LT1319CS [Linear]

Multiple Modulation Standard Infrared Receiver; 多种调制标准的红外接收器
LT1319CS
型号: LT1319CS
厂家: Linear    Linear
描述:

Multiple Modulation Standard Infrared Receiver
多种调制标准的红外接收器

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LT1319  
Multiple Modulation Standard  
Infrared Receiver  
U
DESCRIPTIO  
EATURE  
S
F
The LT®1319 is a general purpose building block that  
contains all the circuitry necessary to transform modu-  
lated photodiode signals back to digital signals. The  
circuit’sflexibilitypermitsittoreceivemultiplemodulation  
methods. A low noise, high frequency preamplifier per-  
forms a current-to-voltage conversion while rejecting low  
frequency ambient interference with an AC coupling loop.  
Two separate high impedance filter buffer inputs are  
provided so that off-chip filtering can be tailored for  
specificmodulationschemes.Thefilterbuffersdrivesepa-  
rate differential gain stages that end in comparators with  
internalhysteresis. Thecomparatorthresholdsareadjust-  
able externally by the current into Pin 11. One channel has  
ahighspeed25nscomparatorrequiredforhighdatarates.  
The second channel’s comparator has a 60ns response  
time and is well suited to more modest data rates. A power  
savingshutdownfeatureisusefulinportableapplications.  
Receives Multiple IR Modulation Methods  
Low Noise, High Speed Preamp: 2pA/Hz, 7MHz  
Low Frequency Ambient Rejection Loops  
Dual Gain Channels: 8MHz, 400V/V  
25ns and 60ns Comparators  
16-Lead SO Package  
5V Single Supply Operation  
Supply Current: 14mA  
Shutdown Supply Current: 500µA  
External Comparator Threshold Setting  
W
U
U
ODULATIO STA DARDS  
IRDA: SIR, FIR  
Sharp/Newton  
TV Remote  
High Data Rate Modulation Methods  
For IRDA 4PPM contact the LTC Marketing Department.  
, LTC and LT are registered trademarks of Linear Technology Corporation.  
U
TYPICAL APPLICATION  
IRDA and Sharp/Newton Data Receiver  
SHUTDOWN INPUT  
IRDA DATA  
SHARP/NEWTON DATA  
V
CC  
1
2
3
4
5
6
7
8
16  
15  
14  
13  
12  
11  
10  
9
AN_GND  
BYPASS  
IN  
LT1319  
V
CC  
FILT1  
PREOUT  
C
B3  
10µF  
SHDN  
DATAL  
C
C
R
B1  
0.1µF  
B2  
T1  
10µF  
30k  
V
DIG_GND  
BIAS  
L
F1  
R
R
F1  
1k  
F2  
FILTINL  
FILT2L  
FILTIN  
V
TH  
D1*  
100µH  
2k  
C
T1  
1µF  
DATA  
FILT2  
C
C
C
B4  
1µF  
C
C
F5  
1µF  
C
F3  
F2  
F4  
F1  
100pF  
1nF  
2.2nF  
10nF  
*BPW34FA OR BPV22NF  
DGND  
AGND  
LT1319 • TA01  
1
LT1319  
W W W  
U
/O  
ABSOLUTE AXI U RATI GS  
PACKAGE RDER I FOR ATIO  
Total Supply Voltage (VCC to GND) ........................... 6V  
Differential Voltage (Any Two Pins) .......................... 6V  
Maximum Junction Temperature ......................... 150°C  
Operating Temperature Range .................... 0°C to 70°C  
Specified Temperature Range..................... 0°C to 70°C  
Storage Temperature Range ................ 65°C to 150°C  
Lead Temperature (Soldering, 10 sec)................. 300°C  
TOP VIEW  
ORDER PART  
AN_GND  
IN  
1
2
3
4
5
6
7
8
16  
15  
14  
13  
12  
11  
10  
9
BYPASS  
NUMBER  
V
CC  
FILT1  
SHDN  
LT1319CS  
PREOUT  
DATAL  
DIG_GND  
V
BIAS  
FILTINL  
FILT2L  
FILTIN  
V
TH  
DATA  
FILT2  
S PACKAGE  
16-LEAD PLASTIC SO  
TJMAX = 150°C, θJA = 100°C/W  
Consult factory for Industrial or Military grade parts.  
ELECTRICAL CHARACTERISTICS  
TA = 25°C, V15 = 5V, V1 = V12 = 0V, V6 = V8 = V14 = 2V, unless otherwise specified.  
