LT6600CS8-20#TR [Linear]

LT6600-20 - Very Low Noise, Differential Amplifier and 20MHz Lowpass Filter; Package: SO; Pins: 8; Temperature Range: 0°C to 70°C;
LT6600CS8-20#TR
型号: LT6600CS8-20#TR
厂家: Linear    Linear
描述:

LT6600-20 - Very Low Noise, Differential Amplifier and 20MHz Lowpass Filter; Package: SO; Pins: 8; Temperature Range: 0°C to 70°C

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LT6600-20  
Very Low Noise, Differential  
Amplifier and 20MHz Lowpass Filter  
U
FEATURES  
DESCRIPTIO  
Programmable Differential Gain via Two External  
The LT®6600-20 combines a fully differential amplifier  
with a 4th order 20MHz lowpass filter approximating a  
Chebyshev frequency response. Most differential amplifi-  
ers require many precision external components to tailor  
gain and bandwidth. In contrast, with the LT6600-20, two  
externalresistorsprogramdifferentialgain, andthefilter’s  
20MHzcutofffrequencyandpassbandrippleareinternally  
set. The LT6600-20 also provides the necessary level  
shifting to set its output common mode voltage to accom-  
modate the reference voltage requirements of A/Ds.  
Resistors  
Adjustable Output Common Mode Voltage  
Operates and Specified with 3V, 5V, ±5V Supplies  
0.5dB Ripple 4th Order Lowpass Filter with 20MHz  
Cutoff  
76dB S/N with 3V Supply and 2VP-P Output  
Low Distortion, 2VP-P, 800Load  
2.5MHz: 83dBc 2nd, 88dBc 3rd  
20MHz: 63dBc 2nd, 64dBc 3rd  
Fully Differential Inputs and Outputs  
Using a proprietary internal architecture, the LT6600-20  
integrates an antialiasing filter and a differential amplifier/  
driver without compromising distortion or low noise  
performance. At unity gain the measured in band  
signal-to-noise ratio is an impressive 76dB. At higher  
gains the input referred noise decreases so the part can  
process smaller input differential signals without signifi-  
cantly degrading the output signal-to-noise ratio.  
SO-8 Package  
Compatible with Popular Differential Amplifier  
Pinouts  
U
APPLICATIO S  
High Speed ADC Antialiasing and DAC Smoothing in  
Networking or Cellular Base Station Applications  
The LT6600-20 also features low voltage operation. The  
differential design provides outstanding performance for  
a2VP-P signallevelwhilethepartoperateswithasingle3V  
supply.  
High Speed Test and Measurement Equipment  
Medical Imaging  
Drop-in Replacement for Differential Amplifiers  
, LTC and LT are registered trademarks of Linear Technology Corporation.  
The LT6600-20 is packaged in an SO-8 and is pin compat-  
ible with stand alone differential amplifiers.  
U
TYPICAL APPLICATIO  
An 8192 Point FFT Spectrum  
0
INPUT 5.9MHz  
–10  
A/D  
LTC1748  
LT6600-20  
5V  
2V  
f
P-P  
SAMPLE  
–20  
= 80MHz  
–30  
–40  
–50  
0.1µF  
5V  
R
402Ω  
IN  
3
+
1
7
2
8
V
49.9Ω  
49.9Ω  
4
–60  
–70  
+
+
V
MID  
D
A
IN  
18pF  
OUT  
V
–80  
0.01µF  
OCM  
5
–90  
V
IN  
+
V
CM  
V
R
6
IN  
402Ω  
–100  
–110  
–120  
1µF  
GAIN = 402/R  
IN  
20  
FREQUENCY (MHz)  
0
10  
30  
40  
66002 TA01a  
66002 TA01b  
66002f  
1
LT6600-20  
W W U W  
U
W
U
ABSOLUTE AXI U RATI GS  
(Note 1)  
PACKAGE/ORDER I FOR ATIO  
Total Supply Voltage................................................ 11V  
Operating Temperature Range (Note 6) ...–40°C to 85°C  
Specified Temperature Range (Note 7)....–40°C to 85°C  
Junction Temperature........................................... 150°C  
Storage Temperature Range ................. 65°C to 150°C  
Lead Temperature (Soldering, 10 sec).................. 300°C  
ORDER PART  
TOP VIEW  
NUMBER  
+
IN  
1
2
3
4
8
7
6
5
IN  
LT6600CS8-20  
LT6600IS8-20  
V
V
OCM  
MID  
+
V
V
+
OUT  
OUT  
S8 PART MARKING  
S8 PACKAGE  
8-LEAD PLASTIC SO  
660020  
600I20  
TJMAX = 150°C, θJA = 100°C/W  
Consult LTC Marketing for parts specified with wider operating temperature ranges.  
ELECTRICAL CHARACTERISTICS  
The denotes specifications that apply over the full operating temperature  
range, otherwise specifications are at TA = 25°C. Unless otherwise specified VS = 5V (V+ = 5V, V= 0V), RIN = 402, and RLOAD = 1k.  
