L6566 HAMAMATSU [Hamamatsu Corporation], L6566 Datasheet - Page 5

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L6566

Manufacturer Part Number
L6566
Description
The best light source is supported by the best electrode technology
Manufacturer
HAMAMATSU [Hamamatsu Corporation]
Datasheet

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7
SPECIFICATIONS
HEATER VOLTAGE AND CURRENT
L2D2 Lamps
Extremely high stability of intensity is required for deuterium lamps because of their applications.
Therefore, use of a power supply designed to drive the lamps with stable operation is recommended.
Hamamatsu
a constant-voltage circuit in the filament power supply section to assure a reliable operation.
Hamamatsu offers not only OEM power supplies specially designed for your applications, as well as the following
types according to the operation mode of various lamps.
Control Methode
Input
Output
Ambient Temperature
Cooling
Dimensions (W × H × D)
Weight
Certification
C1518 (2.5 V)
C1518 (10 V)
C1518 (SQ2.5 V)
C1518 (SQ10 V)
C7860/M7628-2510
C7860/M7628-2517
C7860/M7628-3000
C7860/M7628-1035
C7860/M7628-1070
C7860/M7628-1555
NOTE A C7860 series are manufactured only when the order is placed.
* Characteristics are measured at 23±1 °C after 30 min of warming up.
POWER SUPPLY
Type No.
Anode
Heater
,
s power supply for deuterium lamps uses a constant-current circuit in the main power supply section and
Parameter
Input Voltage
Input Wattage
Output Voltage
Output Current
Trigger Voltage
Fluctuation (p-p)
Drift
Output Voltage
Output Current
Warm-up Time
A
A
A
A
(Deuterium Lamps )
C1518
Voltage (V dc)
2.5 ± 0.15
2.5 ± 0.15
15 ± 0.75
2.5 ± 0.2
2.5 ± 0.2
3 ± 0.15
10 ± 0.5
10 ± 0.5
10 ± 1
10 ± 1
With Load
Without Load
Warm-up
TLSOF0068
Current (A dc typ.)
(AC) 100/118/230 ±10 %
0.8
1.2
0.8
1.2
0.5
200 × 107 × 240
4
4
4
4
5
Dropper Type
Not required
See below
See below
(DC) 160
600 ± 50
(DC) 80
0 to +40
C1518
±0.1
100
300
0.1
6.7
20
Voltage (V dc)
1.0 ± 0.1
3.5 ± 0.5
1.7 ± 0.2
7.0 ± 0.5
1.7 ± 0.1
3.5 ± 0.2
5.5 ± 0.3
1 ± 0.05
7 ± 0.35
0
(AC) 90 to 115/180 to 250
C7860
Operation
113 × 122 × 220
Switching Type
Not required
(Automatic)
See below
See below
(DC) 160
600 ± 50
0 to +40
Current (A dc typ.)
(DC) 80
C7860
300
±0.1
0.5
2.7
60
25
TLSOF0150
1.8
0.3
3.3
1.8
3.3
0.3
0.3
1
0
1
20 CMF of forced air
L6565, L7293, L6999, L6999-50
L7307, L7174, L6301, L6302
L6307, L6308, L7292
L7298, L6303, L6304, L7306
L7296, L7295, L6309, L6310, L7296-50
L6565, L7293, L6999, L6999-50
L7307, L7174, L6301, L6302
L7298, L6303, L6304, L7306
L6566, L6305, L6306
L6307, L6308, L7292
L7296, L7295, L6309, L6310, L7296-50
L6311, L6311-50, L6312, L6312-50
100 × 118 × 36.2
Switching Type
(DC) 24 ± 2.4
See below
See below
(DC) 160
600 ± 50
(DC) 80
0 to +40
M7628
UL/CE
±0.1
0.17
300
48
0.5
25
Applicable Lamps
M7628
%/h Max.
VA Max.
V peak
% Max.
TLSOF0150
V Typ.
V Typ.
s Typ.
Unit
mA
mm
°C
kg
V
TECHNICAL INFORMATION
Deuterium lamps emit high intensity light in the UV range at wavelengths
shorter than 400 nm. Light intensity on the short wavelength side is deter-
mined by the window material used.
GSynthetic silica
The following 4 types of window material are available for deuterium lamps.
Figure 2 shows the transmittance of various window materials.
UV light at wavelengths shorter than 190 nm attenuates greatly due to its
