Hamamatsu C5965-31 Photonic multichannel spectral analyzer model: pma-11 Datasheet

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 multichannel photodetector are rigidly fixed, resulting in
excellent wavelength reproducibility. The wavelength
axis and spectral response characteristics are calibrated 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.
● Compact Integration of
a Spectrograph and Multichannel Photodetector
● High Sensitivity
● Easy Measurement Using
Optical Fiber Input
PMA-11 Standard Configuration
Main unit
HAMAMATSU
C7473
SIGNAL INPUT
Light source
SCSI
POWER
Fiber input optics
Microscope
attachment
Basic software
C5965
(MOS linear image sensor model)
C5966
(CCD image sensor model)
C7473
(BT- CCD image sensor model)
C8147
(InGaAs linear image sensor model)
Personal computer
[Standard Configuration]
1
1
1
Main unit
Fiber input optics
Basic software
Microscope
* SCSI cable not included
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
● 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.
● Superb cost perfomance model : C5965
The C5965 uses a MOS linear image sensor realises high performance and
low cost.
● High sensitivity model : C5966
The C5699 uses the CCD leaner image sensor has sensitivity a hundred
times better than the C5965 model.
● 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 CzernyTurner 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.
● 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.
● High efficiency optics
Adoption of a ø 1mm bundle fiber and a bright spectrograph detects a
measured light efficiently.
● Compact design
High performance is built in a small case. This completely new design
ensures that the PMA-11 will fit anywhere.
● External synchronisation can be used
Measurements can now be carried out synchronised to external trigger
signals, allowing measurement of pulse phenomena.
● Standard SCSI interface allows connection to computer
APPLICATIONS
[ Scientific applications ]
● UV to visible spectroscopy
● Fluorescence spectroscopy
● Raman scattering
● Chemiluminescence analysis
● Liquid chromatography
[ Industrial applications ]
● Gas chromatography
● ICP emission analysis
● Discharge emission analysis
● Combustion analysis
● Micro spectroscopy
● Water quality testing
● Evaluation of light sources
● Chromaticity measurements
● Impurities testing
● Thin film thickness monitors
● UV-ray monitors
● Plasma monitors
● Fruit tester
● Plastic sorting
● Color filter testing
MEASUREMENT EXAMPLES
Relative Intensity
2.0
Optical Density
1.5
1.0
0.5
0.0
0
450
300
600
Wavelength (nm)
750
900
500
700
600
Wavelength (nm)
800
900
2Absorption spectrum of a didymium filter
1Luminescence spectrum of a deuterium lamp
Angle of field
: 2˚
0.8
Relative Intensity
Tristimulus value
X : 58.25
Y : 100.00
Z :
0.96
Chromaticity coordinates
x : 0.3659
y : 0.6281
0.6
[y]
Dominant wavelength
: 559.04 nm
Excitation purity
: 98.97%
0.4
0
450
300
600
Wavelength (nm)
750
0.2
900
3Luminescence spectrum of an LED
0.00.
0.00
0.15
0.30
0.45
0.60
[x]
Relative Intensity
4Chromaticity coordinates of an LED
0
450
300
600
Wavelength (nm)
750
900
63-d display of plasma emission spectra
5Fluorescence spectrum of fluorosein
100
90
Transmittance (%)
Transmittance (%)
75
80
70
50
25
60
900
1050
1200
1350
Wavelength (nm)
1500
7Transmittance spectra in near infrared reagion
Dotted line: Compact disc
Solid line: PET botle
1650
0
900
1050
1200
1350
Wavelength (nm)
1500
8Transmittance spectra in near infrared reagion
Dotted line : Styren monomer
Solid line : Polystyren
1650
SPECIFICATIONS
● Main unit
Type No.