PARAMETER  
Filter Gain, V = 3V  
CONDITIONS  
MIN  
– 0.4  
– 0.1  
– 0.2  
– 0.1  
0.8  
TYP  
0.1  
0
MAX  
0.5  
0.1  
0.5  
1.9  
1
UNITS  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
dB  
V
V
V
V
V
V
V
V
V
V
V
V
V
V
V
= 2V , f = DC to 260kHz  
P-P IN  
S
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
IN  
= 2V , f = 2MHz (Gain Relative to 260kHz)  
P-P IN  
= 2V , f = 10MHz (Gain Relative to 260kHz)  
0.1  
0.5  
0
P-P IN  
= 2V , f = 16MHz (Gain Relative to 260kHz)  
P-P IN  
= 2V , f = 20MHz (Gain Relative to 260kHz)  
P-P IN  
= 2V , f = 60MHz (Gain Relative to 260kHz)  
– 33  
– 50  
0
– 28  
P-P IN  
= 2V , f = 100MHz (Gain Relative to 260kHz)  
P-P IN  
Filter Gain, V = 5V  
= 2V , f = DC to 260kHz  
0.5  
– 0.1  
– 0.2  
– 0.3  
– 1.3  
0.5  
0.1  
0.4  
1.6  
0.6  
–28  
S
P-P IN  
= 2V , f = 2MHz (Gain Relative to 260kHz)  
0
P-P IN  
= 2V , f = 10MHz (Gain Relative to 260kHz)  
0.1  
0.4  
–0.4  
33  
50  
0.1  
P-P IN  
= 2V , f = 16MHz (Gain Relative to 260kHz)  
P-P IN  
= 2V , f = 20MHz (Gain Relative to 260kHz)  
P-P IN  
= 2V , f = 60MHz (Gain Relative to 260kHz)  
P-P IN  
= 2V , f = 100MHz (Gain Relative to 260kHz)  
P-P IN  
Filter Gain, V = ±5V  
= 2V , f = DC to 260kHz  
0.6  
0.4  
S
P-P IN  
Filter Gain, R = 100Ω  
V
V
V
= 2V , f = DC to 260kHz, V = 3V  
11.6  
11.5  
11.4  
12.1  
12.0  
11.9  
12.6  
12.5  
12.4  
dB  
dB  
dB  
IN  
IN  
IN  
IN  
P-P IN  
S
= 2V , f = DC to 260kHz, V = 5V  
P-P IN  
S
= 2V , f = DC to 260kHz, V = ±5V  
P-P IN  
S
Filter Gain Temperature Coefficient (Note 2)  
f
= 250kHz, V = 2V  
P-P  
780  
118  
ppm/C  
IN  
IN  
Noise  
Noise BW = 10kHz to 20MHz  
2.5MHz, 2V , R = 800Ω  
µV  
RMS  
Distortion (Note 4)  
2nd Harmonic  
3rd Harmonic  
83  
88  
dBc  
dBc  
P-P  
L
20MHz, 2V , R = 800Ω  
2nd Harmonic  
3rd Harmonic  
63  
64  
dBc  
dBc  
P-P  
L
Differential Output Swing  
Input Bias Current  
Measured Between Pins 4 and 5  
Average of Pin 1 and Pin 8  
V = 5V  
S
3.80  
3.75  
4.75  
4.50  
V
V
S
P-P DIFF  
P-P DIFF  
V = 3V  
– 95  
50  
µA  
66002f  
2
LT6600-20  
ELECTRICAL CHARACTERISTICS  
The denotes specifications that apply over the full operating temperature  
range, otherwise specifications are at TA = 25°C. Unless otherwise specified VS = 5V (V+ = 5V, V= 0V), RIN = 402, and RLOAD = 1k.  
PARAMETER  
CONDITIONS  
MIN  
TYP  
MAX  
UNITS  
Input Referred Differential Offset  
R
IN  
= 402Ω  
V = 3V  
5
10  
10  
25  
30  
35  
mV  
mV  
mV  
S
V = 5V  
S
V = ±5V  
S
R
IN  
= 100Ω  
V = 3V  
5
5
5
15  
17  
20  
mV  
mV  
mV  
S
V = 5V  
S
V = ±5V  
S
Differential Offset Drift  
10  
µV/°C  
Input Common Mode Voltage (Note 3)  
Differential Input = 500mV  
IN  
,
V = 3V  
0.0  
0.0  
–2.5  
1.5  
3.0  
1.0  
V
V
V
P-P  
S
R
= 100Ω  
V = 5V  
S
V = ±5V  
S
Output Common Mode Voltage (Note 5)  
Differential Input = 2V  
Pin 7 at Mid-Supply  
,
V = 3V  
1.0  
1.5  
–1.0  
1.5  
3.0  
2.0  
V
V
V
P-P  
S
V = 5V  
S
Common Mode Voltage at Pin 2  
V = ±5V  
S
Output Common Mode Offset  
(with Respect to Pin 2)  
V = 3V  
–35  
–40  
–55  
5
0
–5  
40  
40  
35  
mV  
mV  
mV  
S
V = 5V  
S
V = ±5V  
S
Common Mode Rejection Ratio  
66  
dB  
Voltage at V  
(Pin 7)  
V = 5  
S
2.46  
4.35  
2.51  
1.5  
2.55  
7.65  
V
V
MID  
S
V = 3  
V
V
Input Resistance  
Bias Current  
5.7  
kΩ  
MID  
V
= V = V /2  
V = 5V  
–15  
–10  
–3  
–3  
µA  
µA  
OCM  
OCM  
MID  
S
S
V = 3V  
S
Power Supply Current  
V = 3V, V = 5  
42  
46  
53  
56  
mA  
mA  
mA  
S
S
V = 3V, V = 5  
S
S
V = ±5V  
46  
S
Note 1: Absolute Maximum Ratings are those values beyond which the life  
of a device may be impaired.  