SYMBOL PARAMETER  
CONDITIONS  
MIN  
TYP  
MAX  
UNITS  
V
OS  
Preamp Input Offset Voltage  
Preamp Output Offset Voltage  
Preamp Loop Offset Voltage  
High Gain Loop Offset Voltage  
Low Gain Loop Offset Voltage  
V (Pin 2) – V (Pin 5)  
V (Pin 4) – V (Pin 5)  
V (Pin 3) – V (Pin 5)  
V (Pin 9) – V (Pin 5)  
V (Pin 7) – V (Pin 5)  
4
15  
25  
250  
950  
950  
mV  
mV  
mV  
mV  
mV  
10  
50  
600  
600  
150  
800  
800  
A
VP  
Preamp Transimpedance  
±10µA Into Pin 2, Measure V (Pin 4), Fix Pin 3  
10  
15  
17  
kΩ  
Preamp Output Swing, Positive  
Preamp Output Swing, Negative  
100µA Out of Pin 2, Measure V (Pin 4), Fix Pin 3  
100µA Into Pin 2, Measure V (Pin 4), Fix Pin 3  
0.25  
0.55  
0.4  
0.4  
0.55  
0.25  
V
V
BW  
Preamp Bandwidth  
C (Pin 3) = 1µF, Measure f  
C (Pin 3) = 1µF, f = 10kHz  
7
2
MHz  
P
3dB  
i
n
Preamp Input Noise Current  
pA/Hz  
Preamp Loop Rejection, Positive  
Preamp Loop Rejection, Negative  
50µA Into Pin 2, Measure V (Pin 4)  
50µA Out of Pin 2, Measure V (Pin 4)  
–3  
–3  
–1  
1
3
3
mV  
mV  
Preamp Loop Output Current, Positive  
Preamp Loop Output Current, Negative  
100µA Out of Pin 2, Measure I (Pin 3), (Note 1)  
100µA Into Pin 2, Measure I (Pin 3), (Note 1)  
150  
50  
100  
100  
50  
150  
µA  
µA  
V
V
Bias Voltage  
V (Pin 5)  
1.7  
4.75  
0.1  
1.9  
4.9  
0.5  
40  
2.1  
4.95  
1.4  
V
V
µA  
BIAS  
Bypass Voltage  
Filter Buffer Input Bias Current  
Filter Buffer Input Resistance  
V (Pin 16)  
I (Pin 6), I (Pin 8)  
BYPASS  
I
B
R
V = 0.1V, Measure I Pin 6, Pin 8  
MΩ  
IN  
B
Gain Stage Loop Rejection, Positive  
Gain Stage Loop Rejection, Negative  
V = 50mV (Pin 6, Pin 8), Measure V (Pin 7, Pin 9)  
0.33  
0.45  
0.45  
0.57  
0.33  
V
V
V = 50mV (Pin 6, Pin 8), Measure V (Pin 7, Pin 9) 0.57  
A
Gain Stages Voltage Gain  
Gain Stages Bandwidth  
(Note 2)  
400  
8
V/V  
VG  
BW  
C (Pin 7) = C (Pin 9) = 1µF  
MHz  
G
t
Fast Comparator Response Time  
Slow Comparator Response Time  
10mV Overdrive  
10mV Overdrive  
25  
60  
ns  
ns  
r
V
V
V
Fast Comparator Hysteresis Voltage  
Slow Comparator Hysteresis Voltage  
(Note 3)  
(Note 3)  
35  
40  
mV  
mV  
HYS  
Fast Comparator Output High Voltage  
Slow Comparator Output High Voltage  
V (Pin 9) = 200mV, 1mA Out of Pin 10 (Note 4)  
V (Pin 7) = 200mV, 0.1mA Out of Pin 13 (Note 4)  
2.4  
2.4  
3.5  
3.9  
V
V
OH  
Fast Comparator Output Low Voltage  
Slow Comparator Output Low Voltage  
V (Pin 9) = 200mV, 800µA Into Pin 10  
V (Pin 7) = 200mV, 800µA Into Pin 13  
0.35  
0.39  
0.5  
0.5  
V
V
OL  
2
LT1319  
ELECTRICAL CHARACTERISTICS  
TA = 25°C, V15 = 5V, V1 = V12 = 0V, V6 = V8 = V14 = 2V, unless otherwise specified.  
SYMBOL PARAMETER  
Threshold Transimpedance  
CONDITIONS  
100µA Into Pin 11 (Note 5)  
100µA Into Pin 11, V (Pin 11)  
MIN  
TYP  
2
MAX  
UNITS  
kΩ  
V
V
V
V
Threshold External Voltage  
Shutdown Input High Voltage  
Shutdown Input Low Voltage  
Shutdown Input High Current  
Shutdown Input Low Current  
Supply Current  
0.8  
2
0.9  
1.2  
TH  
IH  
IL  
V
V
0.8  
10  
130  
18  
I
I
I
I
V (Pin 14) = 2.4V  
V (Pin 14) = 0.4V  
140  
400  
10  
60  
260  
14  
µA  
µA  
mA  
µA  
IH  
IL  
V (Pin 14) = 2V  
S
Supply Current in Shutdown  
V (Pin 14) = 0.8V, V (Pin 6) = V (Pin 8) = 0V  
300  
500  
800  
SHDN  
0°C TA 70°C, V15 = 5V, V1 = V12 = 0V, V6 = V8 = V14 = 2V, unless otherwise specified.  
