THS6007CPWPRG4 [TI]

IC,LINE TRANSCEIVER,2 DRIVER,2 RCVR,TSSOP,28PIN,PLASTIC;
THS6007CPWPRG4
型号: THS6007CPWPRG4
厂家: TEXAS INSTRUMENTS    TEXAS INSTRUMENTS
描述:

IC,LINE TRANSCEIVER,2 DRIVER,2 RCVR,TSSOP,28PIN,PLASTIC

驱动 光电二极管 驱动器
文件: 总35页 (文件大小:659K)
中文:  中文翻译
下载:  下载PDF数据表文档文件
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
PWP PACKAGE  
(TOP VIEW)  
ADSL Differential Line Driver and Receiver  
Driver Features  
– 140 MHz Bandwidth (–3dB) With  
25-Load  
– 1300 V/µs Slew Rate, G = 5  
– 400 mA Output Current Minimum Into  
25-Load  
1
28  
27  
26  
25  
24  
23  
22  
21  
20  
19  
18  
17  
16  
15  
R1 OUT  
R1 IN–  
R1 IN+  
NC  
R V  
CC+  
2
R2 OUT  
R2 IN–  
R2 IN+  
NC  
3
4
5
NC  
– –72 dBc 3rd Order Harmonic Distortion  
6
R V  
D V  
NC  
CC–  
CC–  
at f = 1 MHz, 25-Load, and 20 V  
7
D V  
O(PP)  
CC–  
8
D1 OUT  
NC  
D2 OUT  
NC  
Receiver Features  
– 175 MHz Bandwidth (–3dB)  
– 230 V/µs Slew Rate  
9
10  
11  
12  
13  
14  
D V  
D V  
CC+  
CC+  
D1 IN+  
D1 IN–  
NC  
D2 IN+  
D2 IN–  
NC  
79 dBc Total Harmonic Distortion at  
f = 1 MHz, R 1 kΩ  
L
– Quiescent Current = 3.4 mA Per Channel  
Wide Supply Range ±4.5 V to ±16 V  
Available in the PowerPAD Package  
NC  
NC  
NC – No internal connection  
description  
The THS6007 contains two high-current, high-speed drivers and two low-power, high-speed receivers. These  
drivers and receivers can be configured differentially for driving and receiving signals over low-impedance lines.  
The THS6007 is ideally suited for asymmetrical digital subscriber line (ADSL) applications where it supports  
the high-peak voltage and current requirements of that application. The drivers are current feedback amplifiers  
designed for the high slew rates necessary to support low total harmonic distortion (THD) in ADSL applications.  
The receivers are traditional voltage feedback amplifiers designed for maximum flexibility while consuming only  
3.4 mA per channel quiescent current. Separate power supply connections for each driver and both receivers  
are provided to minimize crosstalk.  
The THS6007 is packaged in the patented PowerPAD package. This package provides outstanding thermal  
characteristics in a small footprint package, which is fully compatible with automated surface-mount assembly  
procedures. Theexposedthermalpadontheundersideofthepackageisindirectcontactwiththedie. Bysimply  
soldering the pad to the PWB copper and using other thermal outlets, the heat is conducted away from the  
junction.  
AVAILABLE OPTIONS  
PACKAGED DEVICE  
EVALUATION  
T
A
PowerPAD TSSOP  
(PWP)  
MODULE  
0°C to 70°C  
THS6007CPWP  
THS6007IPWP  
THS6007EVM  
40°C to 85°C  
The PWP packages are available taped and reeled. Add an R suffix to the device type (i.e.,  
THS6007PWPR)  
CAUTION: The THS6007 provides ESD protection circuitry. However, permanent damage can still occur if this device is subjected  
to high-energy electrostatic discharges. Proper ESD precautions are recommended to avoid any performance degradation or loss  
of functionality.  
Please be aware that an important notice concerning availability, standard warranty, and use in critical applications of  
Texas Instruments semiconductor products and disclaimers thereto appears at the end of this data sheet.  
PowerPAD is a trademark of Texas Instruments.  
Copyright 2000, Texas Instruments Incorporated  
PRODUCTION DATA information is current as of publication date.  
Products conform to specifications per the terms of Texas Instruments  
standard warranty. Production processing does not necessarily include  
testing of all parameters.  