Note 2: This is the temperature coefficient of the internal feedback  
Note 5: Output common mode voltage is the average of the voltages at  
Pins 4 and 5. The output common mode voltage is equal to the voltage  
applied to Pin 2.  
resistors assuming a temperature independent external resistor (R ).  
Note 3: The input common mode voltage is the average of the voltages  
Note 6: The LT6600C-20 is guaranteed functional over the operating  
temperature range –40°C to 85°C.  
IN  
applied to the external resistors (R ). Specification guaranteed for  
Note 7: The LT6600C-20 is guaranteed to meet 0°C to 70°C specifications  
and is designed, characterized and expected to meet the extended  
temperature limits, but is not tested at –40°C and 85°C. The LT6600I-20  
is guaranteed to meet specified performance from –40°C to 85°C.  
IN  
R
IN  
100.  
Note 4: Distortion is measured differentially using a differential stimulus,  
The input common mode voltage, the voltage at Pin 2, and the voltage at  
Pin 7 are equal to one half of the total power supply voltage.  
66002f  
3
LT6600-20  
U W  
TYPICAL PERFOR A CE CHARACTERISTICS  
Amplitude Response  
Passband Gain and Phase  
Passband Gain and Group Delay  
10  
0
2
0
50  
45  
40  
35  
30  
25  
20  
15  
10  
5
2
0
95  
V
= 5V  
V
= 5V  
GAIN  
GAIN  
S
S
GAIN = 1  
= 25°C  
50  
GAIN = 1  
= 25°C  
T
A
T
A
–10  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
–90  
–2  
–2  
5
–4  
–4  
–40  
–85  
–130  
–175  
–220  
–265  
–310  
–355  
PHASE  
GROUP  
DELAY  
–6  
–6  
–8  
–8  
–10  
–12  
–14  
–16  
–18  
–10  
–12  
–14  
–16  
–18  
V
S
= 5V  
GAIN = 1  
= 25°C  
T
A
0
0.1  
1
10  
100  
0.5  
6.5  
12.5  
18.5  
24.5  
30.5  
0.5  
6.5  
12.5  
18.5  
24.5  
30.5  
FREQUENCY (MHz)  
FREQUENCY (MHz)  
FREQUENCY (MHz)  
66002 G01  
66002 G03  
66002 G02  
Passband Gain and Group Delay  
Output Impedance  
Common Mode Rejection Ratio  
100  
80  
75  
70  
65  
60  
55  
50  
45  
40  
35  
30  
14  
12  
10  
8
50  
45  
40  
35  
30  
25  
20  
15  
10  
5
INPUT = 1V  
P-P  
V
S
= 5V  
V
= 5V  
S
GAIN  
V
= 5V  
GAIN = 1  
= 25°C  
GAIN = 4  
= 25°C  
S
GAIN = 1  
= 25°C  
T
A
T
A
T
A
10  
1
GROUP  
DELAY  
6
4
2
0
–2  
–4  
–6  
0.1  
0
0.1  
1
10  
100  
0.5  
6.5  
12.5  
18.5  
24.5  
30.5  
0.1  
1
10  
100  
FREQUENCY (MHz)  
FREQUENCY (MHz)  
FREQUENCY (MHz)  
66002 G05  
66002 G06  
66002 G04  
Distortion vs Signal Level,  
VS = 3V  
Power Supply Rejection Ratio  
Distortion vs Frequency  
–40  
–50  
–60  
–70  
–80  
–90  
–40  
–50  
100  
90  
+
DIFFERENTIAL INPUT,  
2ND HARMONIC  
DIFFERENTIAL INPUT,  
3RD HARMONIC  
SINGLE-ENDED INPUT,  
2ND HARMONIC  
SINGLE-ENDED INPUT,  
3RD HARMONIC  
3RD HARMONIC  
10MHz INPUT  
V
V
TO DIFFOUT  
= 3V  
= 25°C  
V
= 3V  
S
R
= 800AT  
L
S
A
T
EACH OUTPUT  
GAIN = 1  
80  
2ND  
HARMONIC  
10MHz INPUT  
T
= 25°C  
70  
A
–60  
–70  
60  
50  
3RD  
40  
30  
20  
10  
0
HARMONIC  
V
= 2V  
= 3V  
IN  
S
L
P-P  
–80  
–90  
1MHz INPUT  
V
2ND HARMONIC  
1MHz INPUT  
R
= 800AT  
EACH OUTPUT  
GAIN = 1  
T
= 25°C  
A
–100  
–100  
0.1  
1
10  
100  
0
1
2
3
4
5
0.001  
0.01  
0.1  
1
10  
100  
FREQUENCY (MHz)  
INPUT LEVEL (V  
)
FREQUENCY (MHz)  
P-P  
66002 G07  
66002 G08  
66002 G09  
66002f  
4
LT6600-20  
U W  
TYPICAL PERFOR A CE CHARACTERISTICS  
Distortion vs Signal Level,  
VS = ±5V  
Distortion  
