Data Sheet ADPD2214
Rev. 0 | Page 9 of 13
THEORY OF OPERATION
OVERVIEW
The ADPD2214 is an integrated, low power, optical sensor
composed of a deep junction silicon photodiode coupled to a
low noise current amplifier in an optically transparent chip
scale package. The ADPD2214 is optimized for battery-
powered, wearable, medical, and industrial optical sensing
applications requiring low power and high SNR.
SHOT NOISE LIMITED PERFORMANCE
The on-board photodiode of the ADPD2214 is operated in
photoconductive mode with a zero bias voltage. This mode of
operation allows the diode to operate with no dc dark current
caused by leakage across the depletion area of the diode,
providing a fundamental limit of shot noise. The noise level is
proportional to the square root of the frequency bandwidth.
SENSITIVITY AND SNR
SNR is a measure of the ability of the sensor to separate the
signal of interest from spurious signals that occur from the
surrounding environment of the device, such as ambient light,
nonlinearity, and noise within the device itself.
The ADPD2214 operates its integrated photodiode in a zero
biased photoconductive mode to provide near zero dark current
and, therefore, no dark shot noise component contribution
from the photodiode. The integrated current amplifier requires
an internal bias current of 10 nA to improve bandwidth and
linearize response at low light levels. This bias generates a shot
noise component of 90 fA/Hz at the output of the current
amplifier and establishes the noise floor of the ADPD2214.
To optimize the sensitivity of the ADPD2214, it is important to
ensure that the optical signal is concentrated on the photoactive
area of the integrated photodiode. The on-board precision
current amplifier is shielded and is not significantly affected by
light hitting its surface, but device sensitivity is based solely on
the optical power incident to the photodetector.
LINEARITY
Linearity is critical to PPG due to the need to accurately extract
a small amplitude, pulsatile ac signal modulated onto the large
dc component, which is caused by nonpulsatile tissue absorption
and ambient light. In pulsed light applications, bandwidth is a
critical component of the linearity because fast recovery of the
device from dark and/or power-down conditions can have a
profound effect on the ability of the sensor to extract the signal
of interest. The ADPD2214 is production trimmed to ensure
60 dB linearity at an irradiance of up to E
E
= 890 µW/cm
2
, λ =
528 nm, at a supply voltage of 3.3 V.
PACKAGE CONSIDERATIONS
The ADPD2214 is packaged with a transparent epoxy molding
compound. To maintain optimum sensitivity, take care in
handling the device to prevent scratches or chemicals that may
affect the surface finish above the photodiode. Due to the lack
of stabilizing fillers (typically up to 70% silica) used in opaque
molding compounds, the maximum storage temperature of the
ADPD2214 is 105°C. The temperature profile for soldering is
shown in Figure 2.
EPAD CONNECTION
The EPAD on the ADPD2214 acts as a common electrical, thermal,
and mechanical platform for the photodiode and amplifier and
must not be connected externally. External cooling is not required
due to the extremely low power consumption of the ADPD2214.
Analog Devices, Inc., recommends removal of traces beneath
the device to eliminate potential coupling of external signals into
the sensitive internal nodes of the ADPD2214.
ADPD2214 Data Sheet
Rev. 0 | Page 10 of 13
APPLICATIONS INFORMATION
The current output of the ADPD2214 provides flexibility in
interfacing to external circuitry.
POWERING THE DEVICE
The ADPD2214 is powered from a single positive 1.8 V to 5.0 V
supply. The ADPD2214 features high PSRR, but proper circuit
layout and bypassing is recommended to provide maximum
sensitivity, especially in situations where the ADPD2214 may share
reference nodes with transmitters in pulse mode applications.
Above the quiescent current of the integrated current amplifier,
there is a linear relationship to incident light as the current
amplifier amplifies the photodiode output by a factor of 24. In
typical battery-powered operation, the output of the source
LEDs is dynamically reduced to save power based on the
received signal strength of the photosensor. The extremely low
noise floor of the ADPD2214 provides very high SNR, allowing
accurate signal extraction with minimal source power and at
low incident optical power.
