Electronic Components Datasheet Search |
|
C1953P Datasheet(PDF) 4 Page - PerkinElmer Optoelectronics |
|
C1953P Datasheet(HTML) 4 Page - PerkinElmer Optoelectronics |
4 / 11 page EU PerkinElmer Optoelectronics GmbH Heimann Opto 65020 Wiesbaden, Germany PO-Box 3007 http://www.perkinelmer.com/opto USA PerkinElmer Optoelectronics 2175 Mission College Blvd. Santa Clara, CA 95054 Tel. ++1 (408) 565 - 0830 Fax ++1 (408) 565 - 0703 http://www.perkinelmer.com/opto Excellent photon counting resolution At gains exceeding 107 the single photo electron pulse is perfectly separated from the electrical noise, due to a sa- turation effect of the channel. The CPM exhibits single photon resolution with excellent peak to valley ratios. Fig. 3 shows the single photo electron spectrum taken from a multi-channel analyzer compared to a conventional photomultiplier (Fig. 3). Choice of entrance window The CPM is available with different window materials, which are: MgF2, Quartz, UV-glass, and Borosilicate glass. The com- bination of different photocathodes and entrance windows results in a spectral range from 115 nm to 900 nm. Other window materials and photocathode combinations are available on a custom basis (Fig. 4.1 and 4.2). Available related products • High Voltage supply CHV 30N (supplies 1 CPM, negative output voltage), CHV 30P (supplies 1 CPM, positive output voltage), J4-3N (supplies 10 to 15 CPMs) • CPM Modules MP900-series: Photoncounting module with TTL output, including CPM, electronic and high voltage MD900-series: DC module including high voltage supply, amplifier, I/U converter, output 0 to 10 V, bandwidth 1kHz MH900-series: High voltage module, including CPM and high voltage power supply • CPM Formats 1 /3“ C900-series 1 /2“ C1300-series 3 /4“ C1900-series Datasheets on request 0 50 100 150 200 CPM PMT 250 300 2000 1500 1000 500 0 Channel Fig. 3: Typical photo electron spectrum Wavelength (nm) 100 C 922 C 952 C 911 C 972 200 300 400 500 600 700 800 900 100 10 1 0.1 Fig. 4.1: Typical spectral response C 973 Wavelength (nm) 100 C 942 C 943 C 962 200 300 400 500 600 700 800 900 Fig. 4.2: Typical spectral response 100 10 1 0.1 C 944 High stability in dark current level As a result of the semiconductive inner surface of the CPM, no charge-up effects occur at the glass surface. This results in a very high stability of the dark current level over time, with no sudden changes (bursts). The semiconductive surface also causes high-light recovery times to be extremely small. |
Similar Part No. - C1953P |
|
Similar Description - C1953P |
|
|
Link URL |
Privacy Policy |
ALLDATASHEET.COM |
Does ALLDATASHEET help your business so far? [ DONATE ] |
About Alldatasheet | Advertisement | Datasheet Upload | Contact us | Privacy Policy | Link Exchange | Manufacturer List All Rights Reserved©Alldatasheet.com |
Russian : Alldatasheetru.com | Korean : Alldatasheet.co.kr | Spanish : Alldatasheet.es | French : Alldatasheet.fr | Italian : Alldatasheetit.com Portuguese : Alldatasheetpt.com | Polish : Alldatasheet.pl | Vietnamese : Alldatasheet.vn Indian : Alldatasheet.in | Mexican : Alldatasheet.com.mx | British : Alldatasheet.co.uk | New Zealand : Alldatasheet.co.nz |
Family Site : ic2ic.com |
icmetro.com |