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R1463P中文资料

R1463P中文资料
R1463P中文资料

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 are subject to change without notice. No patent rights are granted to any of the circuits described herein. ? 1998 Hamamatsu Photonics K.K.

Figure 1: Typical Spectral Response

PHOTOMULTIPLIER TUBES R1463, R1463P

CHARACTERISTICS (at 25°C)

Parameter

Min.Unit Cathode Sensitivity

Anode Sensitivity D

Gain D

Anode Dark Current D (After 30 minute storage in the darkness)

Anode Dark Count D (After 3 hour storage in the darkness) (for R1463P)

Time Response

μA/lm mA/W mA/W %—A/lm A/W A/W —nA cps ns ns

80———0.1530———————

————————201000——

Max.Typ.1205119190.21205.1 × 1041.9 × 1041 × 106

49002.524

Luminous B

Radiant at 420nm at 633nm

Quantum Efficiency at 290nm Red/White Ratio C Luminous E

Radiant at 420nm at 633nm

Anode Pulse Rise Time D, F

Electron Transit Time D,G

NOTES

A:Averaged over any interval of 30 seconds maximum.

B:The light source is a tungsten filament lamp operated at a distribution temperature of 2856K. The light input is 10-3 lumen. Supply voltage is 150 volts

between the cathode and all other electrodes connected together as anode.

C:Red/White Ratio is the quotient of the cathode current measured using a red filter (Toshiba R-68) interposed between the light source and the tube by the

cathode current measured with the filter removed under the same conditions as Note B.

D: Measured with the anode-to-cathode supply voltage and voltage distribution ratio shown in Table 1.E: The light input is 10-8 lumens with the same light source as Note B.

F: The rise time is the time for the output pulse to rise from 10% to 90% of the peak amplitude when the entire photocathode is illuminated by a delta function

light pulse.

G: The electron transit time is the interval between the arrival of a delta function light pulse at the entrance window of the tube and the time the output pulse

reaches the peak amplitude. In measurement the entire photocathode is illuminated.

Supply Voltage: 1000Vdc, K: Cathode, Dy: Dynode, P: Anode

Table 1: VOLTAGE DISTRIBUTION RATIO

Electrodes Distribution Ratio K Dy11Dy21Dy31Dy41Dy51Dy61Dy71Dy81Dy91

11Dy10P

100

10

1

0.1

0.01

WAVELENGTH (nm)C A T H O D E R A D I A N T S E N S I T I V I T Y (m A /W )Q U A N T U M E F F I C I E N C Y (%)

Figure 2: Anode Sensitivity and Gain Characteristics

104

103102

10110010-110-2

108

107

106

105

104

103

102SUPPLY VOLTAGE (V)

A N O D E L U M I N O U S S E N S I T I V I T Y (A /l m )

G A I N

Figure 3: Typical Time Response

TPMHB0532EA

Figure 4: Typical Temperature Coefficient of Anode Sensitivity

TPMHB0533EA

200

100806040

20

10864

2

1

SUPPLY VOLTAGE (V)

T I M E (n s )

+1.5

+1.0

+0.5

-1.0

-0.5

-1.5

200400600800

WAVELENGTH (nm)

T E M P E R A T U R E C O E F F I C I E N T (%/°C )

Figure 5: Typical Temperature Characteristic of Dark Current and Dark Counts (R1463P)

TPMHB0534EA

Figure 6: Typical Single Photoelectron Pulse Height Distribution (R1463P)

TPMHB0535EA

100

1010.1

0.01

10000

1000

100

10

1

TEMPERATURE (°C)

A N O D E D A R K C U R R E N T (n A )

A N O D E D A R K C O U N T (c p s )

0.3m m 2m 3m

PULSE HEIGHT

C O U N T R A T E (C o u n t s /C h a n n e l )

INCIDENT LIGHT : 600nm TEMPERATURE : 25°C SUPPLY VOLTAGE: 1500V

SIGNAL + NOISE = Σ = 8100cps NOISE = Σ = 900cps

Σ (Count) = Σ (Count)M is defined to satisfy the

following equation

m 0.3m

0.3m

3m 3m

m

3m

0.3m

TPMH1216E01AUG. 1998

HAMAMATSU PHOTONICS K.K., Electoron Tube Center

314-5, Shimokanzo, Toyooka-village, Iwata-gun, Shizuoka-ken, 438-0193, Japan, Telephone: (81)539/62-5248, Fax: (81)539/62-2205

U.S.A.: Hamamatsu Corporation: 360 Foothill Road, P. O. Box 6910, Bridgewater. N.J. 08807-0910, U.S.A., Telephone: (1)908-231-0960, Fax: (1)908-231-1218

Germany: Hamamatsu Photonics Deutschland GmbH: Arzbergerstr. 10, D-82211 Herrsching am Ammersee, Germany, Telephone: (49)8152-375-0, Fax: (49)8152-2658

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

United Kingdom: Hamamatsu Photonics UK Limited: Lough Point, 2 Gladbeck Way, Windmill Hill, Enfield, Middlesex EN2 7JA, United Kingdom, Telephone: (44)181-367-3560, Fax: (44)181-367-6384North Europe: Hamamatsu Photonics Norden AB: F?r?gatan 7, S-164-40 Kista Sweden, Telephone: (46)8-703-29-50, Fax: (46)8-750-58-95

Italy: Hamamatsu Photonics Italia: S.R.L.: Strada della Moia, 1/E, 20020 Arese, (Milano), Italy, Telephone: (39)02-935 81 733, Fax: (39)02-935 81 741

TACCA0005EA

TPMHA0014EA

TACCA0022EA

TACCA0021EA

TPMHA0435EA

Figure 7: Dimensional Outline and Basing Diagram (Unit: mm)

Figure 8: Optional Socket Assembly E849-34 and E849-35 (Unit: mm)

PHOTOMULTIPLIER TUBES R1463, R1463P

Socket (E678-13A)

DY4SHORT PIN

R1463

R1463P

E849-34

E849-35

The E849-34 and E849-35 are socket assemblies specifically designed for 1/2 inch diameter, 10 stage, head-on type photomultiplier tubes having a 13-pin glass base. It contains a voltage-divider network potted with silicone rubber, thus eliminating troublesome soldering for making up the divider network.

330k ?

R1 to R11 :SOCKET

: 330k ?: 0.01μF

Warning - Personal Safety Hazards Electrical Shock — Operating voltage applied to this device presents shock hazard.

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