vs Input Common Mode Level  
Distortion  
vs Input Common Mode Level  
–40  
–50  
–40  
–50  
–40  
–50  
2V 1MHz INPUT  
2ND HARMONIC,  
10MHz INPUT  
3RD HARMONIC,  
10MHz INPUT  
2ND HARMONIC,  
1MHz INPUT  
2ND HARMONIC,  
= 3V  
2ND HARMONIC,  
P-P  
R
= 800AT  
V
S
V
= 3V  
L
S
EACH OUTPUT  
GAIN = 1  
3RD HARMONIC,  
= 3V  
3RD HARMONIC,  
= 3V  
V
V
S
S
T
A
= 25°C  
2ND HARMONIC,  
= 5V  
2ND HARMONIC,  
= 5V  
–60  
–70  
–60  
–70  
V
–60  
–70  
V
S
S
3RD HARMONIC,  
1MHz INPUT  
3RD HARMONIC,  
= 5V  
3RD HARMONIC,  
= 5V  
V
V
S
S
–80  
–90  
–80  
–90  
–80  
–90  
V
= ±5V  
S
L
R
= 800AT  
EACH OUTPUT  
GAIN = 1  
500mV 1MHz INPUT, GAIN = 4,  
L
P-P  
T
A
= 25°C  
R
= 800AT EACH OUTPUT  
–100  
–100  
–100  
0
1
2
3
4
5
–3  
–2  
–1  
0
1
2
3
–3  
–2  
–1  
0
1
2
3
INPUT LEVEL (V  
)
INPUT COMMON MODE VOTLAGE RELATIVE TO PIN 7 (V)  
INPUT COMMON MODE VOTLAGE RELATIVE TO PIN 7 (V)  
P-P  
66002 G10  
66002 G11  
66002 G12  
Distortion  
vs Output Common Mode  
–40  
2ND HARMONIC,  
V
= 3V  
S
–50  
–60  
3RD HARMONIC,  
= 3V  
V
S
2ND HARMONIC,  
= 5V  
V
S
3RD HARMONIC,  
= 5V  
–70  
V
S
2ND HARMONIC,  
= ±5V  
–80  
V
S
3RD HARMONIC,  
= ±5V  
V
S
–90  
–100  
–110  
2V 1MHz INPUT, GAIN = 1,  
L
P-P  
R
= 800AT EACH OUTPUT  
–1.5 –1 –0.5  
0
2
–2  
0.5  
1
1.5  
VOLTAGE PIN 2 TO PIN 7 (V)  
66002 G13  
Total Supply Current  
vs Total Supply Voltage  
Transient Response, Gain = 1  
60  
50  
+
T
T
= 85°C  
A
A
VOUT  
50mV/DIV  
40  
30  
= 25°C  
= –40°C  
T
DIFFERENTIAL  
INPUT  
200mV/DIV  
A
20  
10  
0
100ns/DIV  
66002 G15  
0
1
2
3
4
5
6
7
8
9
10  
TOTAL SUPPLY VOLTAGE (V)  
66002 G14  
66002f  
5
LT6600-20  
U
U
U
PI FU CTIO S  
INand IN+ (Pins 1, 8): Input Pins. Signals can be applied  
to either or both input pins through identical external  
resistors, RIN. The DC gain from differential inputs to the  
differential outputs is 402/RIN.  
supply applications, bypass Pin 3 to ground and Pin 6 to  
ground with a quality 0.1µF ceramic capacitor.  
OUT+ and OUT(Pins 4, 5): Output Pins. Pins 4 and 5 are  
the filter differential outputs. Each pin can drive a 100Ω  
and/or 50pF load.  
V
OCM (Pin 2): Is the DC Common Mode Reference Voltage  
for the 2nd Filter Stage. Its value programs the common  
mode voltage of the differential output of the filter. Pin 2 is  
a high impedance input, which can be driven from an  
external voltage reference, or Pin 2 can be tied to Pin 7 on  
the PC board. Pin 2 should be bypassed with a 0.01µF  
ceramiccapacitorunlessitisconnectedtoagroundplane.  
V+ and V(Pins 3, 6): Power Supply Pins. For a single  
3.3V or 5V supply (Pin 6 grounded) a quality 0.1µF  
ceramic bypass capacitor is required from the positive  
supply pin (Pin 3) to the negative supply pin (Pin 6). The  
bypass should be as close as possible to the IC. For dual  
V
MID (Pin 7): The VMID pin is internally biased at mid-  
supply, see block diagram. For single supply operation,  
the VMID pin should be bypassed with a quality 0.01µF  
ceramic capacitor to Pin 6. For dual supply operation, Pin  
7 can be bypassed or connected to a high quality DC  
ground. A ground plane should be used. A poor ground  
will increase noise and distortion. Pin 7 sets the output  
common mode voltage of the 1st stage of the filter. It has  
a 5.5kimpedance, and it can be overridden with an  
external low impedance voltage source.  