Photodetector
C5965-31
C5966-3x
C7473-36
MOS linear image sensor
CCD linear image sensor
BT- CCD linear image sensor
No. of photosensitive device channels
1024 ch
Cooling temepareture
512 electrons/scan( at 0˚C; 20ms )
-10˚C
0˚C
10 electrons
12,500 electrons
75 electrons/scan ( at -15˚C; 20ms )
A/D resolution
20,000 electrons/scan ( at 0˚C; 5ms )
2.5 × 107 electrons/scan ( at -10˚C; 5ms )
16bit
Spectrograph F number
3
Spectrograph type
4
Concave spherical grating type
Simultaneous measurement
wavelength range
300 nm to 800nm
x=1 300 nm to 800 nm
x=2 200 nm to 400 nm
x=3 600 nm to 1000nm
< 3 nm(FWHM)
x=1 < 3 nm(FWHM)
x=2 < 1.5 nm(FWHM)
x=3 < 2.5 nm(FWHM)
Wavelength resolution *
Czerny-Turner type
200 nm to 950 nm
1600 nm to 2350 nm
900 nm to 1650 nm
< 2 nm(FWHM)
Effective Light-receiving area of optical fiber
< 9 nm(FWHM)
< 9 nm(FWHM)
1mm
Optical fiber length
1.5m
Exposure time
20ms to 32s
5 ms to 50 ms (typ.)
5 ms to 32 s
External trigger input
TTL level / High impedance
Interface
SCSI
AC100V to 240V ±10%, 50, 60Hz
Line voltage
*Tested by the bright-line spectrum of Hg-Ar lamp
(at 312.57nm, 435.84nm, 546.07nm, 696.54nm, 1013.98nm)
● Basic software
Measurement
functions
50 µm(H) × 250 µm (V)
-15˚C
60 electrons
12,500 electrons/scan ( at 25˚C; 20ms )
256 ch
24 µm(H) × 2.928 mm(V)
0˚C
10 000 electrons
InGaAs linear image sensor
1024 ch
24µm (H) × 3.07 mm(V)
non-cooling
Read-out noise
Dark current
1024 ch
25 µm(H) × 2.5 mm (V)
Channel size
C8147-38
C8147-34
•
•
•
•
Spectral measurement
Reflection spectra measurement
Absorption spectra measurement
Color measurement
DIMENSIONAL OUTLINES (Unit :mm)
● C5965. C5966 (approx. 4.5kg)
PMA-11
PHOTONIC MULTI-CHANNEL ANALYZER
Display functions
• Spectrum (non-limited accumulation)
• Temporal fluctuation of waveform over time
(non-limited accumulation)
• Chromaticity diagram
Wavelength axis display
• Wavelength (nm) ,Wavenumber (cm -1),
Energy (eV)
Brightness axis display
• Linear, logarithm
3±0.5
40±1
260±1
333±1
● C7473 (approx. 5kg)
C7473
PHOTONIC MULTI-CHANNEL ANALYZER
SIGNAL INPUT
98.5±1
Calibration and
correction
• Wavelength axis
• Sensitivity uniformity
• Dark current
170±1
232±1
POWER
6±1
• Exposure time
• Memory integration count times
• Temporal fluctuation measurement
200±1
325±1
3±0.5
262±1
25±1
383±1
● C8147 (approx. 7.5kg)
PMA-11
PHOTONIC MULTI-CHANNEL ANALYZER
123.5±1
Data acquisition
condition setting
POWER
6±1
Temporal resolution
measurement functions
98.5±1
SIGNAL INPUT
• Temporal fluctuation of spectra over time
• Temporal fluctuation of reflection factor and
transmittance over time
SIGNAL INPUT
Wavelength (Wavenumber etc.) vs, intensity
Peak detection
FWHM between two cursors
Integrated intensity
375±1
3±0.5
262±1
25±1
433±1
● Fiber input optics (approx.100g)
C1
PVC sheathed SUS
flexible tube ( 7)
3
0.2
• Smoothing
• Differential waveform
• Color measurement
200±1
+0
10-0.1
Other analytical
functions
•
•
•
•
+0
12-0.1
Cursor analysis
functions
6±1
POWER
Bundle diameter 1.0
15 strands
80
50
ISO 9001
Certificate: 09 105 79045
1500
★ Product and software package names noted in this documentation are trademarks or registered trademarks of their respective manufacturers.
●
●
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:[email protected]
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: [email protected]
Germany: Hamamatsu Photonics Deutschland GmbH: Arzbergerstr. 10, D-82211 Herrsching am Ammersee, Germany, Telephone: (49)8152-375-0, Fax: (49)8152-2658,, E-mail: [email protected]
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: [email protected]
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: [email protected]
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:
[email protected]
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: [email protected]
JUL /2002 HPK
Created in Japan (PDF)
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