spectrometer is the size of the entrance aperture. Entrance slits are
rectangular apertures, 1-mm tall and various widths from 5 µm to 200 µm,
with the width determining the amount of light entering the bench. Note
that the smallest slit achieves the best optical resolution. (For more on
how your slit choice affects optical resolution,
click
here.) A slit is permanent; it only can be changed by our technicians.
You can opt against having a slit, in which case the diameter of the fiber
connected to the spectrometer determines the size of the entrance
aperture.
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Slit |
Description |
Pixel Resolution |
Price |
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SLIT-5 |
5-µm wide x 1-mm high |
~5.3 pixels |
$174 |
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SLIT-10 |
10-µm wide x 1-mm high |
~5.7 pixels |
$174 |
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SLIT-25 |
25-µm wide x 1-mm high |
~7.5 pixels |
$174 |
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SLIT-50 |
50-µm wide x 1-mm high |
~11.6 pixels |
$174 |
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SLIT-100 |
100-µm wide x 1-mm high |
~21 pixels |
$174 |
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SLIT-200 |
200-µm wide x 1-mm high |
~42 pixels |
$174 |
We offer longpass absorbing or blocking
filters; each filter has a transmission band and a blocking band to
restrict radiation to a certain wavelength region for eliminating second-
and third-order effects. These filters are installed permanently between
the slit and the clad mode aperture in the bulkhead of the SMA 905
Connector.
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Item |
Description |
Price |
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OF1-WG305 |
Longpass filter; transmits light >305 nm |
$81 |
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OF1-GG375 |
Longpass filter; transmits light >375 nm |
$59 |
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OF1-GG475 |
Longpass filter; transmits light >475 nm |
$59 |
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OF1-OG515 |
Longpass filter; transmits light >515 nm |
$59 |
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OF1-OG550 |
Longpass filter; transmits light >550 nm |
$59 |
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OF1-OG590 |
Longpass filter: transmits light >590 nm |
$59 |
You can replace standard aluminum-coated
reflective mirrors with our proprietary, UV-absorbing SAG+ Mirrors, which
increase reflectance in the VIS-NIR and, in turn, increase the sensitivity
of the spectrometer. SAG+ Mirrors are often specified for fluorescence.
These mirrors also absorb nearly all UV light, which reduces the effects
of excitation scattering in fluorescence measurements. Unlike typical
silver-coated mirrors, the SAG+ mirrors won't oxidize. They have excellent
reflectivity -- more than 95% across the VIS-NIR. The price of the SAG+UPG
is $290.
You choose from among 14 gratings for each
spectrometer. With each grating, you consider its groove density (which
helps determine the resolution), its spectral range (which helps determine
the wavelength range) and its blaze wavelength (which helps determine the
most efficient range). Click here for your Grating & Wavelength Choices.
Predicted Ranges &
Resolutions
See a series of graphs to demonstrate the
predicted Range and Resolution of
your USB2000+ or USB4000 Spectrometer.
At right is a detector with the L4 lens. This
cylindrical lens, made in-house to ensure aberration-free performance, is fixed
to the detector’s window to focus the light from the tall slit onto the shorter
detector elements. It increases light-collection efficiency and reduces stray
light. It also is useful in a configuration with a large-diameter fiber for low
light-level applications. An L2 or L4 Detector Collection Lens is
$174.
The USB2000+ utilizes the
Sony ILX511
linear silicon CCD array detector. Our next-generation USB4000
Spectrometer utilizes the
Toshiba TCD1304AP linear CCD array detector, which has some electronic
advances over the Sony, such as a user-programmable microcontroller. Both
are linear silicon CCD arrays, with an effective range of 200-1100 nm, and
with the same dynamic range (1300:1). There are some differences between
the detectors. For example, the Toshiba detector achieves better optical
resolution. Also, on a per-unit area basis, the sensitivity is about the
same. Because the Toshiba detector has an electronic shutter, you can
almost never have too much light; the shutter prevents the detector from
saturating, making possible analysis of transient events such as laser
pulses.
Our OFLV Variable Longpass Order-sorting Filters are
applied to the detector’s window to eliminate second- and third-order effects.
We use patented coating technology to apply the filter onto the substrate. In
fact, we are the only miniature spectrometer manufacturer to offer “clean”
first-order spectra. There are two OFLV Filter options available for the USB4000
Optical Bench -- the DET4-350-1000 and DET4-200-850 Detectors.
When you specify a detector with the UV2 or UV4 Detector Window Upgrade, we replace the
detector’s standard BK7 window with a quartz window to enhance the
spectrometer‘s performance from 200-340 nm. The UV2 is available in the USB2000+
Optical Bench with the DET2-UV Detector. The UV4 is available in the USB4000
Optical Bench with the DET4-UV and DET4-200-850 Detectors.
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Detector |
Description |
Spectrometer |
Detector
Price |
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DET2-VIS |
Sony ILX511 Detector installed into an
USB2000+ User-Configured Spectrometer; best for systems
with wavelength ranges above 400 nm. |
USB2000+ |
$0 |
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DET2-UV |
Sony ILX511 Detector with UV2 Detector Window
Upgrade installed into an HR2000+ User-Configured
Spectrometer; best for systems with wavelength ranges in
the UV |
USB2000+ |
$174
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DET4-VIS |
Toshiba TCD1304AP Detector installed into a
USB4000 User-Configured Spectrometer; best for systems with
wavelength ranges above 400 nm |
USB4000 |
$0
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DET4-UV |
Toshiba TCD1304AP Detector with UV4 Detector
Window Upgrade installed into a USB4000 User-Configured
Spectrometer; best for systems with wavelength ranges in the
UV |
USB4000 |
$174
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DET4-350-1000 |
Toshiba TCD1304AP Detector with OFLV-350-1000
Variable Longpass Order-sorting Filter installed into a
USB4000 User-Configured Spectrometer; best when using
Grating #2, #3 or #4 |
USB4000 |
$220
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DET4-200-850 |
Toshiba TCD1304AP Detector with UV4 Detector
Window Upgrade and OFLV-200-850 Variable Longpass Order-sorting Filter installed into a USB4000 Spectrometer;
best when using Grating #1 or #2 |
USB4000 |
$347
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Detector Specifications
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Specification |
Sony Detector |
Toshiba Detector |
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Detector:
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Sony ILX511B linear silicon CCD array |
Toshiba TCD1304AP
Linear CCD array |
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Detector range: |
200-1100 nm |
200-1100 nm |
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Pixels:
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2048 pixels |
3648 pixels |
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Pixel size:
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14 µm x 200 µm |
8 μm x 200 μm |
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Pixel well depth:
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~62,500 electrons |
100,000 electrons |
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Signal-to-noise ratio: |
250:1 (at full signal) |
300:1 (at full signal) |
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A/D resolution: |
16 bit |
16 bit |
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Dark noise: |
2.5 RMS counts |
50 RMS counts |
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Corrected linearity: |
>99.8% |
>99.8% |
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Sensitivity: |
75 photons/count at 400 nm;
41 photons/count
at 600 nm |
130 photons/count at 400 nm; 60
photons/count at 600 nm |
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