W
BLOCK DIAGRA  
R
IN  
+
+
V
IN  
IN  
V
OUT  
5
V
MID  
8
7
6
+
V
11k  
11k  
PROPRIETARY  
LOWPASS  
402  
FILTER STAGE  
200Ω  
V
OP AMP  
200Ω  
200Ω  
+
+
OCM  
V
V
OCM  
+
+
200Ω  
402Ω  
1
2
3
4
66002 BD  
+
+
V
V
IN  
IN  
OCM  
V
OUT  
R
IN  
66002f  
6
LT6600-20  
W U U  
APPLICATIO S I FOR ATIO  
U
Interfacing to the LT6600-20  
output voltage is 1.65V, and the differential output voltage  
is2VP-P forfrequenciesbelow20MHz.Thecommonmode  
output voltage is determined by the voltage at pin 2. Since  
pin 2 is shorted to pin 7, the output common mode is the  
mid-supply voltage. In addition, the common mode input  
voltage can be equal to the mid-supply voltage of Pin 7  
(see the Distortion vs Input Common Mode Level graphs  
in the Typical Performance Characteristics).  
The LT6600-20 requires two equal external resistors, RIN,  
to set the differential gain to 402/RIN. The inputs to the  
+
filter are the voltages VIN and VINpresented to these  
external components, Figure 1. The difference between  
VIN+ and VINis the differential input voltage. The average  
+
of VIN and VIN is the common mode input voltage.  
Similarly, the voltages VOUT+ and VOUTappearing at Pins  
4 and 5 of the LT6600-20 are the filter outputs. The  
Figure 2 shows how to AC couple signals into the  
LT6600-20. In this instance, the input is a single-ended  
signal. AC coupling allows the processing of single-ended  
or differential signals with arbitrary common mode levels.  
The 0.1µF coupling capacitor and the 402gain setting  
resistor form a high pass filter, attenuating signals below  
4kHz. Larger values of coupling capacitors will propor-  
tionally reduce this highpass 3dB frequency.  
+
+
difference between VOUT and VOUT is the differential  
output voltage. The average of VOUT and VOUT is the  
common mode output voltage.  
Figure 1 illustrates the LT6600-20 operating with a single  
3.3V supply and unity passband gain; the input signal is  
DCcoupled. Thecommonmodeinputvoltageis0.5V, and  
the differential input voltage is 2VP-P. The common mode  
3.3V  
0.1µF  
V
V
3
402Ω  
3
2
1
0
3
2
1
0
1
7
2
8
+
V
V
4
IN  
IN  
+
+
V
V
+
OUT  
OUT  
V
OUT  
LT6600-20  
+
V
IN  
0.01µF  
V
OUT  
5
+
402Ω  
6
t
t
66002 F01  
V
IN  
Figure 1  
3.3V  
3
0.1µF  
V
V
0.1µF  
0.1µF  
402Ω  
402Ω  
1
3
2
1
0
2
1
4
+
+
V
V
+
7
2
8
OUT  
OUT  
V
V
OUT  
LT6600-20  
+
V
0.01µF  
IN  
OUT  
0
t
+
5
V
+
IN  
6
–1  
66002 F02  
Figure 2  
62pF  
5V  
0.1µF  
V
V
3
100Ω  
1
+
3
3
V
4
IN  
+
+
V
V
OUT  
+
7
OUT  
OUT  
LT6600-20  
2
1
0
2
1
2
8
V
0.01µF  
OUT  
V
500mV (DIFF)  
P-P  
5
V
+
IN  
+
V
V
100Ω  
IN  
6
t
t
0
+
66002 F03  
2V  
IN  
62pF  
Figure 3  
66002f  
7
LT6600-20  
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APPLICATIO S I FOR ATIO  
In Figure 3 the LT6600-20 is providing 12dB of gain. The  
gain resistor has an optional 62pF in parallel to improve  
the passband flatness near 20MHz. The common mode  
output voltage is set to 2V.  
examples where impedance must be considered is the  
evaluation of the LT6600-20 with a network analyzer.  
Figure 5 is a laboratory setup that can be used to charac-  
terizetheLT6600-20usingsingle-endedinstrumentswith  
50source impedance and 50input impedance. For a  
unity gain configuration the LT6600-20 requires a 402Ω  
source resistance yet the network analyzer output is  
calibrated for a 50load resistance. The 1:1 transformer,  
53.6and 388resistors satisfy the two constraints  
above. The transformer converts the single-ended source  
into a differential stimulus. Similarly, the output of the  
LT6600-20 will have lower distortion with larger load  
resistance yet the analyzer input is typically 50. The 4:1  
turns (16:1 impedance) transformer and the two 402Ω  
resistors of Figure 5, present the output of the LT6600-20  
with a 1600differential load, or the equivalent of 800Ω  
to ground at each output. The impedance seen by the  
network analyzer input is still 50, reducing reflections in  
the cabling between the transformer and analyzer input.  
Use Figure 4 to determine the interface between the  
LT6600-20 and a current output DAC. The gain, or “trans-  
impedance,” is defined as A = VOUT/IIN. To compute the  
transimpedance, use the following equation:  
402 R1  
A =  
( )  
R1+R2  
(
)
By setting R1 + R2 = 402, the gain equation reduces to  
A = R1().  