1
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
absolute maximum ratings over operating free-air temperature (unless otherwise noted)  
Supply voltage, V  
to V  
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 33 V  
CC–  
CC+  
Input voltage, V (driver and receiver) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±V  
I
CC  
Output current, I (driver) (see Note 1) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 800 mA  
O
Output current, I (receiver) (see Note 1) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 150 mA  
O
Differential input voltage, V (driver and receiver) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±4 V  
ID  
Maximum junction temperature, T . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 150°C  
Continuous total power dissipation at (or below) T = 25°C (see Note 1) . . . . . . . . . . . . . . . . . . . . . . . . . 4.48 W  
Operating free air temperature, T . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 40°C to 85°C  
Storage temperature, T  
J
A
A
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 65°C to 125°C  
stg  
Lead temperature, 1,6 mm (1/16 inch) from case for 10 seconds . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 300°C  
Stresses beyond those listed under “absolute maximum ratings” may cause permanent damage to the device. These are stress ratings only, and  
functional operation of the device at these or any other conditions beyond those indicated under “recommended operating conditions” is not  
implied. Exposure to absolute-maximum-rated conditions for extended periods may affect device reliability.  
NOTE 1: The THS6007 incorporates a PowerPad on the underside of the chip. This acts as a heatsink and must be connected to a thermal  
dissipation plane for proper power dissipation. Failure to do so can result in exceeding the maximum junction temperature, which could  
permanently damage the device. See the Thermal Information section of this document for more information about PowerPad  
technology.  
recommended operating conditions  
MIN  
±4.5  
9
TYP  
MAX  
±16  
32  
UNIT  
V
Split supply  
Supply voltage, V  
and V  
CC–  
CC+  
Single supply  
Operating free-air temperature, T  
40  
85  
°C  
A
2
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
functional block diagram  
Driver 1  
10  
D V  
+
CC  
11  
12  
D1 IN+  
D1 IN–  
+
8
D1 OUT  
_
7
D V  
D V  
+
CC  
Driver 2  
19  
CC  
18  
17  
+
D2 IN+  
D2 IN–  
21  
22  
D2 OUT  
_
D V  
CC  
Receiver 1  
28  
1
R V  
+
CC  
3
2
+
_
R1 IN+  
R1 IN–  
R1 OUT  
25  
26  
+
_
R2 IN+  
R2 IN–  
27  
6
R2 OUT  
R V  
CC  
Receiver 2  
3
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
DRIVER  
electrical characteristics, V  
= ±15 V, R = 25 , R = 1 k, T = 25°C (unless otherwise noted)  
CC  
L
F
A
dynamic performance  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
MAX  
UNIT  
V = 200 mV,  
G = 1,  
R = 25 Ω  
L
I
V
V
V
V
V
= ±15 V  
= ±5 V  
140  
CC  
CC  
CC  
CC  
CC  
R
= 680 ,  
F
V = 200 mV,  
G = 1,  
R = 25 Ω  
L
I
F
100  
120  
100  
315  
265  
30  
R
= 1 k,  
V = 200 mV,  
G = 2,  
R = 25 Ω  
L
I
F
= ±15 V  
= ±5 V  
R
= 620 ,  
Small-signal bandwidth (–3 dB)  
MHz  
V = 200 mV,  
G = 2,  
R = 820 Ω  
F
I
L
R
= 25 ,  
BW  
V = 200 mV,  
G = 1,  
R = 100 Ω  
L
I
F
= ±15 V  
= ±15 V  
R
= 820 ,  
V = 200 mV,  
G = 2,  
R = 100 Ω  
L
I
F
V
V
CC  
R
= 560 ,  
= ±5 V,  
= 820 Ω  
CC  
R
F
Bandwidth for 0.1 dB flatness  
V = 200 mV,  
I
G = 1  
MHz  
MHz  
V
R
= ±15 V,  
= 680 Ω  
CC  
40  
F
V
V
V
V
= ±15 V,  
= ±5 V,  
= ±15 V,  
= ±5 V,  
V
V
V
V
= 20 V  
= 4 V  
20  
35  
CC  
CC  
CC  
CC  
O(PP)  
O(PP)  
O
Full power bandwidth  
= 20 V  
,
G = 5  
G = 2  
G = 2  
1300  
900  
70  
(PP)  
SR  
Slew rate  
V/µs  
= 5 V  
,
(PP)  
O
t
s
Settling time to 0.1%  
0 V to 10 V Step,  
ns  
Full power bandwidth = slew rate/2π V  
.