SYMBOL PARAMETER  
CONDITIONS  
MIN  
TYP  
MAX  
UNITS  
V
OS  
Preamp Input Offset Voltage  
Preamp Output Offset Voltage  
Preamp Loop Offset Voltage  
High Gain Loop Offset Voltage  
Low Gain Loop Offset Voltage  
V (Pin 2) – V (Pin 5)  
V (Pin 4) – V (Pin 5)  
V (Pin 3) – V (Pin 5)  
V (Pin 9) – V (Pin 5)  
V (Pin 7) – V (Pin 5)  
4
17  
27  
350  
1200  
1200  
mV  
mV  
mV  
mV  
mV  
10  
30  
400  
400  
150  
800  
800  
A
VP  
Preamp Transimpedance  
±10µA Into Pin 2, Measure V (Pin 4)  
8.5  
15  
18.5  
kΩ  
Preamp Output Swing, Positive  
Preamp Output Swing, Negative  
100µA Out of Pin 2, Measure V (Pin 4)  
100µA Into Pin 2, Measure V (Pin 4)  
0.2  
0.6  
0.4  
0.4  
0.6  
0.2  
V
V
Preamp Loop Rejection, Positive  
Preamp Loop Rejection, Negative  
50µA Into Pin 2, Measure V (Pin 4)  
50µA Out of Pin 2, Measure V (Pin 4)  
3.5  
3.5  
–1  
1
3.5  
3.5  
mV  
mV  
Preamp Loop Output Current, Positive  
Preamp Loop Output Current, Negative  
100µA Out of Pin 2, Measure I (Pin 3), (Note 1)  
100µA Into Pin 2, Measure I (Pin 3), (Note 1)  
160  
40  
100  
100  
40  
160  
µA  
µA  
V
V
Bias Voltage  
Bypass Voltage  
V (Pin 5)  
V (Pin 16)  
1.5  
4.7  
1.9  
4.9  
0.5  
0.45  
0.45  
2.3  
4.97  
1.6  
0.6  
0.3  
V
V
BIAS  
BYPASS  
I
Filter Buffer Input Bias Current  
Gain Stage Loop Rejection, Positive  
Gain Stage Loop Rejection, Negative  
I (Pin 6), I (Pin 8)  
V = 50mV (Pin 6, Pin 8), Measure V (Pin 7, Pin 9)  
V = 50mV (Pin 6, Pin 8), Measure V (Pin 7, Pin 9) 0.6  
0.05  
0.3  
µA  
V
V
B
V
V
Fast Comparator Output High Voltage  
Slow Comparator Output High Voltage  
V (Pin 9) = 200mV, 1mA Out of Pin 10 (Note 4)  
V (Pin 7) = 200mV, 0.1mA Out of Pin 13 (Note 4)  
2.4  
2.4  
3.5  
3.9  
V
V
OH  
Fast Comparator Output Low Voltage  
Slow Comparator Output Low Voltage  
V (Pin 9) = 200mV, 800µA Into Pin 10  
V (Pin 7) = 200mV, 800µA Into Pin 13  
0.35  
0.39  
0.5  
0.5  
V
V
OL  
V
V
V
Threshold External Voltage  
Shutdown Input High Voltage  
Shutdown Input Low Voltage  
Shutdown Input High Current  
Shutdown Input Low Current  
Supply Current  
100µA Into Pin 11, V (Pin 11)  
0.7  
2
0.9  
1.3  
V
V
TH  
IH  
IL  
0.8  
0
V
I
I
I
I
V (Pin 14) = 2.4V  
160  
450  
9
60  
260  
14  
µA  
µA  
mA  
µA  
IH  
V (Pin 14) = 0.4V  
V (Pin 14) = 2V  
80  
20  
IL  
S
Supply Current in Shutdown  
V (Pin 14) = 0.8V, V (Pin 6) = V (Pin 8) = 0V  
200  
500  
900  
SHDN  
Note 1: Measure V (Pin 3) without input current for Pin 2. Force Pin 3 to  
this measured voltage (which disables the preamp loop). Measure the  
current into and out of Pin 3 when Pin 2 is driven.  
Note 4: Measure V (Pin 7) and V (Pin 9). Force these voltages to 200mV  
below their nominal value to switch the comparators high.  
Note 5: The current into Pin 11 is multiplied by 4 and then applied to a  
500resistor on the positive comparator inputs. The threshold is  
I (Pin 11) • 4 • 500.  
Note 2: The gain is the differential voltage at the comparator inputs divided  
by the differential voltage between the filter buffer output and V  
parameter is not tested.  
. This  
BIAS  
Note 3: Hysteresis is the difference in comparator trip point measured  
when the output is high and when the output is low. This parameter is  
not tested.  
3
LT1319  
U W  
TYPICAL PERFORMANCE CHARACTERISTICS  
Preamp Highpass vs  
Gain Stage Highpass vs  
Capacitance on FILT2 or FILT2L  
Preamp Frequency Response vs  
Capacitance on FILT1  
Input Capacitance  
5
4
1000  
100  
10  
1000  
100  
10  
T
= 25°C  
T = 25°C  
A
T
= 25°C  
A
A
3
2
50pF  
10pF  
1
0
–1  
–2  
–3  
–4  
–5  
30pF  
10M  
1
0.1  
100  
1
100k  
1M  
100M  
1k  
10k  
100k  
1M  
1k  
10k  
100k  
1M  
10M  
FREQUENCY (Hz)  
HIGHPASS CORNER FREQUENCY (Hz)  
HIGHPASS CORNER FREQUENCY (Hz)  
1319 G01  
1319 G02  
1319 G03  
Input-Referred Noise vs  
Lowpass Filter on PREOUT  
FILTIN- or FILTINL- Referred  
Threshold Voltage vs RT1  
Preamp Output Noise vs  
Input Capacitance  
20  
15  
10  
5
1.0  
0.9  
0.8  
0.7  
0.6  
0.5  
250  
200  
150  
100  
50  
T
= 25°C  
T
= 25°C  
A
T = 25°C  
A
FILTER  
A
R
= 1k  
50pF  
30pF  
10pF  
0
0
0.1  
1
10  
20  
30  
(k)  
40  
10k  
100k  
1M  
FREQUENCY (Hz)  
10M  
100M  
FILTER CUTOFF FREQUENCY (MHz)  
R
T1  
1319 G04  
1319 G05  
1319 G06  
U
CIRCUIT DESCRIPTIO  
The LT1319 is a general purpose low noise, high speed,  
high gain, infrared receiver designed to easily provide IR  
communications with portable computers, PDAs, desktop  
computers and peripherals. The receiver takes the photo-  
current from an infrared photodiode (Siemens BPW34FA  
or Temic BPV22NF) and performs a current-to-voltage  
conversion. After external filtering that is tailored for the  
desired communication standard, two filter buffers are  
provided. There are dual gain chains with nominal gain of  
400V/Vthatfeedinternalcomparatorswithhysteresis. The  
comparatorthresholdsaresetexternallywithacurrentinto  
theVTHpin.Thehighfrequencycomparatorhasaresponse  
time of 25ns and is well-suited to high data rates.  
