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IC212 highspeed photoreceiver rev a2, page 1/ 15 features ? bandwidth dc to 1.4 ghz ? si pin photodiode, ? 0.4 mm active area diameter ? spectral response range = 320 to 1000 nm ? ampli?er transimpedance (gain) 3.125 v/ma ? max. conversion gain 1.625 v/mw @ 760 nm applications ? fast pulse and transient measurement ? optical triggering ? optical front-end for oscilloscopes block diagram copyright ? 2010 ic-haus http://www.ichaus.com p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 2/ 15 description the ic-haus highspeed photoreceiver IC212 has been developed for optical high speed measurement. with its bandwidth ranging from dc up to 1.4 ghz it detects photo signals from constant light to high speed with rise times down to 280 ps. the IC212 highspeed photoreceiver also features offset adjust- ment to compensate dc levels of the input signal. the photodiode used offers a spectral range from 320 to 1000 nm with an active area diameter of about ? 0.4 mm, which is increased by an ? 1.5 mm ball lens, resulting in an effective usable area of typical 0.75 mm2. the highspeed photoreceiver is able to detect optical power levels in the sub mw range at ghz speed. the IC212 highspeed photoreceiver comes with m6 mounting holes for integration in optical bench sys- tems and an optional ?ber-optic input adapter for op- tical ?ber coupling. absolute maximum ratings beyond these values damage may occur; device operation is not guaranteed. item symbol parameter conditions unit no. min. max. g001 pmax optical input power 10 mw g002 vs power supply voltage 20 v electrical characteristics test conditions: vs = 15 v, ta = 25 c, system impedace 50
item symbol parameter conditions unit no. min. typ. max. gain 101 a ampli?er transimpedance conversion gain 50
load 3.125 v/ma = 760 nm 1.625 v/mw frequency response 201 fmax upper cut-off frequency -3 db 1.4 ghz 202 a gain flatness 1 db 203 tr rise time 10 to 90% 280 ps 204 tpd propagation delay optical in => electrical out, 50% to 50% 750 ps detector (si pin photodiode) 301 d active area diameter ball lens ? 1.5 mm 0.4 mm 302 aeff effective active area ball lens ? 1.5 mm, note tolerances from fig. 3 0.75 mm2 303 spectral range 320 1000 nm 304 pmax max. optical input power average 10 mw linear ampli?cation @ 760 nm 615 w 305 nep noise equivalent power including ampli?er noise, at =760nm and f = 1 ghz; (for frequency dependence see fig. ?? ) 115 pw/ p hz output 401 rout output impedance 50
402 vout output voltage swing 50
load, for linear ampli?cation -0.3 1.0 v 403 vos offset voltage (adjustable) dc offset cancellation -1.25 0.15 v 404 pos offset (adjustable) equivalent optical power -92 750 w 405 twu warm-up time stable offset voltage 30 min power supply 501 vs supply voltage 15 v 502 is supply current 150 ma the output is clipped to -0.5 v, if the offset voltage is less than 0.5 v and no dc light is present. p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 3/ 15 contents the purchased parts package includes ? highspeed photoreceiver IC212 ? power adapter (230 vac) ? coaxial cable with sma plugs ? sma to bnc adapter ? fiber adapter figure 1: box contents p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 4/ 15 dimensions figure 2: case dimensions (all units in mm) p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 5/ 15 connectors input optical, with microbench adapter (? 25 mm) and sma ?ber adaption output sma connector power supply hirose series hr10-7r-6p, 6-pin pin 1, 2: +vs pin 3, 6: gnd pin 4, 5: -vs table 1: connectors photodiode with ball lens figure 3: photodiode with ball lens (lens type borosilicate glass) p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 6/ 15 response figure 4: spectral response figure 5: pulse response p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 7/ 15 application notes these application notes are meant to demonstrate some typical measurement tasks, carried out with the IC212 and veri?ed with a standard optical power meter. mesurement of total optical output power p opt 1. put laser in pulse mode 2. adjust lens, for maximum amplitude at the output of IC212 (fig. 6 ) 3. read amplitude: u = 0.803 v (fig. 7 ) calculation: = 635 nm, spectral response taken from figure 4 : s(@635 nm) = 1.34 v/mw p opt ( ic 212) = u s = 0.803 v 1.34 v mw = 0.60 mw 4. put laser in cw mode 5. put newport sensor into laser beam and read the power: p opt (newport) = 0.641 mw (fig. 8 ) the results match within 7%. figure 6: the laser light focused