O(Peak)  
Slew rate is measured from an output level range of 25% to 75%.  
noise/distortion performance  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
65  
79  
MAX  
UNIT  
V
V
= 20 V  
= 2 V  
V
= ±15 V,  
R
= 680 ,  
F
O(PP)  
CC  
G = 2,  
f = 1 MHz  
R = 680 ,  
F
O(PP)  
THD  
Total harmonic distortion  
dBc  
V
= ±5 V,  
CC  
G = 2,  
V
= 2 V  
76  
1.7  
O(PP)  
f = 1 MHz  
V
= ±5 V or ±15 V,  
f = 10 kHz,  
f = 10 kHz,  
CC  
G = 2,  
V
n
Input voltage noise  
nV/Hz  
pA/Hz  
Single-ended  
= ±5 V or ±15 V,  
Positive (IN+)  
Negative (IN–)  
11.5  
16  
V
G = 2  
CC  
I
n
Input noise current  
V
CC  
V
CC  
V
CC  
V
CC  
= ±5 V  
= ±15 V  
= ±5 V  
= ±15 V  
0.04%  
0.05%  
0.07°  
0.08°  
G = 2,  
NTSC,  
40 IRE Modulation  
A
Differential gain error  
D
R
= 150 ,  
L
G = 2,  
= 150 Ω,  
NTSC,  
40 IRE Modulation  
φ
D
Differential phase error  
Crosstalk  
R
L
Driver to driver V = 200 mV,  
f = 1 MHz  
62  
dB  
I
4
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
DRIVER  
electrical characteristics, V  
(continued)  
= ±15 V, R = 25 , R = 1 k, T = 25°C (unless otherwise noted)  
CC  
L
F
A
dc performance  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
1.5  
5
MAX  
UNIT  
V
= ±5 V  
CC  
Open loop transresistance  
MΩ  
V
V
V
V
= ±15 V  
CC  
T
= 25°C  
2
5
7
A
V
IO  
Input offset voltage  
= ±5 V or ±15 V  
= ±5 V or ±15 V,  
= ±5 V or ±15 V  
mV  
µV/°C  
mV  
CC  
CC  
CC  
T
A
= full range  
= full range  
= 25°C  
Input offset voltage drift  
T
A
20  
T
A
1.5  
4
5
Differential input offset voltage  
T
A
= full range  
= 25°C  
T
A
3
4
9
Negative  
Positive  
µA  
µA  
T
A
= full range  
= 25°C  
12  
10  
12  
8
T
A
I
IB  
Input bias current  
V
V
= ±5 V or ±15 V  
= ±5 V or ±15 V,  
CC  
T
A
= full range  
= 25°C  
T
A
1.5  
10  
Differential  
µA  
T
A
= full range  
= full range  
11  
Differential input offset voltage drift  
T
A
µV/°C  
CC  
NOTE: Full range = 40°C to 85°C  
input characteristics  
PARAMETER  
TEST CONDITIONS  
= ±5 V  
MIN  
TYP  
MAX  
UNIT  
V
V
±3.6  
±3.7  
CC  
V
ICR  
Common-mode input voltage range  
V
= ±15 V  
±13.4 ±13.5  
CC  
Common-mode rejection ratio  
Differential common-mode rejection ratio  
Input resistance  
62  
70  
100  
300  
1.4  
CMRR  
V
CC  
= ±5 V or ±15 V,  
T
A
= full range  
dB  
R
C
kΩ  
I
I
Differential input capacitance  
pF  
NOTE: Full range = 40°C to 85°C  
5
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
DRIVER  
electrical characteristics, V  
(continued)  
= ±15 V, R = 25 , R = 1 k, T = 25°C (unless otherwise noted)  
CC  
L
F
A
output characteristics  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
MAX  
UNIT  
3
to  
2.8  
3.2  
to  
–3  
V
CC  
V
CC  
V
CC  
V
CC  
= ±5 V  
= ±15 V  
= ±5 V  
= ±15 V  
Single ended  
Differential  
R
= 25 Ω  
V
L
L
11.8  
to  
–11.5  
12.5  
to  
–12.2  
V
O
Output voltage swing  
6
to  
5.6  
6.4  
to  
–6  
R
= 50 Ω  
V
23.6  
to  
23 24.4  
25  
to  
V
V
= ±5 V,  
R
R
= 5 Ω  
500  
CC  
L
L
I
I
Output current (see Note 2)  
mA  
O
= ±15 V,  
= 25 Ω  
400  
500  
800  
13  
CC  
Short-circuit output current (see Note 2)  
Output resistance  
mA  
OS  
R
Open loop  
O
NOTE 2: A heat sink is required to keep the junction temperature below absolute maximum when an output is heavily loaded or shorted. See  
absolute maximum ratings and Thermal Information section.  