The low frequency comparator responds in 60ns and is  
useful for more modest data rates such as Sharp/Newton  
andIRDA-SIR.Thecircuitalsocontainsshutdowncircuitry  
to reduce power consumption. Rejection of ambient inter-  
ferenceisaccomplishedwithACcouplingloopsaroundthe  
preamp and the two gain stages. The rejection frequency is  
set with an internal resistor and an external capacitor to  
ground. This feature allows changing of the break fre-  
quencybysimplyswitchinginadditionalcapacitors. Toaid  
in rejection of power supply noise there is internal supply  
regulation and a fully differential topology after the filter  
buffers.  
4
LT1319  
W
BLOCK DIAGRA  
DS2  
DS1  
AN_GND  
1
BYPASS  
16  
+
C
B3  
10µF  
R
R
S3  
20k  
S5  
20k  
Q3  
R
R
R
S2  
FB  
S4  
V
5V  
CC  
15k  
20k  
20k  
R
S6  
Q2  
15  
1k  
+
0.1µF  
+
IPD  
C
IN  
2
C
B1  
B2  
Q4  
V
Q1  
10µF  
R
S1  
SHDN  
14  
PHOTO-  
DIODE  
20k  
PREAMP  
R
+
L1  
REG  
R
H1  
10k  
50k  
R
R
C1  
G1  
+
V
BIAS  
A1  
1k  
500Ω  
FILTER  
BUFFER  
+
+
+
+
1
DATAL  
13  
GM1  
A2  
= 20  
A3  
= 20  
R
R
C2  
500Ω  
G2  
FILT1  
3
COMP 1  
+
A
A
V
g
1k  
V
m
4k  
+
C
F1  
LOW FREQUENCY  
COMPARATOR  
10nF  
V
BIAS  
R
L2  
10k  
+
g
m
+
DIG_GND  
12  
1
PREOUT  
4
4k  
GM2  
V
BIAS  
5
R
R
F2  
F1  
2k  
1k  
5V  
+
C
R
R
B4  
T1  
SC  
V
TH  
L
1µF  
30k  
F1  
2k  
V
TH  
100µH  
11  
GEN  
+
C
T1  
FILTINL  
1µF  
6
R
H2  
50k  
+
C
F3  
FILT2L  
7
100pF  
R
R
C3  
G3  
+
A4  
1k  
500Ω  
+
C
FILTER  
BUFFER  
F4  
+
+
+
DATA  
10  
2.2nF  
A5  
= 20  
A6  
= 20  
R
R
C4  
500Ω  
G4  
COMP 2  
A
A
V
1k  
V
FILTIN  
8
HIGH FREQUENCY  
COMPARATOR  
V
GM3  
+
BIAS  
C
F2  
R
L3  
10k  
1nF  
+
g
m
+
1
4k  
FILT2  
9
+
C
F5  
1µF  
NOTE: EXTERNAL COMPONENTS ARE SHOWN FOR AN IRDA AND SHARP/NEWTON DATA RECEIVER.  
LT1319 • BD  
5
LT1319  
U
W U U  
APPLICATIONS INFORMATION  
ing the voltage noise gain. Referring to the Block Diagram,  
at frequencies beyond the corner frequency of the AC  
coupling loop, the preamp is in a noise gain of 2.5 due to  
the ratio of (RFB + RL1)/RL1. At high frequencies the input  
capacitanceapproachesthesameimpedanceasRL1 sothe  
noise gain increases. For example, at 500kHz the 30pF  
input capacitance looks like 10.6kwhich increases the  
noise gain to almost 4. The preamp is compensated to  
provideaflatcurrent-to-voltagefrequencyresponsewitha  
–3dB corner at 7MHz. The input current noise peaks up  
considerably if full bandwidth is used. To obtain best noise  
performance,theoutputofthepreampshouldbefilteredto  
the minimum bandwidth required for the desired modula-  
tion scheme. The graph of input-referred noise versus  
lowpass filtering on the preamp output shows the noise  
penalty for higher bandwidths.  
Layout and Passive Components  
TheLT1319requirescarefullayouttechniquestominimize  
parasitic signal coupling to the preamp input. A sample  
board layout for the circuit on the first page is shown in the  
Typical Application section. The lead lengths on the photo-  
diode must be as short as possible to Pin 2. Shielding is  
recommended over the entire circuit. A ground plane must  
be used and connected to Pin 1. The ground plane should  
extendunderthepackageandsurroundPins1to9andPin  
16. A single point connection should be made to the  
groundplaneatPin12(DIG_GND).TheleadsonPins6and  
8 should be short to prevent pickup into the gain stages.  
The comparator output leads (Pins 10 and 13) should be  
as short as possible to minimize coupling back to the input  
via parasitic capacitance.  
Capacitance on Pin 10 should be minimized as the com-  
parator output is pulled up by an internal 5k resistor. The  
associated digital circuitry should be located on the oppo-  
site side of the PC board from the LT1319 or separated as  
much as possible if on the same side of the board. Filter  
components should be located on the analog ground side  
of the package. Bypass capacitors should be used on Pins  
5, 11, 15 and 16 for best supply rejection.  
AC Coupling Loops  
There are three AC loops in the circuit that reject low  
frequency inputs. The first loop is around the preamp and  
provides rejection of ambient light sources. The operation  
can be explained by looking at the Block Diagram. For low  
frequency signals the transconductance amplifier, GM1,  
compares the preamp output to the VBIAS voltage. This  
differential voltage is transformed into a current that is fed  
into the high impedance node at Pin 3 and transformed  
back to a voltage. There is a voltage gain of approximately  
60dB to this point which is then buffered to drive a 10k  
resistor that is connected back to the input of the preamp.  