The voltage at the pins of the DAC is determined by R1,  
R2, the voltage on Pin 7 and the DAC output current.  
Consider Figure 4 with R1 = 49.9and R2 = 348. The  
voltage at Pin 7 is 1.65V. The voltage at the DAC pins is  
given by:  
Differential and Common Mode Voltage Ranges  
R1  
R1R2  
R1+R2  
V
DAC = VPIN7  
+I •  
IN  
The differential amplifiers inside the LT6600-20 contain  
circuitry to limit the maximum peak-to-peak differential  
voltage through the filter. This limiting function prevents  
excessive power dissipation in the internal circuitry  
and provides output short-circuit protection. The limiting  
function begins to take effect at output signal levels above  
2VP-P and it becomes noticeable above 3.5VP-P. This is  
illustrated in Figure 6; the LT6600-20 was configured with  
unity passband gain and the input of the filter was driven  
with a 1MHz signal. Because this voltage limiting takes  
place well before the output stage of the filter reaches the  
R1+R2 + 402  
= 26mV +I • 48.3Ω  
IN  
IIN is IIN+ or IIN. The transimpedance in this example is  
50.4.  
Evaluating the LT6600-20  
The low impedance levels and high frequency operation of  
the LT6600-20 require some attention to the matching  
networks between the LT6600-20 and other devices. The  
previous examples assume an ideal (0) source imped-  
ance and a large (1k) load resistance. Among practical  
2.5V  
0.1µF  
CURRENT  
OUTPUT  
DAC  
3.3V  
COILCRAFT  
TTWB-16A  
4:1  
COILCRAFT  
TTWB-1010  
NETWORK  
ANALYZER  
SOURCE  
NETWORK  
ANALYZER  
INPUT  
0.1µF  
3
388Ω  
1:1  
1
7
2
8
402Ω  
4
+
3
R2  
R2  
I
I
50Ω  
IN  
1
7
2
8
LT6600-20  
4
53.6Ω  
50Ω  
+
V
V
+
OUT  
R1  
+
5
+
0.01µF  
LT6600-20  
402Ω  
388Ω  
6
0.1µF  
IN  
OUT  
66002 F05  
5
+
6
R1  
66002 F04  
2.5V  
Figure 5  
Figure 4  
66002f  
8
LT6600-20  
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APPLICATIO S I FOR ATIO  
20  
The LT6600-20 was designed to process a variety of input  
signals including signals centered around the mid-supply  
voltage and signals that swing between ground and a  
positive voltage in a single supply system (Figure 1). The  
range of allowable input common mode voltage (the  
average of VIN and VIN in Figure 1) is determined by  
the power supply level and gain setting (see Distortion vs  
Input Common Mode Level in the Typical Performance  
Characteristics).  
1dB PASSBAND GAIN  
COMPRESSION POINTS  
1MHz 25°C  
0
1MHz 85°C  
–20  
3RD HARMONIC  
85°C  
–40  
3RD HARMONIC  
+
25°C  
–60  
2ND HARMONIC  
–80  
25°C  
2ND HARMONIC  
85°C  
–100  
–120  
4
6
7
0
1
2
3
5
Common Mode DC Currents  
1MHz INPUT LEVEL (V  
)
P-P  
66002 F06  
In applications like Figure 1 and Figure 3 where the  
LT6600-20 not only provides lowpass filtering but also  
level shifts the common mode voltage of the input signal,  
DC currents will be generated through the DC path be-  
tweeninputandoutputterminals.Minimizethesecurrents  
to decrease power dissipation and distortion.  
Figure 6. Output Level vs Input Level,  
Differential 1MHz Input, Gain = 1  
supply rails, the input/output behavior of the IC shown in  
Figure 6 is relatively independent of the power supply  
voltage.  
Consider the application in Figure 3. Pin 7 sets the output  
common mode voltage of the 1st differential amplifier  
insidetheLT6600-20(seetheBlockDiagramsection)at  
2.5V. Since the input common mode voltage is near 0V,  
there will be approximately a total of 2.5V drop across the  
series combination of the internal 402feedback resistor  
and the external 100input resistor. The resulting 5mA  
common mode DC current in each input path, must be  
The two amplifiers inside the LT6600-20 have indepen-  
dent control of their output common mode voltage (see  
theblockdiagramsection). Thefollowingguidelineswill  
optimize the performance of the filter.  
Pin 7 must be bypassed to an AC ground with a 0.01µF or  
largercapacitor. Pin7canbedrivenfromalowimpedance  
source, provided it remains at least 1.5V above Vand at  
least 1.5V below V+. An internal resistor divider sets the  
voltage of Pin 7. While the internal 11k resistors are well  
matched, their absolute value can vary by ±20%. This  
should be taken into consideration when connecting an  
external resistor network to alter the voltage of Pin 7.  
+
absorbed by the sources VIN and VIN. Pin 2 sets the  
common mode output voltage of the 2nd differential  
amplifier inside the LT6600-20, and therefore sets the  
common mode output voltage of the filter. Since, in the  
example of Figure 3, Pin 2 differs from Pin 7 by 0.5V, an  
additional2.5mA(1.25mAperside) ofDCcurrentwillflow  
in the resistors coupling the 1st differential amplifier  
output stage to filter output. Thus, a total of 12.5mA is  
used to translate the common mode voltages.  
