ADR420/ADR421/ADR423/ADR425 Data Sheet
Rev. J | Page 16 of 24
TERMINOLOGY
Temperature Coefficient
The change of output voltage over the operating temperature
range is normalized by the output voltage at 25°C, and
expressed in ppm/°C as




6
10/
12
OUT
1
OUT
2
OUT
OUT
TTC25V
TVTV
CppmTCV
where:
V
OUT
(25°C) = V
OUT
at 25°C.
V
OUT
(T
1
) = V
OUT
at Temperature 1.
V
OUT
(T
2
) = V
OUT
at Temperature 2.
Line Regulation
The change in output voltage due to a specified change in input
voltage. It includes the effects of self-heating. Line regulation is
expressed in either percent per volt, parts per million per volt,
or microvolts per volt change in input voltage.
Load Regulation
The change in output voltage due to a specified change in load
current. It includes the effects of self-heating. Load regulation is
expressed in either microvolts per milliampere, parts per
million per milliampere, or ohms of dc output resistance.
Long-Term Stability
Typical shift of output voltage at 25°C on a sample of parts
subjected to operation life test of 1000 hours at 125°C.


1
OUT
0
OUTOUT
tVtVV



6
10
0
OUT
1
OUT
0
OUT
OUT
tV
tVtV
ppmV
where:
V
OUT
(t
0
) = V
OUT
at 25°C at Time 0.
V
OUT
(t
1
) = V
OUT
at 25°C after 1000 hours operation at 125°C.
Thermal Hysteresis
The change of output voltage after the device is cycled through
temperatures from +25°C to −40°C to +125°C and back to
+25°C. This is a typical value from a sample of parts put
through such a cycle.
TCOUTOUTHYSOUT
VC25VV
__