This high gain loop attenuates the effect of low frequency  
signalsbytheamountoftheloopgaintimestheratioofRL1  
to RFB (i.e., 1000V/V • 15/10 = 1500). For higher frequen-  
ciestheattenuationdecreasesduetotheexternalcapacitor  
onPin3. Atfrequenciesbeyondwheretheloopgainequals  
10/15, signals are no longer attenuated. This high fre-  
quency cutoff is at:  
Preamp  
The LT1319 preamp is a low noise, high speed current-to-  
voltage converter that has been optimized for an input  
capacitance of 30pF (which corresponds to the capaci-  
tance of the above-mentioned photodiodes with approxi-  
mately 2V of back bias). A range of 0pF to 50pF is  
acceptable. The amplifier obtains high bandwidth by pro-  
vidingalowimpedanceinputsothattheinputcurrentisnot  
filtered by the photodiode capacitance.  
The dynamic range of the circuit will be limited at the low  
end by the input-referred current noise of the preamplifier  
and the desired signal-to-noise ratio. At the other extreme  
ofthedynamicrangeforverylargeinputsignals,theoutput  
of the preamp is clamped by Schottky diodes across the  
feedback resistor.  
f = (15/10)/(2π • 4k• CPIN3  
)
where 1/(4k) is the transconductance of the loop ampli-  
fier. For example, if CPIN3 = 300pF, the highpass frequency  
is 200kHz which can aid in rejection of a wide range of  
ambient interference.  
The noise bandwidth is shaped by filtering at the output of  
the preamplifier and by the AC coupling loop. The input  
capacitance causes noise peaking for high bandwidth  
applications. Noise peaking can be explained by consider-  
The other two loops operate similarly around the gain  
stages and also provide low frequency rejection. In addi-  
6
LT1319  
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APPLICATIONS INFORMATION  
tion, the loops around the gain stages provide an accurate  
DC threshold setting for the comparators. At DC, the loops  
force the differential voltages at the output of the gain  
stages to zero. The comparator threshold is set by the  
currents provided by the VTH generator through the 500Ω  
resistors RC1 and RC3. These currents are equal to 4 times  
thecurrentintoPin11.For100µAintoPin11,thecompara-  
tor thresholds are nominally 200mV.  
pass filter network. The application on the first page of the  
datasheetisrepeatedintheBlockDiagramandcanbeused  
to illustrate the filtering for IRDA-SIR and Sharp/Newton.  
ThepreamphighpasszeroissetbyGM1andCF1.Thebreak  
frequency is located at:  
f = (15k/10k)/(2π • 4k• 10nF) = 6kHz  
Onthelowspeedchannelthereisalowpassfilterat800kHz  
set by RF2 and CF3. The gain stage has a highpass filter set  
by GM2 and CF4 at approximately 500kHz. The high speed  
channel has an LC tank circuit at 500kHz with Q = 3 set by  
RF1. The high speed gain stage has a highpass character-  
istic set by GM3 and CF5 with a break frequency of 1.1kHz.  
These filters are suitable for the 1.6µs pulses and up to  
115kBd data rates of IRDA-SIR on the slow channel. The  
fast channel is used for Sharp/Newton ASK Modulation  
with 500kHz bursts at data rates up to 38.4kBd.  
Power Supply Rejection and Biasing  
TheLT1319hasveryhighgainandbandwidthsogreatcare  
is taken to reduce false output transitions due to power  
supplynoise. AsafirststeptheVCC inputisregulateddown  
to approximately 4V to power all the analog sections of the  
circuitwhicharealsotiedtoAnalogGround(Pin1)asisthe  
substrate of the die. Additionally, the internal 4V is by-  
passedatPin16. Thedigitalcircuitry(thecomparatorsand  
shutdown logic) is powered directly off of VCC and is  
returned to Digital Ground (Pin 12). To provide a clean bias  
point for the preamp, filter buffers and the gain stages, a  
1.9V reference is generated from the 4V rail and is by-  
passed at Pin 5. The gain stages are pure differential  
designs which inherently reject supply variations.  
A second circuit is shown in the Typical Applications  
section for IRDA SIR/FIR and Sharp. This circuit is Demo  
Board 54. The first filter is a preamp highpass loop set at  
600Hz by CF7 for IRDA or 180kHz by CF1 for Sharp. Sharp  
modulation is run on the low speed channel and is next  
filtered by a tank circuit formed by RF2, LF1 and CF3 and  
centered at 500kHz. LF1 also provides the DC bias for the  
filter buffer input. A final highpass for the lower speed  
channel is set by CF4 at 130kHz. The high speed channel is  
usedbyIRDASIRandFIRwhichuse1.6µsand220nswide  
pulses. A lowpass formed by RF1 and CF2 limit the noise  
bandwidth. The final highpass is set by CF5 (2.5MHz for  
FIR)orCF6(450kHz).ThesquelchcircuitformedbyQ1,Q2,  
Q3 and RC1 to RC6 extends the short range performance  
and will be discussed later.  
Filtering  
Filtering is needed for two main reasons: sensitivity and  
ambient rejection. Lowpass filtering is needed to limit the  
bandwidth in order to minimize the noise. Low noise  
permits reliable detection of smaller input signals over a  
larger distance. Highpass filtering is used to reject interfer-  
ing ambient signals. Interference includes low frequency  
sources of infrared light such as sunlight, incandescent  
lights, and ordinary fluorescent lights, as well as high  
frequencysourcessuchasTVremotecontrols(40kHz)and  
high frequency fluorescent lighting (40kHz to 80kHz).  
In designing custom filters for different applications, the  
following guidelines should be used.  
1. Limit the noise bandwidth with a lowpass filter that has  
a rise time equal to half the pulse width. For example, for  
1µs pulses a 700kHz lowpass filter has a 10% to 90%  
rise time of 0.35/700kHz = 500ns.  