Pin 2 can be shorted to Pin 7 for simplicity. If a different  
common mode output voltage is required, connect Pin 2  
to a voltage source or resistor network. For 3V and 3.3V  
supplies the voltage at Pin 2 must be less than or equal to  
the mid supply level. For example, voltage (Pin 2) 1.65V  
on a single 3.3V supply. For power supply voltages higher  
than 3.3V the voltage at Pin 2 should be within the voltage  
of Pin 7 – 1V to the voltage of Pin 7 + 2V. Pin 2 is a high  
impedance input.  
A simple modification to Figure 3 will reduce the DC  
common mode currents by 36%. If Pin 7 is shorted to  
Pin 2 the common mode output voltage of both op amp  
stages will be 2V and the resulting DC current will be 8mA.  
Of course, by AC coupling the inputs of Figure 3, the  
common mode DC current can be reduced to 2.5mA.  
66002f  
9
LT6600-20  
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APPLICATIO S I FOR ATIO  
2.5V  
Noise  
0.1µF  
SPECTRUM  
ANALYZER  
INPUT  
ThenoiseperformanceoftheLT6600-20canbeevaluated  
with the circuit of Figure 7.  
COILCRAFT  
TTWB-1010  
1:1  
R
R
3
IN  
IN  
V
IN  
1
7
2
8
25Ω  
4
+
LT6600-20  
Given the low noise output of the LT6600-20 and the 6dB  
attenuation of the transformer coupling network, it is  
necessary to measure the noise floor of the spectrum  
analyzer and subtract the instrument noise from the filter  
noise measurement.  
50Ω  
5
+
25Ω  
0.1µF  
6
66002 F07  
2.5V  
Example: With the IC removed and the 25resistors  
grounded, Figure 7, measure the total integrated noise  
(eS) of the spectrum analyzer from 10kHz to 20MHz. With  
the IC inserted, the signal source (VIN) disconnected, and  
the input resistors grounded, measure the total integrated  
noise out of the filter (eO). With the signal source con-  
nected, set the frequency to 1MHz and adjust the ampli-  
tude until VIN measures 100mVP-P. Measure the output  
amplitude, VOUT, and compute the passband gain  
A = VOUT/VIN. Now compute the input referred integrated  
noise (eIN) as:  
Figure 7  
50  
250  
V
= 5V  
S
40  
30  
20  
10  
0
200  
150  
100  
50  
SPECTRAL DENSITY  
INTEGRATED  
0
0.1  
1
10  
100  
(eO)2 (eS)2  
FREQUENCY (MHz)  
66002 F08  
eIN =  
A
Figure 8. Input Referred Noise, Gain = 1  
Table 1 lists the typical input referred integrated noise for  
various values of RIN.  
noisepoweraddedtogether,theresultingcalculatednoise  
level will be higher than the true differential noise.  
Figure 8 is plot of the noise spectral density as a function  
of frequency for an LT6600-20 with RIN = 402using the  
fixture of Figure 7 (the instrument noise has been sub-  
tracted from the results).  
Power Dissipation  
The LT6600-20 amplifiers combine high speed with large-  
signal currents in a small package. There is a need to  
ensure that the die junction temperature does not exceed  
150°C. TheLT6600-20packagehasPin6fusedtothelead  
frame to enhance thermal conduction when connecting to  
a ground plane or a large metal trace. Metal trace and  
plated through-holes can be used to spread the heat  
generated by the device to the backside of the PC board.  
Forexample,ona3/32"FR-4boardwith2ozcopper,atotal  
of 660 square millimeters connected to Pin 6 of the  
LT6600-20(330squaremillimetersoneachsideofthePC  
board) will result in a thermal resistance, θJA, of about  
85°C/W. WithouttheextrametaltraceconnectedtotheV–  
pin to provide a heat sink, the thermal resistance will be  
around 105°C/W. Table 2 can be used as a guide when  
Table 1. Noise Performance  
INPUT REFERRED  
PASSBAND  
GAIN (V/V)  
INTEGRATED NOISE  
10kHz TO 20MHz  
INPUT REFERRED  
NOISE dBm/Hz  
R
IN  
4
2
1
100Ω  
200Ω  
402Ω  
42µV  
–148  
–143  
–139  
RMS  
67µV  
RMS  
118µV  
RMS  
The noise at each output is comprised of a differential  
component and a common mode component. Using a  
transformerorcombinertoconvertthedifferentialoutputs  
tosingle-endedsignalrejectsthecommonmodenoiseand  
gives a true measure of the S/N achievable in the system.  
Conversely,ifeachoutputismeasuredindividuallyandthe  
considering thermal resistance.  
66002f  
10  
LT6600-20  
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APPLICATIO S I FOR ATIO  
Table 2. LT6600-20 SO-8 Package Thermal Resistance  
For a given supply voltage, the worst-case power dissi-  
pation occurs when the differential input signal is maxi-  
mum, the common mode currents are maximum (see  
Applications Information regarding common mode DC  
currents), the load impedance is small and the ambient  
temperature is maximum. To compute the junction tem-  
perature, measure the supply current under these worst-  
case conditions, estimate the thermal resistance from  
Table2, thenapplytheequationforTJ. Forexample, using  
the circuit in Figure 3 with a DC differential input voltage  
of 250mV, a differential output voltage of 1V, no load  
resistance and an ambient temperature of 85°C, the  
supply current (current into Pin 3) measures 55.5mA.  
