BPW20RF. Silicon PN Photodiode. Vishay Semiconductors. Description. Features. Applications. Absolute Maximum Ratings

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Silicon PN Photodiode Description BPW20RF is a planar Silicon PN photodiode in a hermetically sealed short TO 5 case, especially designed for high precision linear applications. Due to its extremely high dark resistance, the short circuit photocurrent is linear over seven decades of illumination level. On the other hand, there is a strictly logarithmic correlation between open circuit voltage and illumination over the same range. Equipped with a clear, flat glass window, the spectral responsitivity reaches from blue to near infrared. 94 8482 Features Hermetically sealed TO 5 case Flat glass window Cathode connected to case Wide viewing angle ϕ = 50 Large radiant sensitive area (A=7.5 mm 2 ) Suitable for visible and near infrared radiation High sensitivity UV enhanced Low dark current High shunt resistance Excellent linearity For photodiode and photovoltaic cell operation Applications Sensor for light measuring techniques in cameras, photometers, color analyzers, exposure meters (e.g. solariums) and other medical and industrial measuring and control applications. Absolute Maximum Ratings T amb = 25 C Parameter Test Conditions Symbol Value Unit Reverse Voltage V R V Power Dissipation T amb 50 C P V 300 mw Junction Temperature T j 125 C Operating Temperature Range T amb 55...+125 C Storage Temperature Range T stg 55...+125 C Soldering Temperature t 5 s T sd 260 C Thermal Resistance Junction/Ambient R thja 250 K/W 1 (5)

Basic Characteristics (T amb = 25 C) T amb = 25 C Parameter Test Conditions Symbol Min. Typ. Max. Unit Forward Voltage I F = 50 ma V F 1.3 V Breakdown Voltage I R = 20 µa, E = 0 V (BR) V Reverse Dark Current V R = 5 V, E = 0 I ro 2 30 na Diode Capacitance V R = 0 V, f = 1 MHz, E = 0 C D 1.2 nf V R = 5 V, f = 1 MHz, E = 0 C D 400 pf Dark Resistance V R = mv R D 38 GΩ Open Circuit Voltage E A = 1 klx V o 330 500 mv Temp. Coefficient of V o E A = 1 klx TK Vo 2 mv/k Short Circuit Current E A = 1 klx I k 20 60 µa Temp. Coefficient of I k E A = 1 klx TK Ik 0.1 %/K Reverse Light Current E A = 1 klx, V R = 5 V I ra 20 60 µa E e = 1 mw/cm 2, λ = 950 nm, V R = 5 V I ra 42 µa Angle of Half Sensitivity ϕ 50 deg Wavelength of Peak Sensitivity λ p 920 nm Range of Spectral Bandwidth λ 0.5 550...40 nm Rise Time V R = 0 V, R L = 1k Ω, λ = 820 nm Fall Time V R = 0 V, R L = 1k Ω, λ = 820 nm t r 3.4 µs t f 3.7 µs Typical Characteristics (T amb = 25 C, unless otherwise specified) I ro Reverse Dark Current ( na ) 94 8468 4 3 2 1 0 20 40 60 80 120 T amb Ambient Temperature ( C ) I ra rel Relative Reverse Light Current 94 8469 1.3 1.2 1.1 0.9 0 20 40 60 80 T amb Ambient Temperature ( C ) 120 Figure 1. Reverse Dark Current vs. Ambient Temperature Figure 2. Relative Reverse Light Current vs. Ambient Temperature 2 (5)

2 1400 I Short Circuit Current ( A ) k 1 0 1 2 3 C D Diode Capacitance ( pf ) 1200 0 800 600 400 200 E=0 f=1mhz 4 2 1 0 1 2 3 4 94 8470 E A Illuminance ( lx ) Figure 3. Short Circuit Current vs. Illuminance I ra Reverse Light Current ( A ) 94 8471 I ra Reverse Light Current ( A ) 94 8472 1 0.1 0.01 0.1 1 E e Irradiance ( mw/cm 2 ) Figure 4. Reverse Light Current vs. Irradiance 1mW/cm 2 0.5mW/cm 2 0.2mW/cm 2 0.1mW/cm 2 0.05mW/cm 2 1 0.1 1 V R Reverse Voltage ( V ) Figure 5. Reverse Light Current vs. Reverse Voltage 0 0.1 1 94 8473 V R Reverse Voltage ( V ) Figure 6. Diode Capacitance vs. Reverse Voltage S ( ) rel Relative Spectral Sensitivity 94 8474 0.4 0.2 0 350 550 750 950 Wavelength ( nm ) 1150 Figure 7. Relative Spectral Sensitivity vs. Wavelength S rel Relative Sensitivity 94 8475 0.9 0.7 0 0.4 0.2 0 0.2 0.4 20 Figure 8. Relative Radiant Sensitivity vs. Angular Displacement 30 40 50 60 70 80 3 (5)

Dimensions in mm 96 12181 4 (5)

Ozone Depleting Substances Policy Statement It is the policy of Vishay Semiconductor GmbH to 1. Meet all present and future national and international statutory requirements. 2. Regularly and continuously improve the performance of our products, processes, distribution and operating systems with respect to their impact on the health and safety of our employees and the public, as well as their impact on the environment. It is particular concern to control or eliminate releases of those substances into the atmosphere which are known as ozone depleting substances (ODSs). The Montreal Protocol (1987) and its London Amendments (1990) intend to severely restrict the use of ODSs and forbid their use within the next ten years. Various national and international initiatives are pressing for an earlier ban on these substances. Vishay Semiconductor GmbH has been able to use its policy of continuous improvements to eliminate the use of ODSs listed in the following documents. 1. Annex A, B and list of transitional substances of the Montreal Protocol and the London Amendments respectively 2. Class I and II ozone depleting substances in the Clean Air Act Amendments of 1990 by the Environmental Protection Agency (EPA) in the USA 3. Council Decision 88/540/EEC and 91/690/EEC Annex A, B and C (transitional substances) respectively. Vishay Semiconductor GmbH can certify that our semiconductors are not manufactured with ozone depleting substances and do not contain such substances. We reserve the right to make changes to improve technical design and may do so without further notice. Parameters can vary in different applications. All operating parameters must be validated for each customer application by the customer. Should the buyer use Vishay Telefunken products for any unintended or unauthorized application, the buyer shall indemnify Vishay Telefunken against all claims, costs, damages, and expenses, arising out of, directly or indirectly, any claim of personal damage, injury or death associated with such unintended or unauthorized use. Vishay Semiconductor GmbH, P.O.B. 3535, D-74025 Heilbronn, Germany Telephone: 49 (0)7131 67 2831, Fax number: 49 (0)7131 67 2423 5 (5)