Thecircuittopologyallowsforfilteringbetweenthepream-  
plifier and the filter buffers as well as filtering with the three  
internalhighpassloops.Withtwochannelsthefilteringcan  
be optimized for different modulation schemes. The high  
speed channel (with a 25ns comparator) is ideal for modu-  
lation schemes using frequencies above 1MHz. Carrier-  
based methods as well as narrow pulse schemes can have  
superior ambient rejection by adding in a dedicated high-  
2. Limit the maximum highpass to 1/(4 • pulse width). For  
1µs pulses, 1/4µs = 250kHz.  
3. In setting the highpass filters, space the filters apart by  
a factor of 5 to 10 to reduce overshoot due to filter  
7
LT1319  
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APPLICATIONS INFORMATION  
interaction. Overshoot becomes especially important  
for high input levels because it can cause false pulses  
which may not be tolerated in certain modulation  
schemes. It is also more of a problem in modulation  
schemes such as IRDA-SIR and FIR where the duty  
cycle can get very low (i.e., transmitting data with lots of  
ones which are signaled with the absence of pulses). AC  
coupled receivers when faced with low duty cycle data  
set their thresholds close to the baseline DC level of the  
data stream which converts small overshoots into erro-  
neously received pulses.  
which translates to a photodiode current as follows (using  
the BPW34FA data sheet specs):  
2
7mm  
I
= 40mW/sr  
(
)
PD MIN  
(
)
2
)
1000mm  
(
0.65A / W 0.95 0.95 = 164nA  
)( )(  
(
)
The7mm2 termisthephotodiodearea. The1000mmisthe  
distance from the light source. The 0.65A/W is the spectral  
sensitivity at 880nm wavelength. The first 0.95 term is the  
relative sensitivity at 850nm wavelength and the second  
term is the sensitivity at 15° off axis. Similar calculations  
are detailed in the Infrared Data Association Serial Infrared  
(SIR) Physical Layer Link Specification, version 1.0. This  
minimum photocurrent implies that the input-referred  
noise current of the receiver be less than 13.7nA rms for a  
bit error rate of 1E-9. With an 800kHz lowpass filter on the  
preampoutputtheLT1319hasapproximately3.6nArmsof  
input-referred current noise. The maximum photodiode  
current at 20mm, on-axis with 500mW/sr intensity:  
4. As a general rule, place the lowest frequency highpass  
aroundthepreampandthehighesthighpassaroundthe  
gain stage or between the preamp and gain stage. The  
reason for this is again due to high signal levels where  
there can be slow photocurrent tails. The tail response  
can be filtered out by high enough frequency filters.  
5. Inallcaseswithcustomfiltering,orwhenmodifyingone  
of the applications presented in this data sheet, try the  
system over the full distance range with a full range of  
dutycycledatastreams. Modulationmethodswithfixed  
orlimiteddutycyclearesuperiorbecausetheyhavelittle  
or no data dependent problems.  
2
7mm  
Dynamic Range  
I
= 500mW/sr  
(
)
PD MAX  
(
)
2
20mm  
The calculation of dynamic range can only be made in the  
context of a specific modulation scheme and with the  
system variations taken into account. The required infor-  
mation includes: minimum signal-to-noise ratio (or BER,  
Bit Error Rate requirement), photodiode capacitance at  
1.9V back bias, preamp noise spectrum, preamp output  
filtering, AC loop cutoff frequencies, modulation method,  
demodulation method including allowable pulse widths  
and the effect of missing or extra pulses, photodiode rise  
and fall times, and ambient interference. The best solution  
istoexperimentallydeterminethemaximumandminimum  
distancesatwhichadesiredBERisobtained.Thismeasure  
ofdynamicrangeismoremeaningfulintermsoftheoverall  
system than any analytic solution.  
(
)
0.65A/ W 0.95 = 5.4mA  
)(  
(
)
so we see that the dynamic range requirement is 90.4dB.  
What is not obvious, however, is that the photodiode  
output current is not simply a pulse of current, there is a  
significanttailathighcurrentlevelsthathasatimeconstant  
of more than 1µs which can cause distortion in the output  
pulse width of the LT1319. This tail can be shown in the  
following photograph which shows the voltage across a 5k  
resistor that is connected between the anode of a photo-  
diode and ground. The cathode of the photodiode is  
connected to 2V. There is a 2pF Schottky diode across the  
resistor to clamp the voltage swing to less than 0.5V. With  
about 30pF photodiode capacitance and 10pF for an oscil-  
loscope probe, any tail observed with a time constant  
greater than 210ns is due to decaying photocurrent. The  
Using the IRDA-SIR modulation scheme as an example,  
however, we can illustrate how some limits on the required  
receiver/photodiode combination can be obtained. The  
minimum light intensity in the angular range is 40mW/sr  
8
LT1319  
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APPLICATIONS INFORMATION  
or nominally 0.68mV for RT1 = 30k. The largest practical  
value of RT1 is 39k. The limitation tends to be switching  
transients at the comparator outputs parasitically coupling  
to the FILTIN or FILTINL inputs and is layout dependent.  
first trace in the photograph shows the current with the  
photodiode 10cm from a source with 100mW/sr intensity.  
At 200mV/div, there is about 40µA of peak current and the  
decay is consistent with the 210ns time constant. The  
lower trace shows the current with the photodiode 2cm  
from the LEDs where the photodiode current is theoreti-  
cally25timesgreaterthanat10cm. Thevoltageisclamped  
by the photodiode to nearly 0.4V, but what is now notice-  
able is that there is a tail with a time constant a bit greater  
than 1µs. If the signal is AC coupled and has a low duty  
cycle, the waveform will be centered at the very bottom  
which can result in very wide output pulses. This issue will  
be discussed later in more detail and a method to circum-  
vent it will be shown.  