power supply  
PARAMETER  
TEST CONDITIONS  
Split supply  
Single supply  
MIN  
±4.5  
9
TYP  
MAX  
±16.5  
33  
UNIT  
V
CC  
Power supply operating range  
V
V
= ±5 V  
T
= full range  
= 25°C  
A
12  
CC  
CC  
A
I
Quiescent current (each driver)  
Power supply rejection ratio  
T
11.5  
74  
72  
13  
mA  
CC  
V
= ±15 V  
T
A
= full range  
= 25°C  
15  
T
A
68  
65  
64  
62  
V
= ±5 V  
dB  
dB  
CC  
CC  
T
A
= full range  
= 25°C  
PSRR  
T
A
V
= ±15 V  
T
A
= full range  
NOTE: Full range = 40°C to 85°C  
6
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
RECEIVER  
electrical characteristics at T = 25°C, V  
= ±15 V, R = 150 (unless otherwise noted)  
L
A
CC  
dynamic performance  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
175  
160  
70  
MAX  
UNIT  
V
V
V
V
V
V
V
V
V
V
V
V
V
V
= ±15 V  
CC  
Gain = 1  
Gain = –1  
Gain = 1  
MHz  
= ±5 V  
= ±15 V  
= ±5 V  
= ±15 V  
= ±5 V  
CC  
Small-signal bandwidth (–3 dB)  
Bandwidth for 0.1 dB flatness  
CC  
MHz  
MHz  
MHz  
V/µs  
ns  
65  
CC  
BW  
SR  
35  
CC  
35  
CC  
= 20 V,  
= 5 V,  
V
V
= ±15 V  
= ±5 V  
2.7  
7.1  
230  
170  
43  
O(pp)  
O(pp)  
CC  
Full power bandwidth  
CC  
= ±15 V,  
= ±5 V,  
= ±15 V,  
= ±5 V,  
= ±15 V,  
= ±5 V,  
20-V step  
5-V step  
5-V step  
2-V step  
5-V step  
2-V step  
Gain = 5  
Gain = 1  
CC  
CC  
CC  
CC  
CC  
CC  
Slew rate  
Settling time to 0.1%  
Gain = –1  
Gain = –1  
30  
t
s
233  
280  
Settling time to 0.01%  
ns  
Full power bandwidth = slew rate/2π V  
.
O(Peak)  
Slew rate is measured from an output level range of 25% to 75%.  
noise/distortion performance  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
–79  
–77  
10  
MAX  
UNIT  
V
V
= ±15 V  
= ±5 V  
R
R
= 1 kΩ  
= 1 kΩ  
V
= 2 V,  
CC  
L
L
O(pp)  
f = 1 MHz, Gain = 2  
THD  
Total harmonic distortion  
dBc  
CC  
V
n
Input voltage noise  
V
CC  
V
CC  
V
CC  
= ±5 V or ±15 V, f = 10 kHz  
= ±5 V or ±15 V, f = 10 kHz  
= ±5 V or ±15 V, f = 1 MHz  
nV/Hz  
pA/Hz  
dB  
I
n
Input current noise  
0.7  
X
T
Receiver-to-receiver crosstalk  
–75  
dc performance  
PARAMETER  
TEST CONDITIONS  
MIN  
10  
9
TYP  
MAX  
UNIT  
T
= 25°C  
19  
A
V
V
= ±15 V,  
= ±5 V,  
V
= ±10 V,  
= ±2.5 V,  
R
= 1 kΩ  
V/mV  
CC  
O
L
L
T
A
= full range  
= 25°C  
Open loop gain  
T
A
8
16  
1
V
R
= 250 Ω  
V/mV  
CC  
O
T
A
= full range  
= 25°C  
7
T
A
7
8
V
OS  
Input offset voltage  
Offset voltage drift  
Input bias current  
mV  
µV/°C  
µA  
T
= full range  
= full range  
= 25°C  
A
A
T
A
15  
V
CC  
= ±5 V or ±15 V  
T
1.2  
6
8
I
I
IB  
T
A
= full range  
= 25°C  
T
A
20  
250  
400  
Input offset current  
Offset current drift  
nA  
OS  
T
A
= full range  
T
A
= full range  
0.3  
nA/°C  
NOTE: Full range = 40°C to 85°C  
7
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
RECEIVER  
electrical characteristics at T = 25°C, V = ±15 V, R = 150 (unless otherwise noted) (continued)  
A
CC  
L
input characteristics  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