6
_
_
10
C25V
VC25V
ppmV
OUT
TCOUTOUT
HYSOUT
where:
V
OUT
(25°C) = V
OUT
at 25°C.
V
OUT_TC
= V
OUT
at 25°C after temperature cycle at +25°C to
−40°C to +125°C and back to +25°C.
Input Capacitor
Input capacitors are not required on the ADR42x. There is
no limit for the value of the capacitor used on the input, but a
1 µF to 10 µF capacitor on the input improves transient response
in applications where the supply suddenly changes. An addi-
tional 0.1 µF capacitor in parallel also helps to reduce noise
from the supply.
Output Capacitor
The ADR42x do not need output capacitors for stability under
any load condition. An output capacitor, typically 0.1 µF, filters
out any low level noise voltage and does not affect the operation
of the part. On the other hand, the load transient response can
be improved with an additional 1 F to 10 F output capacitor
in parallel. A capacitor here acts as a source of stored energy for
sudden increase in load current. The only parameter that
degrades by adding an output capacitor is the turn-on time,
which depends on the size of the selected capacitor.
Data Sheet ADR420/ADR421/ADR423/ADR425
Rev. J | Page 17 of 24
THEORY OF OPERATION
The ADR42x series of references uses a reference generation
technique known as XFET (eXtra implanted junction FET).
This technique yields a reference with low supply current, good
thermal hysteresis, and exceptionally low noise. The core of the
XFET reference consists of two junction field-effect transistors
(JFET), one having an extra channel implant to raise its pinch-
off voltage. By running the two JFETs at the same drain current,
the difference in pinch-off voltage can be amplified and used to
form a highly stable voltage reference.
The intrinsic reference voltage is about 0.5 V with a negative
temperature coefficient of about −120 ppm/°C. This slope is
essentially constant to the dielectric constant of silicon and can
be closely compensated by adding a correction term generated
in the same fashion as the proportional-to-temperature (PTAT)
term used to compensate band gap references. The primary
advantage over a band gap reference is that the intrinsic tem-
perature coefficient is approximately 30 times lower (therefore
requiring less correction). This results in much lower noise
because most of the noise of a band gap reference comes from
the temperature compensation circuitry.
Figure 38 shows the basic topology of the ADR42x series. The
temperature correction term is provided by a current source
with a value designed to be proportional to absolute tempera-
ture. The general equation is
V
OUT
= G × (∆V
P
R1 × I
PTAT
) (1)
where:
G is the gain of the reciprocal of the divider ratio.
V
P
is the difference in pinch-off voltage between the two JFETs.
I
PTAT
is the positive temperature coefficient correction current.
Each ADR42x device is created by on-chip adjustment of R2
and R3 to achieve the specified reference output.
02432-039
*
R3
GND
*EXTRA CHANNEL IMPLANT
V
OUT
= G(ΔV
P
– R1 × I
PTAT
)
R2
I
PTAT
ΔV
P
R1
V
IN
V
OUT
ADR420/ADR421/
ADR423/ADR425
I
1
I
1
Figure 38. Simplified Schematic
DEVICE POWER DISSIPATION CONSIDERATIONS
The ADR42x family of references is guaranteed to deliver load
currents to 10 mA with an input voltage that ranges from 4.5 V
to 18 V. When these devices are used in applications at higher
currents, the following equation should be used to account for
the temperature effects due to power dissipation increases:
T
J
= P
D
× θ
JA
+ T
A
(2)
where:
T
J
and T
A
are the junction temperature and the ambient
temperature, respectively.
P
D
is the device power dissipation.
θ
JA
is the device package thermal resistance.
BASIC VOLTAGE REFERENCE CONNECTIONS
Voltage references, in general, require a bypass capacitor
connected from V
OUT
to GND. The circuit in Figure 39
illustrates the basic configuration for the ADR42x family of
references. Other than a 0.1 µF capacitor at the output to help
improve noise suppression, a large output capacitor at the
output is not required for circuit stability.
02432-040
NIC = NO INTERNA
L CONNECTION
T
P
= TEST PIN (DO NOT CONNECT)
ADR420/
ADR421/
ADR423/
ADR425
T
OP
VIEW
(Not to Scale)
T
P
1
V
IN
2
NIC
3
4
TP
8
NIC
7
OUTPUT
6
TRIM
5
0.1µ
F
0.1
µ
F10µ
F
+
Figure 39. Basic Voltage Reference Configuration
NOISE PERFORMANCE
The noise generated by ADR42x references is typically less
than 2 µV p-p over the 0.1 Hz to 10 Hz band for the ADR420,
ADR421, and ADR423. Figure 24 shows the 0.1 Hz to 10 Hz
noise of the ADR421, which is only 1.75 µV p-p. The noise
measurement is made with a band-pass filter made of a 2-pole
high-pass filter with a corner frequency at 0.1 Hz and a 2-pole
low-pass filter with a corner frequency at 10 Hz.
TURN-ON TIME
At power-up (cold start), the time required for the output
voltage to reach its final value within a specified error band
is defined as the turn-on settling time. Two components typi-
cally associated with this are the time for the active circuits to
settle and the time for the thermal gradients on the chip to
stabilize. Figure 31 to Figure 35 show the turn-on settling time
for the ADR421.
ADR420/ADR421/ADR423/ADR425 Data Sheet
Rev. J | Page 18 of 24
APPLICATIONS
OUTPUT ADJUSTMENT
The ADR42x trim terminal can be used to adjust the output
voltage over a ±0.5% range. This feature allows the system
designer to trim system errors out by setting the reference to
a voltage other than the nominal. This is also helpful if the
part is used in a system at temperature to trim out any error.
Adjustment of the output has a negligible effect on the
temperature performance of the device. To avoid degrading
temperature coefficients, both the trimming potentiometer
and the two resistors need to be low temperature coefficient
types, preferably <100 ppm/°C.
02432-041
ADR420/
ADR421/
ADR423/
ADR425
R2
V
IN
INPUT
GND
TRIM
R1
470k
R
P
10k
10k (ADR420)
15k
(ADR421)
OUTPUT
V
OUT
= ±0.5%
V
OUT
2
4
5
6
Figure 40. Output Trim Adjustment
REFERENCE FOR CONVERTERS IN OPTICAL
NETWORK CONTROL CIRCUITS
In the high capacity, all optical router network of Figure 41,
arrays of micromirrors direct and route optical signals from
fiber to fiber, without first converting them to electrical form,
which reduces the communication speed. The tiny micro-
mechanical mirrors are positioned so that each is illuminated
by a single wavelength that carries unique information and
can be passed to any desired input and output fiber. The mirrors
are tilted by the dual-axis actuators controlled by precision
analog-to-digital converters (ADCs) and digital-to-analog
converters (DACs) within the system. Due to the microscopic
movement of the mirrors, not only is the precision of the
converters important, but the noise associated with these
controlling converters is extremely critical, because total noise
within the system can be multiplied by the numbers of
converters used. Consequently, the exceptional low noise of the
ADR42x is necessary to maintain the stability of the control
loop for this application.
02432-042
DAC
DAC
ADC
DSP
CONTRO
L
ELECTRONICS
ACTIVA
TOR
LEFT
LASER BEAM
SOURCE FIBER
GIMBAL
+ SENSOR
DESTINATION
FIBER
ACTI
VA
TOR
RIGHT
MEMS MIRROR
AMP
LPREAM
PAMP
L
ADR421
ADR421
ADR421
Figure 41. All Optical Router Network
HIGH VOLTAGE FLOATING CURRENT SOURCE
The circuit in Figure 42 can be used to generate a floating
current source with minimal self-heating. This particular
configuration can operate on high supply voltages determined
by the breakdown voltage of the N-channel JFET.
02432-044
+V
S
–V
S
SST11
1
VISHA
Y
V
IN
GND
V
OUT
ADR420/
ADR421/
ADR423/
ADR425
2N3904
R
L
2.10k
OP09
2
4
6
Figure 42. High Voltage Floating Current Source

ADR423BRZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Voltage References Low Noise 3.00V Ultraprecision
Lifecycle:
New from this manufacturer.
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