absorption by oxygen. To obtain the fullest performance in window trans-
mittance, it is recommended that the inside of the equipment be filled with
nitrogen or vacuum-evacuated to eliminate this absorption effect.
GUV glass
UV glass has a higher ultraviolet transmittance than normal optical glass
(borosilicate glass). It has the longest cut off wavelength of 185 nm among
the four types. However the generation of ozone is lower than other wind-
ow material types, it is not necessary to have special anti-ozone treat-
ments.
Synthetic silica is obtained by fusing a silica crystal that is artificially
grown. Although its cut off wavelength is 160 nm, it contains less impuri-
ties than fused silica, and transmittance at 200 nm has been improved by
approx. 50 %.
GMgF
MgF
ultraviolet transmittance, a low deliquescence and is used as window
material for vacuum ultraviolet applications. Its cut off wavelength is 115
nm.
Figure 1: Spectral Distribution
Figure 2: Typical Transmittance of Various Window Materials
(1) UV glass
(3) MgF
Spectral Distribution
Window Material
2
is a crystallized form of alkali metal halide that has an excellent
2
2
0.01
0.05
0.5
0.1
160
100
TLSOB0024ED
80
60
40
20
100
TLSOB0038EC
(2) Synthetic silica
200
UV GLASS
150
240
WAVELENGTH (nm)
SYNTHETIC SILICA
(PROJECTING TYPE, 1 mm THICK)
WAVELENGTH (nm)
200
280
UV GLASS
SYNTHETIC SILICA
MgF
250
320
2
360
300
400
350
Figure 4: Directivity (Light Distribution)
15°
15°
Arc intensity is determined by the aperture (light exit) size. Figure 5
shows typical spectral distributions for lamps with different aperture sizes.
At the same input current and voltage, lamps with an aperture of 0.5 mm
diameter (high brightness type) provide 1.6 times higher brightness than
lamps with an aperture of 1.0 mm diameter (standard type). The half
width of spectral distribution also becomes narrower with a reduced aper-
ture size. When higher intensity is required or the object to be irradiated
is very small, the high brightness type is recommended.
The non-projecting type uses the side of the cylindrical glass bulb as the
emission window, whilst the projecting type uses a plane glass attached
to a projection on the bulb.
The projecting type has a uniformed transmittance due to the plane glass.
Since the window is located far from the discharge position, the amount
of dirt produced by spattering from the electrodes is reduced resulting in
low deterioration of light output. The non-projecting type requires less
space and has a wider directivity since there is no projection, enabling
effective use of emitted light. The long-nose projecting type uses an
MgF
type is used with the tip of the nose inserted into the vacuum equipment.
Figure 3: External View
0
Figure 5: Arc Distribution
30°
30°
Non-projecting type
Arc Distribution
Light Distribution
2
Non-projecting type
window and is suitable for vacuum ultraviolet applications. This
Y
APERTURE: 0.5 mm
(High Brightness Version)
TLSOB0021EA
0.5 mm
APERTURE
15°
15°
0
30°
30°
X
Projecting type
Projecting type
TLSOB0020EA
Y
APERTURE: 1.0 mm
(Standard Version)
Long-nose projecting type
1.0 mm
10°
10°
0
20°
20°
30°
30°
Projecting type
Long-nose
TLSOF0139
APERTURE
TLSOB0049EB
X
TLSOB0077EA
8

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