MAX  
UNIT  
V
CC  
V
CC  
V
CC  
V
CC  
= ±15 V  
= ±5 V  
±13.8 ±14.1  
V
Common-mode input voltage range  
V
ICR  
±3.8  
78  
±3.9  
93  
= ±15 V,  
= ±5 V,  
V
V
= ±12 V,  
= ±2 V,  
T
= full range  
= full range  
dB  
dB  
ICR  
A
CMRR Common mode rejection ratio  
T
A
84  
90  
ICR  
R
C
Input resistance  
1
MΩ  
pF  
I
I
Input capacitance  
1.5  
NOTE: Full range = 40°C to 85°C  
output characteristics  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
MAX  
UNIT  
V
V
V
V
V
V
V
= ±15 V  
= ±5 V  
R
R
= 250 Ω  
= 150 Ω  
±12 ±13.6  
±3.4 ±3.8  
±13 ±13.8  
CC  
CC  
CC  
CC  
CC  
CC  
CC  
L
L
V
V
I
Output voltage swing  
O
= ±15 V  
= ±5 V  
R
R
= 1 kΩ  
= 20 Ω  
V
L
L
±3.5  
65  
±3.9  
85  
= ±15 V  
= ±5 V  
mA  
Output current  
O
50  
70  
I
Short-circuit current  
Output resistance  
= ±15 V  
100  
mA  
SC  
R
Open loop  
13  
O
Observe power dissipation ratings to keep the junction temperature below the absolute maximum rating when the output is heavily loaded or  
shorted. See the absolute maximum ratings section of this data sheet for more information.  
power supply  
PARAMETER  
TEST CONDITIONS  
MIN  
±4.5  
9
TYP  
MAX  
±16.5  
33  
UNIT  
Dual supply  
V
Supply voltage operating range  
Supply current (per amplifier)  
V
CC  
Single supply  
T
= 25°C  
3.4  
2.9  
90  
4.2  
A
V
= ±15 V  
= ±5 V  
CC  
T
A
= full range  
= 25°C  
5
I
mA  
dB  
CC  
T
A
3.7  
V
V
CC  
T
A
= full range  
= full range  
4.5  
PSRR Power supply rejection ratio  
= ±5 V or ±15 V  
T
A
79  
CC  
NOTE: Full range = 40°C to 85°C  
8
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
PARAMETER MEASUREMENT INFORMATION  
1 kΩ  
1 kΩ  
1 kΩ  
1 kΩ  
+
+
Driver 1  
Driver 2  
V
O
V
O
V
I
V
I
25 Ω  
25 Ω  
50 Ω  
50 Ω  
Figure 1. Driver Input-to-Output Crosstalk Test Circuit  
1 kΩ  
1 kΩ  
1 kΩ  
1 kΩ  
+
+
Receiver 1  
Receiver 2  
V
O
V
O
V
I
V
I
150 Ω  
150 Ω  
50 Ω  
50 Ω  
Figure 2. Receiver Input-to-Output Crosstalk Test Circuit  
R
R
f
g
15 V  
Driver  
V
O
+
V
I
R
25 Ω  
L
50 Ω  
–15 V  
Figure 3. Driver Test Circuit, Gain = 1 + (R /R )  
f
g
R
R
f
g
15 V  
Receiver  
V
O
V
I
+
R
150 Ω  
L
50 Ω  
–15 V  
Figure 4. Receiver Test Circuit, Gain = 1 + (R /R )  
f
g
9
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
TYPICAL CHARACTERISTICS  
Table of Graphs  
FIGURE  
5
vs Supply voltage  
Peak-to-peak output voltage  
Driver  
vs Load resistance  
vs Free-air temperature  
vs Free-air temperature  
vs Free-air temperature  
vs Frequency  
6
V
Input offset voltage  
Input bias current  
Driver  
Driver  
Driver  
Driver  
Driver  
Driver  
7
IO  
I
IB  
8
CMMR Common-mode rejection ratio  
9
Driver-to-driver crosstalk  
10  
PSSR  
Power supply rejection ratio  
vs Free-air temperature  
vs Frequency  
11  
Closed-loop output impedance  
12  
vs Supply voltage  
vs Free-air temperature  
vs Output step  
13  
I
Supply current  
Driver  
CC  
14  
SR  
Slew rate  
Driver  
Driver  
Driver  
Driver  
Driver  
Driver  
Driver  
Driver  
15, 16  
17  