POWER-DOWN
The ADPD2214 is optimized for battery-powered operation by
the inclusion of an extremely low power standby mode that can
be quickly switched to provide ultralow power consumption
during dark periods in pulsed or mode locked applications,
where the light source is cycled to improve ambient light
rejection and reduce transmitter power consumption. The
power-down pin is not internally pulled up or down, and must
be connected to an external logic level for proper operation of
the ADPD2214.
PULSE MODE OPERATION
The ADPD2214 is optimized for battery-powered operation by
the inclusion of a power-down pin (PWDN). When sensing is
inactive, the ADPD2214 can be quickly switched into standby
mode, reducing the supply current to 1 µA during dark periods
for pulsed or mode locked applications, where the light source
is cycled to improve ambient light rejection and reduce
transmitter power consumption.
For multiple wavelength systems, sequentially pulsing the optical
emitters removes the need for multiple narrow bandwidth sensors.
For both multiple wavelength (SpO2) and single wavelength
(heart rate monitoring) systems, pulsed operation can provide
significant power savings for battery-powered systems. Pulsed
mode operation provides a calibration signal that is necessary to
compensate for ambient light diffused throughout the tissue,
which can be extracted by measuring the sensor output while
the system emitters are off. Advanced algorithms can then
extract the signal of interest from dc offsets, noise, and
interferer signals such as motion artifacts.
OUTPUT CONFIGURATION
The output of the ADPD2214 allows different configurations
depending on the application. The current gain of the ADPD2214
reduces the effect of surrounding interferers but, for best perfor-
mance, careful design and layout is still necessary to achieve the
best performance. The effect of capacitance on the output must
be considered carefully regardless of configuration as bandwidth
and response time of the system can be limited simply by the
time required to charge and discharge parasitics.
Because theADPD2214 is effectively a current source, the
ADPD2214 output voltage drifts up to its compliance voltage,
approximately 1.2 V below VCC, when connected to an interface
that presents a high impedance. The rate of this drift is dependent
on the ADPD2214 output current, parasitic capacitance, and the
impedance of the load. This drift can require additional settling
time in circuits following the ADPD2214 if they are actively
multiplexing the output of the ADPD2214 or presenting a high
impedance due to power cycling. For multiplexed systems, a
current steering architecture may offer a performance advantage
over a break-before-make switch matrix.
3-WIRE CABLE VOLTAGE CONFIGURATION
The ADPD2214 can be used in a minimal 3-wire voltage
configuration, offering a compact solution with very few
components (see Figure 11). A shunt resistor (R
S
) sets the
transimpedance gain in front of the analog-to-digital converter
(ADC). This configuration allows flexibility in matching the
ADC converter full-scale input to the full-scale output of the
ADPD2214. The dynamic range of the interface is limited to
the compliance voltage of the ADPD2214.
No additional amplification is needed prior to the ADC. Response
time at the lower end of the range is limited by the ability of the
output current to charge the parasitic capacitance presented to
the output of the ADPD2214.
3-WIRE CURRENT MODE CONFIGURATION
When used in the 3-wire current mode configuration with a
photodiode (see Figure 12), the ADPD2214 is insensitive to load
resistance and can be used when the signal processing is further
from the sensor. EMI noise and shielding requirements are
minimized; however, cable capacitance has a direct effect on
bandwidth, making the 3-wire current mode configuration a
better choice for unshielded interfaces. The feedback capacitance
(C
F
) value must be chosen carefully to eliminate stability and
bandwidth degradation of the ADPD2214. Large capacitance
around the feedback loop of the TIA has a direct effect on the
bandwidth of the system.
Data Sheet ADPD2214
Rev. 0 | Page 11 of 13
Figure 11. ADPD2214 Used in 3-Wire Cable Voltage Configuration
Figure 12. ADPD2214 Used in 3-Wire Current Mode Configuration
ADPD2214
CURRENT
AMPLIFIER
+
ADC AND
MICROPROCESSOR
3.3V
3.3V
R
S
GND
OUT
VCC
13722-023
VCC
OUT
GND
3.3V
C
F
R
F
TIA
3.3V
ADPD2214
ADC AND
MICROPROCESSOR
0V TO V
CC
–0.75
CURRENT
AMPLIFIER
+
13722-024

ADPD2214ACPZ-R7

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Photo IC Sensors Ultra-Low Noise Integr Int Sensor
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
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