Assuming a PC board layout with a 35mm2 copper trace,  
theθJA is100°C/W. Theresultingjunctiontemperatureis:  
COPPER AREA  
TOPSIDE BACKSIDE BOARD AREA  
THERMAL RESISTANCE  
(JUNCTION-TO-AMBIENT)  
2
2
2
(mm )  
(mm )  
(mm )  
1100  
330  
35  
1100  
330  
35  
2500  
2500  
2500  
2500  
2500  
65°C/W  
85°C/W  
95°C/W  
35  
0
100°C/W  
0
0
105°C/W  
Junction temperature, TJ, is calculated from the ambient  
temperature, TA, and power dissipation, PD. The power  
dissipation is the product of supply voltage, VS, and  
supply current, IS. Therefore, the junction temperature is  
given by:  
TJ = TA + (PD θJA) = TA + (VS • IS θJA)  
TJ = TA + (PD θJA) = 85 + (5 • 0.0555 • 100) = 113°C  
where the supply current, IS, is a function of signal level,  
load impedance, temperature and common mode  
voltages.  
When using higher supply voltages or when driving small  
impedances, more copper may be necessary to keep TJ  
below 150°C.  
U
PACKAGE DESCRIPTIO  
S8 Package  
8-Lead Plastic Small Outline (Narrow .150 Inch)  
(Reference LTC DWG # 05-08-1610)  
.189 – .197  
(4.801 – 5.004)  
.045 ±.005  
NOTE 3  
.050 BSC  
7
5
8
6
.245  
MIN  
.160 ±.005  
.150 – .157  
(3.810 – 3.988)  
NOTE 3  
.228 – .244  
(5.791 – 6.197)  
.030 ±.005  
TYP  
1
3
4
2
RECOMMENDED SOLDER PAD LAYOUT  
.010 – .020  
(0.254 – 0.508)  
× 45°  
.053 – .069  
(1.346 – 1.752)  
.004 – .010  
(0.101 – 0.254)  
.008 – .010  
(0.203 – 0.254)  
0°– 8° TYP  
.016 – .050  
(0.406 – 1.270)  
.050  
(1.270)  
BSC  
.014 – .019  
(0.355 – 0.483)  
TYP  
NOTE:  
INCHES  
1. DIMENSIONS IN  
(MILLIMETERS)  
2. DRAWING NOT TO SCALE  
3. THESE DIMENSIONS DO NOT INCLUDE MOLD FLASH OR PROTRUSIONS.  
MOLD FLASH OR PROTRUSIONS SHALL NOT EXCEED .006" (0.15mm)  
SO8 0303  
66002f  
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  
LT6600-20  
U
TYPICAL APPLICATIO  
A 5th Order, 20MHz Lowpass Filter  
+
V
0.1µF  
3
R
R
R
1
7
2
8
+
V
V
IN  
IN  
4
+
V
V
+
OUT  
OUT  
LT6600-20  
C
R
5
+
0.1µF  
6
1
C =  
2π • R • 20MHz  
66002 TA02a  
402Ω  
2R  
GAIN =  
, MAXIMUM GAIN = 4  
V
Amplitude Response  
Transient Response, Gain = 1  
10  
0
–10  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
–90  
+
VOUT  
50mV/DIV  
DIFFERENTIAL  
INPUT  
200mV/DIV  
V
= ±2.5V  
S
GAIN = 1  
C = 39pF  
R = 200Ω  
T
A
= 25°C  
100ns/DIV  
66002 TA03  
0.1  
1
10  
100  
FREQUENCY (MHz)  
66002 TA04  
RELATED PARTS  
PART NUMBER  
LTC®1565-31  
LTC1566-1  
LT1567  
DESCRIPTION  
COMMENTS  
650kHz Linear Phase Lowpass Filter  
Low Noise, 2.3MHz Lowpass Filter  
Continuous Time, SO8 Package, Fully Differential  
Continuous Time, SO8 Package  
Very Low Noise, High Frequency Filter Building Block  
Very Low Noise, 4th Order Building Block  
1.4nV/Hz Op Amp, MSOP Package, Fully Differential  
LT1568  
Lowpass and Bandpass Filter Designs Up to 10MHz,  
Differential Outputs  
LT6600-2.5  
LT6600-10  
Very Low Noise Differential Amplifier and 2.5MHz  
Lowpass Filter  
86dB S/N with 3V Supply, SO-8  
Very Low Noise Differential Amplifier and 10MHz  
Lowpass Filter  
82dB S/N with 3V Supply, SO-8  
66002f  
LT/TP 0503 1K • PRINTED IN USA  
12 LinearTechnology Corporation  
1630 McCarthy Blvd., Milpitas, CA 95035-7417  
(408) 432-1900 FAX: (408) 434-0507 www.linear.com  
LINEAR TECHNOLOGY CORPORATION 2003  

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