with a collecting lens onto the sensor figure 7: oscilloscope reading figure 8: total optical output power with 1 cm2 sen- sor (newport) p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 8/ 15 measurment of irradiance e 1. put laser in cw mode 2. homogenisation of laser light with microlens ar- rays (fig. 10 ) 3. put IC212 into the center of the homogenised laser light (fig. 11 ) 4. read oscilloscope: u = 76 mv (fig. 12 ) calculation: = 659 nm, spectral response taken from figure 4 : s(@659 nm) = 1.42 v/mw, effec- tive area (item no. 302: aeff = 0.75 mm2) e ( ic 212) = u s a eff = 0.076 v 1.42 v mw 0.75 mm 2 = 0.071 mw mm 2 figure 9: laser 659 nm, 150 mw with two mi- crolens arrays for homogenisation figure 10: homogeneously illuminated area of ca. 4 cm x 4 cm 5. put newport sensor into laser beam and read the power: p opt (newport) = 6.441 mw (fig. 13 ) 6. with a sensor area of 100 mm2 this results in e(newport) = 0.0644 mw/mm2 the results match within 10%. figure 11: IC212 in the center of the homogenised laser light figure 12: oscilloscope reading figure 13: newport sensor in the center of the ho- mogenised laser light p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 9/ 15 measuring time of ?ight figure 14: laser, pole ?lter, beam expander, beam splitter and two IC212 figure 15: no propagation time difference at same distance from beam splitter figure 16: one IC212 positioned 30 cm closer to the beam splitter figure 17: 30 cm distance difference means 1 ns propagation time difference p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 10/ 15 fiber-optic input figure 18: laser, sma ?ber collimator, ?ber, IC212 ?ber adapter, IC212 figure 19: IC212 ?ber adapter figure 20: sma ?ber collimator figure 21: fiber transmitted light pulse p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 11/ 15 noise equivalent power (nep) nep speci?es the lowest light power (pmin) that can be detected by the sensor. in that case the signal to noise ratio (s/n) would be 1, which means the signal to be measured is of the same magnitude as the noise. p min ( ) = s max s ( ) nep p bw p min ( ) - minimum detectable power, which can be distinguished from noise (only white noise, 1/f-noise ignored) s( ) - photo sensitivity at wavelength s max - maximum photo sensitivity nep - nep at maximum photo sensitivity bw - bandwidth example blue led with = 473 nm, square wave modulated f = 1 mhz (t = 1 s), bandwidth of measuring circuit bw = 93 mhz. s max = 1.625 v/mw (figure 4 ) nep = 115 pw/ p hz (item no. 305) s( = 473 nm) = 0.67 v/mw (figure 4 ) p min ( = 473 nm ) = 1.625 0.67 115 pw p hz p 93 mhz = 2.7 w rms this calculation is only valid, if the input noise is fre- quency independent. figure 22 shows the input noise (inv = input noise voltage) of the photo ampli?er. figure 22: input noise voltage as a function of the frequency - with lower frequencies there is higher noise for frequencies around 93 mhz an input noise of 215 nv/ p hz can be estimated. nep( ) = inv(f) * 1/s( ) nep( = 473 nm) = inv(93 mhz) / s( = 473 nm) nep( = 473 nm) = 215 nv/ p hz * 1 mw / 0.67 v = 320 pw/ p hz noise(bw) = nep( = 473 nm) * p bw noise(93 mhz) = 320 pw/ p hz * p 93 mhz = 3.09 w rms as to be expected this value is slightly higher than in the ?rst estimation. mesurement of minimum optical power p min ( ) 1. homogenisation of the blue led light with mi- crolens arrays (figure 23 ) 2. led modulation with 1 mhz 3. change distance between IC212 and led un- til signal is barely distinguishable from noise (method imprecise but rather simple to get a ba- sic estimation) 4. put newport sensor at same distance as IC212 into the led beam and read the power: pm = 126 w (figure 25 ) because of the duty cycle (50%), the measured power has to be multiplied by 2. the newport sensor is com- pletely illuminated (100 mm2). hence the irradiance can be calculated to e ( newport ) = 2 126 w 100 mm 2 = 2.52 w mm 2 with the effective area of the IC212 sensor (item no. 302, a eff = 0.75 mm2) this yield a total power of p min ( = 473, measured ) = 2.52 w mm 2 0.75 mm 2 = 1.9 w this matches the calculated value reasonably well. output noise without signal: noise ( bw ) = inv ( f ) p bw noise (93 mhz ) = 215 nv p hz p 93 mhz = 2.07 mv rms a slightly higher value of = 3 mv rms has been mea- sured though. p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 12/ 15 figure 23: homogenised blue led light figure 24: homogeniously illuminated IC212 figure 25: homogeniously illuminated newport sensor figure 26: noise figure 27: noise with signal barely detectable p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 13/ 15 ulbricht sphere figure 28: 3-port ulbricht sphere with IC212 and newport power meter figure 29: hg1m laser controller with 2 w cw laser diode on the ideal size of an ulbricht sphere see also "how to select an integrating sphere for your application" by valerie c. coffey at www.optoiq.com . figure 30: laser light coupled into the ulbricht sphere figure 31: laser pulse with 260 ps rise time (chan- nel 1) figure 32: due to size of ulbricht sphere the pulse gets distorted (ca. 4 ns rise time) p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 14/ 15 equipment used mesuring instruments tektronix: tds7404b, 4 ghz, 20 gs/s, 4-channel digital phosphor oscillo- scope newport: optical power meter model 840 newport: sensor 818-st, sensor 818-uv, sensor 818-st/cm newport: 819d-sl-3.3, 3-port 3.3" spectralon ulbricht sphere ocean optics: usb2000 fiber-optic spectrometer 320 - 1100 nm omicron: ldm639.40.500, 40 mw laser, f mod > 500 mhz femto: hsa-x-s-1g4-si, ultra high speed photoreceiver ic-haus: IC212 highspeed photoreceiver, dc to 1.4 ghz hp: 8590l, spectrum analyzer accessories ic-haus: ic149, 8-bit pulse generator ,1 to 64 ns, compatibel to ldmxxx series lasers by omi- cron ic-haus: ic213, 12-bit oszillator, 40 khz to 500 mhz, compatibel to ldmxxx series lasers by omi- cron ic-haus: ic215_6, pulse width modulator, 640 ps to 10.23 ns, compatibel to ldmxxx series lasers by omicron and ic213 ic-haus: hg1m, control module for high speed, high power laser diodes ic-haus expressly reserves the right to change its products and/or speci?cations. an infoletter gives details as to any amendments and additions made to the relevant current speci?cations on our internet website www.ichaus.de/infoletter ; this letter is generated automatically and shall be sent to registered users by email. copying C even as an excerpt C is only permitted with ic-haus approval in writing and precise reference to source. ic-haus does not warrant the accuracy, completeness or timeliness of the speci?cation on this site and does not assume liability for any errors or omissions in the materials. the data speci?ed is intended solely for the purpose of product description. no representations or warranties, either express or implied, of merchantability, ?tness for a particular purpose or of any other nature are made hereunder with respect to information/speci?cation or the products to which information refers and no guarantee with respect to compliance to the intended use is given. in particular, this also applies to the stated possible applications or areas of applications of the product. ic-haus conveys no patent, copyright, mask work right or other trade mark right to this product. ic-haus assumes no liability for any patent and/or other trade mark rights of a third party resulting from processing or handling of the product and/or any other use of the product. as a general rule our developments, ips, principle circuitry and range of integrated circuits are suitable and speci?cally designed for appropriate use in technical applications, such as in devices, systems and any kind of technical equipment, in so far as they do not infringe existing patent rights. in principle the range of use is limitless in a technical sense and refers to the products listed in the inventory of goods compiled for the 2008 and following export trade statistics issued annually by the bureau of statistics in wiesbaden, for example, or to any product in the product catalogue published for the 2007 and following exhibitions in hanover (hannover-messe). we understand suitable application of our published designs to be state-of-the-art technology which can no longer be classed as inventive under the stipulations of patent law. our explicit application notes are to be treated only as mere examples of the many possible and extremely advantageous uses our products can be put to. p r e l i m i n a r y p r e l i m i n a r y
IC212 highspeed photoreceiver rev a2, page 15/ 15 ordering information type package order designation IC212 IC212 for technical support, information about prices and terms of delivery please contact: ic-haus gmbh tel.: +49 (61 35) 92 92-0 am kuemmerling 18 fax: +49 (61 35) 92 92-192 d-55294 bodenheim web: http://www.ichaus.com germany e-mail: sales@ichaus.com appointed local distributors: http://www.ichaus.com/sales_partners p r e l i m i n a r y p r e l i m i n a r y

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