Extending Short Range Performance  
The short range performance of the LT1319 is normally  
limited by the photocurrent tail, but in some instances the  
peak current level cannot be supported by the output of the  
preamplifier and the input will sag at Pin 2. Typically the  
maximum input current is 6mA. To increase this current to  
20mAormore, placeanNPNtransistorwithitsemittertied  
to Pin 2, the base to Pin 4 and collector to the 5V supply.  
The choice of transistor is dependent on the bandwidth  
required for the preamp. The base-emitter capacitance of  
the transistor (CJE), is in parallel with the 15k feedback  
resistor of the preamplifier and performs a lowpass filter-  
ing function. For modest data rates such as IRDA-SIR and  
Sharp/Newton a 2N3904 limits the bandwidth to 2MHz  
which is ample. For the highest data rates, a transistor with  
fT greater than 1GHz is needed such as MMBR941LT1.  
Photocurrent Waveforms  
10cm  
Another issue with large input signals is the photocurrent  
tail. WhenthistailisACcoupledandthedatahasalowduty  
cycle, the output pulse width can become so wide that it  
extendsintothenextbitinterval.Ahighpassfiltercanreject  
thistail,butforthecaseofIRDA-SIR,rejectingthe1µstime  
constantcancauserejectionofthe1.6µspulsewhichleads  
toalossofsensitivityandreducedmaximumlinkdistance.  
Thecircuitonthefrontpageofthedatasheetusesa500kHz  
highpass that trades off some sensitivity for rejection of  
this tail. Unfortunately both maximum and minimum dis-  
tance are compromised. An alternative is shown in the  
IRDA-SIR/FIRapplication.Inthisinstancethefinalhighpass  
filter for SIR is moved into 450kHz, but a clamp/squelch  
circuitconsistingofQ1, Q2, D3andRC1 toRC6 isadded. Q1  
isusedasdescribedabovetoclamptheinput, buttheinput  
currentlevelatwhichtheclampengageshasbeenmodified  
by RC1 and RC2.  
2cm  
1319 AI01  
Threshold Adjustment  
The comparator thresholds are set by the current into Pin  
11. The simplest method of setting this current is by a  
resistor, RT1 tied between Pin 11 and Pin 15 (VCC). Pin 11  
should be bypassed. The current is given by:  
V 0.9V  
(
)
CC  
ITH =  
R + 2kΩ  
(
)
T1  
The threshold referred to the input of the filter buffer is:  
Without the resistors, Q1 would turn on when the voltage  
across the 15k resistor in the preamp reaches about 0.7V  
(a current of 0.7V/15k= 47µA). The drop across RC1  
reducesthisvoltagebyabout365mV.Thedropissetbythe  
I
• 4 • 500Ω  
400V/ V  
TH  
V
=
TH  
9
LT1319  
U
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APPLICATIONS INFORMATION  
current through RC2 which is [VCC – (VBIAS + 0.365V)]/  
15k= 182µA where VBIAS = 1.9V. At this new level  
(0.335V/15k= 22.3µA), Q1 turns on which clamps the  
preamp output. The collector current of Q1 provides base  
drive for Q2 which saturates and pulls its collector close to  
5V. The FILT1, FILT2L and FILT2 inputs are now pulled  
positive by RC3, RC4 and RC6 which forces an offset at the  
inputs to the gain stages and preamp. Referring to the  
Block Diagram, pulling FILT2L or FILT2 positive a voltage  
V provides a voltage of V/11 at the inverting input of the  
first gain stage. This offset effectively cuts off a portion of  
the tail at high input levels. The magnitude of V is set by  
the value of RC3, the current sinking capability of the  
transconductancestages(100µA),thevalueofCF4,CF5 and  
the duty cycle of the data pulses. Likewise an offset of  
V/10kis created at the preamp input to reduce tail  
current contributions.  
RF quality capacitor to reduce the high frequency spikes.  
The current must be selected to achieve the minimum  
output light intensity at a given angle and must be lower  
than the manufacturer’s maximum current rating at the  
maximum duty cycle of the modulation method. The opti-  
mum current is a function of the LED output, the LED  
forward voltage, the drop across the transistor and the  
minimum supply voltage.  
V VLED VSW  
(
)
CC  
ILED  
=
RSERIES  
The minimum light output then can be obtained from the  
LEDdatasheet.ForIRDA-SIRtheminimumintensityat15°  
off axis is 40mW/sr. For IRDA-FIR the spec rises to  
100mW/sr. To increase light output and distance of the  
link, a second LED can be inserted in series with the first to  
obtain twice the light output without consuming additional  
supply current. The current variation will now be greater  
becausetwoLEDforwarddropsmustbeaccountedforand  
the drop across the series resistor is greatly reduced.  
LED Drive Circuits  
There are several simple circuits for driving LEDs. For low  
speed modulation methods such as IRDA-SIR and Sharp/  
Newton with pulses over 1µs, a 2N3904 in a SOT-23  
packagecanbeusedasaswitchwithaseriesresistorinthe  
collector to limit the current drive. This circuit is shown  
below with a suggested limiting resistor of 16which  
typically sets the current at 200mA. The supply voltage  
mustbewellbypassedattheconnectiontotheLEDinorder  
for the supply not to sag when hit with a fast current pulse.  
A10µFlowESRcapacitorshouldbeusedaswellasa0.1µF  
For pulse widths less than 500ns the NPN should be  
replaced by an N-channel MOSFET with on-resistance of  
less than 1with 5V on the gate. The FET can turn off  
much more quickly than the saturated NPN and provides  
a lower effective on-resistance. A suggested circuit is  
shown below and includes three devices available in the  
SOT-23 package.  