V
Input voltage and current noise  
Normalized frequency response  
Output amplitude  
vs Frequency  
n
vs Frequency  
18, 19  
20 – 23  
24 – 27  
28, 29  
30, 31  
32, 33  
34, 35  
36, 37  
38  
vs Frequency  
Normalized output response  
Small and large signal frequency response  
vs Frequency  
vs Frequency  
Single-ended harmonic distortion  
Differential gain and phase  
vs Output voltage  
vs DC input offset voltage  
vs Number of 150-loads  
Driver  
400-mV step response  
10-V step response  
Driver  
Driver  
39  
20-V step response  
Driver  
40  
Driver-to-receiver crosstalk  
Receiver-to-driver crosstalk  
Power supply rejection ratio  
Open loop gain and phase response  
Receiver-to-receiver crosstalk  
Total harmonic distortion  
Settling  
Receiver  
Receiver  
Receiver  
Receiver  
Receiver  
Receiver  
Receiver  
Receiver  
vs Frequency  
vs Frequency  
vs Frequency  
vs Frequency  
vs Frequency  
vs Frequency  
vs Output step  
vs Frequency  
vs Output voltage  
vs Frequency  
vs Frequency  
41  
42  
43  
44  
45  
THD  
46, 47  
48  
PSSR  
Power supply rejection ratio  
49  
50, 51  
52 – 55  
56 – 67  
68, 70  
69  
Distortion  
Receiver  
Output amplitude  
2-V step response  
5-V step response  
20-V step response  
Input offset voltage  
Input bias current  
Receiver  
Receiver  
Receiver  
Receiver  
Receiver  
Receiver  
71  
V
IO  
vs Free-air temperature  
vs Free-air temperature  
vs Supply voltage  
72  
I
IB  
73  
74  
V
O
Output voltage  
Receiver  
vs Free-air temperature  
vs Supply voltage  
75  
V
ICR  
Common-mode input voltage  
Supply current  
Receiver  
Receiver  
Receiver  
76  
I
vs Supply voltage  
77  
CC  
V
I
Voltage and current noise  
vs Frequency  
78  
n, n  
10  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
TYPICAL CHARACTERISTICS (DRIVER)  
PEAK-TO-PEAK OUTPUT VOLTAGE  
INPUT OFFSET VOLTAGE  
vs  
PEAK-TO-PEAK OUTPUT VOLTAGE  
vs  
vs  
SUPPLY VOLTAGE  
FREE-AIR TEMPERATURE  
LOAD RESISTANCE  
15  
10  
5
15  
10  
2
1
T
R
R
= 25°C  
= 1 kΩ  
= 25 Ω  
A
F
L
G = 1  
V
= ±15 V  
CC  
R
= 1 kΩ  
F
V
= ±5 V  
Gain = 1  
CC  
0
V
= ±5 V  
= ±5 V  
CC  
CC  
5
0
T
R
= 25°C  
= 1 kΩ  
Gain = 1  
–1  
–2  
–3  
A
F
0
V
= ±15 V  
CC  
–5  
–10  
–15  
–5  
–10  
–15  
V
–4  
–5  
V
= ±15 V  
CC  
5
6
7
8
9
10 11 12 13 14 15  
10  
100  
1000  
–40 –20  
0
20  
40  
60  
80 100  
R
L
– Load Resistance – Ω  
V
– Supply Voltage – V  
T
A
– Free-Air Temperature – °C  
CC  
Figure 5  
Figure 6  
Figure 7  
INPUT BIAS CURRENT  
vs  
COMMON-MODE REJECTION RATIO  
DRIVER-TO-DRIVER CROSSTALK  
vs  
vs  
FREE-AIR TEMPERATURE  
FREE-AIR TEMPERATURE  
FREQUENCY  
5
4
3
–20  
–30  
–40  
–50  
–60  
–70  
–80  
–90  
80  
G = 1  
= 1 kΩ  
V
I
= ±15 V  
CC  
IB+  
V
V
= ± 15 V  
CC  
= 200 mV  
R
F
I
75  
70  
V
I
= ±5 V  
CC  
IB+  
Input = Driver 1  
Output = Driver 2  
V
= ±15 V  
CC  
2
1
0
1 kΩ  
V
= ±5 V  
1 kΩ  
1 kΩ  
CC  
V
I
= ±15 V  
V
= ±5 V  
CC  
IB–  
+
CC  
V
O
65  
60  
V
I
Input = Driver 2  
Output = