Photonic Multichannel Spectral
Analyzer Model: PMA-11
The PMA-11 is a spectral analyzer that integrates a
spectrograph and high performance multi-channel
photodetector in a single compact chassis. Light
collection is simplified through the use of optical fiber.
The diffraction grating of the spectrograph and multi-
channel photodetector are rigidly fixed, resulting in
excellent wavelength reproducibility. The wavelength
axis and spectral response characteristics are cali-
brated at the factory, so that spectral measurements
can be carried out easily and accurately.
The PMA-11 series offers four different multi-channel
photo-detectors to choose from, for additional flexibility
in grating selection, allowing the user to optimize the
performance for the application at hand.
Equipped with a standard SCSI interface, the PMA-11
is easily connected to any type of computer for data
collection and analysis.
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Compact Integration of
a Spectrograph and Multi-
channel Photodetector
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High Sensitivity
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Easy Measurement Using
Optical Fiber Input
PMA-11 Standard Configuration
Main unit
HAMAMA
TSU
C7473
SIGNAL INPUT
SCSI
Light source
Fiber input optics
POWER
Microscope
attachment
C5965
(MOS linear image sensor model)
C5966
(CCD image sensor model)
C7473
(BT- CCD image sensor model)
C8147
(InGaAs linear image sensor model)
Basic software
Personal computer
[Standard Configuration]
Main unit
Fiber input optics
Basic software
* SCSI cable not included
Microscope
1
1
1
A compact unit containing a multi-channel photo-detector,and
power supply all in one.
Optical fiber input makes spectral measurements easier than ever.
FEATURES
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Measurements of the spectrum are easier and more
accurate than ever before
The spectrum can now be easily measured by light collection through an
optical fiber. The wavelength axis and spectral response characteristics are
calibrated at the factory, so that spectral measurements can be carried out
easily and accurately.
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Near infrared model : C8147-34, C8147-38
The C8147 realises a simultaneous and high-resolution measurement of
absorption or reflection spectra in a near infrared wavelength region with
a wide dynamic range and a low noise.
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High efficiency optics
Adoption of a
ø
1mm bundle fiber and a bright spectrograph detects a
measured light efficiently.
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Superb cost perfomance model : C5965
The C5965 uses a MOS linear image sensor realises high performance and
low cost.
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Compact design
High performance is built in a small case. This completely new design
ensures that the PMA-11 will fit anywhere.
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High sensitivity model : C5966
The C5699 uses the CCD leaner image sensor has sensitivity a hundred
times better than the C5965 model.
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External synchronisation can be used
Measurements can now be carried out synchronised to external trigger
signals, allowing measurement of pulse phenomena.
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Ultra-high sensitivity model : C7473-36
The C7473-36 consists the thermoelectric-cooling type BT-CCD image
sensors, which have a high quantum efficiency and a compact Czerny-
Turner type spectrograph. The simultaneous measurement of the wavelength
from an ultraviolet to a near-infrared region with high wavelength resolution
and high sensitivity is realised.
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Standard SCSI interface allows connection to computer
APPLICATIONS
[ Scientific applications ]
[ Industrial applications ]
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UV to visible spectroscopy
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Fluorescence spectroscopy
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Raman scattering
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Chemiluminescence
analysis
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Liquid chromatography
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Gas chromatography
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ICP emission analysis
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Discharge emission analysis
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Combustion analysis
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Micro spectroscopy
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Water quality testing
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Evaluation of light sources
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Chromaticity
measurements
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Impurities testing
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Thin film thickness monitors
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UV-ray monitors
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Plasma monitors
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Fruit tester
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Plastic sorting
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Color filter testing
MEASUREMENT EXAMPLES
2.0
Relative Intensity
Optical Density
0
300
450
600
Wavelength (nm)
750
900
1.5
1.0
0.5
0.0
500
700
600
Wavelength (nm)
800
900
1Luminescence
spectrum of a deuterium lamp
2Absorption
spectrum of a didymium filter
0.8
Angle of field
: 2˚
Tristimulus value
X : 58.25
Y : 100.00
Z :
0.96
Relative Intensity
0.6
Chromaticity coordinates
x : 0.3659
y : 0.6281
Dominant wavelength
: 559.04 nm
[y]
0.4
Excitation purity
: 98.97%
0
300
450
600
Wavelength (nm)
750
900
0.2
3Luminescence
spectrum of an LED
0.00.
0.00
0.15
0.30
[x]
0.45
0.60
4Chromaticity
coordinates of an LED
Relative Intensity
0
300
450
600
Wavelength (nm)
750
900
5Fluorescence
spectrum of fluorosein
63-d
display of plasma emission spectra
100
90
75
Transmittance (%)
80
Transmittance (%)
1050
1200
1350
Wavelength (nm)
1500
1650
50
70
25
60
900
0
900
1050
1200
1350
Wavelength (nm)
1500
1650
7Transmittance
spectra in near infrared reagion
Dotted line: Compact disc
Solid line: PET botle
8Transmittance
spectra in near infrared reagion
Dotted line : Styren monomer
Solid line : Polystyren
SPECIFICATIONS
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Main unit
Type No.
Photodetector
No. of photosensitive device channels
Channel size
Cooling temepareture
Read-out noise
Dark current
A/D resolution
Spectrograph F number
Spectrograph type
Simultaneous measurement
wavelength range
3
Concave spherical grating type
300 nm to 800nm
x=1 300 nm to 800 nm
x=2 200 nm to 400 nm
x=3 600 nm to 1000nm
x=1 < 3 nm(FWHM)
x=2 < 1.5 nm(FWHM)
x=3 < 2.5 nm(FWHM)
200 nm to 950 nm
C5965-31
MOS linear image sensor
1024 ch
25
µm(H) ×
2.5 mm (V)
non-cooling
10 000 electrons
12,500 electrons/scan ( at 25˚C; 20ms )
C5966-3x
CCD linear image sensor
1024 ch
24µm (H)
×
3.07 mm(V)
0˚C
60 electrons
512 electrons/scan( at 0˚C; 20ms )
C7473-36
BT- CCD linear image sensor
1024 ch
24
µm(H) ×
2.928 mm(V)
-15˚C
10 electrons
75 electrons/scan ( at -15˚C; 20ms )
16bit
4
Czerny-Turner type
900 nm to 1650 nm
1600 nm to 2350 nm
0˚C
12,500 electrons
20,000 electrons/scan ( at 0˚C; 5ms )
2.5
×
10
7
electrons/scan ( at -10˚C; 5ms )
C8147-34
InGaAs linear image sensor
256 ch
50
µm(H) ×
250
µm
(V)
-10˚C
C8147-38
Wavelength resolution
*
< 3 nm(FWHM)
Effective Light-receiving area of optical fiber
Optical fiber length
Exposure time
External trigger input
Interface
Line voltage
< 2 nm(FWHM)
1mm
1.5m
< 9 nm(FWHM)
< 9 nm(FWHM)
20ms to 32s
TTL level / High impedance
SCSI
AC100V to 240V
±
10%, 50, 60Hz
(at 312.57nm, 435.84nm, 546.07nm, 696.54nm, 1013.98nm)
5 ms to 32 s
5 ms to 50 ms (typ.)
*
Tested by the bright-line spectrum of Hg-Ar lamp
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Basic software
Measurement
functions
•
•
•
•
Spectral measurement
Reflection spectra measurement
Absorption spectra measurement
Color measurement
DIMENSIONAL OUTLINES (Unit :mm)
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C5965. C5966 (approx. 4.5kg)
PHOTONIC MULTI-CHANNEL ANALYZER
PMA-11
SIGNAL INPUT
Temporal resolution
measurement functions
Data acquisition
condition setting
Calibration and
correction
6±1
• Temporal fluctuation of spectra over time
• Temporal fluctuation of reflection factor and
transmittance over time
• Exposure time
• Memory integration count times
• Temporal fluctuation measurement
• Wavelength axis
• Sensitivity uniformity
• Dark current
• Spectrum (non-limited accumulation)
• Temporal fluctuation of waveform over time
(non-limited accumulation)
• Chromaticity diagram
• Wavelength (nm) ,Wavenumber (cm ),
Energy (eV)
• Linear, logarithm
-1
POWER
98.5±1
170±1
232±1
3±0.5
40±1
260±1
333±1
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C7473 (approx. 5kg)
PHOTONIC MULTI-CHANNEL ANALYZER
C7473
POWER
200±1
262±1
6±1
98.5±1
SIGNAL INPUT
325±1
3±0.5
25±1
383±1
Display functions
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C8147 (approx. 7.5kg)
PHOTONIC MULTI-CHANNEL ANALYZER
Wavelength axis display
Brightness axis display
Cursor analysis
functions
PMA-11
SIGNAL INPUT
POWER
•
•
•
•
Wavelength (Wavenumber etc.) vs, intensity
Peak detection
FWHM between two cursors
Integrated intensity
200±1
262±1
6±1
123.5±1
375±1
25±1
433±1
3±0.5
+0
12-0.1
+0
10-0.1
Other analytical
functions
• Smoothing
• Differential waveform
• Color measurement
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Fiber input optics (approx.100g)
PVC sheathed SUS
flexible tube ( 7)
C1
3
Bundle diameter 1.0
15 strands
80
1500
50
ISO 9001
Certificate: 09 105 79045
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Product and software package names noted in this documentation are trademarks or registered trademarks of their respective manufacturers.
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Subject to local technical requirements and regulations, availability of products included in this promotional material may vary. Please consult with our sales office.
.
Information furnished by HAMAMATSU is believed to be reliable. However, no responsibility is assumed for possible inaccuracies or omissions.
Specifications and external appearance are subject to change without notice.
.
© 2001Hamamatsu Photonics K.K.
Homepage Address http://www.hamamatsu.com
HAMAMATSU PHOTONICS K.K., Systems Division
812 Joko-cho, Hamamatsu City, 431-3196, Japan, Telephone: (81)53-431-0124, Fax: (81)53-435-1574, E-mail:export@sys.hpk.co.jp
U.S.A. and Canada:
Hamamatsu Photonic Systems: 360 Foothill Road, Bridgewater, N.J. 08807-0910, U.S.A., Telephone: (1)908-231-1116, Fax: (1)908-231-0852, E-mail: usa@hamamatsu.com
Germany:
Hamamatsu Photonics Deutschland GmbH: Arzbergerstr. 10, D-82211 Herrsching am Ammersee, Germany, Telephone: (49)8152-375-0, Fax: (49)8152-2658, E-mail: info@hamamatsu.de
,
France:
Hamamatsu Photonics France S.A.R.L.: 8, Rue du Saule Trapu, Parc du Moulin de Massy, 91882 Massy Cedex, France, Telephone: (33)1 69 53 71 00, Fax: (33)1 69 53 71 10, E-mail: infos@hamamatsu.fr
United Kingdom:
Hamamatsu Photonics UK Limited: 2 Howard Court, 10 Tewin Road, Welwyn Garden City, Hertfordshire, AL7 1BW, U.K., Telephone: (44) 1707-294888, Fax: (44) 1707-325777, E-mail: info@hamamatsu.co.uk
North Europe:
Hamamatsu Photonics Norden AB: Smidesvägen 12, SE-171-41 Solna, Sweden, Telephone: (46)8-509-031-00, Fax: (46)8-509-031-01, E-mail: info@hamamatsu.se
-
Cat. No. SSCS1040E07
Italy:
Hamamatsu Photonics Italia S.R.L.: Strada della Mois, 1/E 20020 Arese (Milano), Italy, Telephone: (39)02-935 81 733, Fax: (39)02-935 81 741, E-mail: info@hamamatsu.it
JUL /2002 HPK
Created in Japan (PDF)
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