U
TYPICAL APPLICATIONS  
LED Drive Circuit  
for IRDA-SIR and Sharp/Newton  
2 LED Drive Circuit  
for IRDA-FIR  
Optional Clamp Circuit  
V
V
CC  
V
CC  
CC  
HSDL4220  
TSH5400  
DN304  
HSDL4220  
TSH5400  
DN304  
2N3904 FOR <1MHz  
MMBR941LT1 FOR >1MHz  
R
F3  
16Ω  
R
3.9Ω  
D2  
R
470Ω  
PIN 2  
PIN 4  
PREOUT  
F4  
IN  
1319 TA03  
Q1  
2N3904  
R
D1  
100Ω  
V
IN  
Q1  
NDS351N  
TN0201T  
2N7002  
V
IN  
1319 TA04  
1319 TA05  
10  
LT1319  
U
TYPICAL APPLICATIONS  
IRDA-SIR/FIR and Sharp or TV Remote Data Receiver  
E1  
SHDN  
E2  
CC  
E3  
GND  
V
V
CC  
V
CC  
D2  
HSDL-4220  
R
C5  
1M  
R
D2  
R
C2  
15k  
Q2  
6.8  
R
C1  
2k  
MMBT3906LT1  
1/2W  
R
D1  
100Ω  
Q1  
R
C4  
10k  
E6  
TX  
MMBT941LT1  
Q3  
2N7002  
Q4  
2N7002  
R
D3  
10k  
R
D3  
BAS16  
C3  
10k  
R
C6  
1k  
DRIVER  
1
16  
BYPASS  
AN_GND  
C
B3  
2
15  
14  
13  
12  
11  
10  
9
V
IN  
CC  
10µF  
3
U1  
LT1319  
R
C
C
B2  
T1  
30k  
B1  
0.1µF  
SHDN  
FILT1  
10µF  
E4  
4
5
6
7
8
DATAL  
PREOUT  
SHARP OR  
TV DATA  
D1  
TEMIC  
BPV22NF  
DIG_GND  
V
BIAS  
R
F2  
1k  
R
F1  
1k  
L
F1  
100µH  
V
FILTINL  
FILT2L  
FILTIN  
TH  
DATA  
FILT2  
C
T1  
1µF  
E5  
IRDA-SIR/FIR  
DATA  
C
C
F4  
10nF  
DGND  
B4  
C
C
F3  
1nF  
C
F2  
33pF  
F1  
330pF  
C
F5  
470pF  
1µF  
V
V
CC  
C
C
CC  
F7  
F6  
AGND  
0.1µF  
2.7nF  
LT1319 • TA02  
1
2
1
2
R
S1  
5.1k  
R
S2  
5.1k  
IRDA  
SIR  
NOTES:  
1. FOR IRDA-SIR/FIR OR TV REMOTE,  
Q5 SHOULD BE TURNED ON WITH  
A HIGH LOGIC INPUT  
Q5  
Q6  
JMP1  
JMP2  
FIR  
MMBT3904LT1  
MMBT3904LT1  
SHARP  
3
3
2. FOR IRDA-SIR, Q6 SHOULD BE TURNED  
ON WITH A HIGH LOGIC INPUT  
3. FOR SHARP ASK, C = 1nF, L = 100µH  
4. FOR TV REMOTE, C = 33nF, L = 470µH  
DGND  
DGND  
F3 F1  
F3  
F1  
PC Board Layout for IRDA-SIR/FIR and Sharp or TV Remote Data Receiver  
COMPONENT  
TOP  
BOTTOM  
Information furnished by Linear Technology Corporation is believed to be accurate and reliable.  
However, no responsibility is assumed for its use. Linear Technology Corporation makes no represen-  
tationthattheinterconnectionofitscircuitsasdescribedhereinwillnotinfringeonexistingpatentrights.  
11  
LT1319  
U
Dimensions in inches (millimeters) unless otherwise noted.  
PACKAGE DESCRIPTION  
S Package  
16-Lead Plastic Small Outline (Narrow 0.150)  
(LTC DWG # 05-08-1610)  
0.386 – 0.394*  
(9.804 – 10.008)  
16  
15  
14  
13  
12  
11  
10  
9
0.150 – 0.157**  
(3.810 – 3.988)  
0.228 – 0.244  
(5.791 – 6.197)  
5
7
8
1
2
3
4
6
0.010 – 0.020  
(0.254 – 0.508)  
× 45°  
0.053 – 0.069  
(1.346 – 1.752)  
0.004 – 0.010  
(0.101 – 0.254)  
0.008 – 0.010  
(0.203 – 0.254)  
0° – 8° TYP  
0.050  
(1.270)  
TYP  
0.014 – 0.019  
(0.355 – 0.483)  
0.016 – 0.050  
0.406 – 1.270  
S16 0695  
*DIMENSION DOES NOT INCLUDE MOLD FLASH. MOLD FLASH  
SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE  
**DIMENSION DOES NOT INCLUDE INTERLEAD FLASH. INTERLEAD  
FLASH SHALL NOT EXCEED 0.010" (0.254mm) PER SIDE  
RELATED PARTS  
PART NUMBER  
DESCRIPTION  
COMMENTS  
LT1113  
Dual, Low Noise Precision JFET Input Op Amp  
4.5nV/Hz Input Voltage Noise  
LT1169  
Dual, Low Noise Picoampere Bias Current Op Amp  
Low Noise, High Speed Op Amp (A 10)  
JFET Input, 10pA Max  
LT1222  
500MHz Gain Bandwidth, External Comp Pin  
V
LT/GP 1095 2K REV A • PRINTED IN USA  
LINEAR TECHNOLOGY CORPORATION 1995  
Linear Technology Corporation  
1630 McCarthy Blvd., Milpitas, CA 95035-7417  
12  
(408) 432-1900 FAX: (408) 434-0507 TELEX: 499-3977  

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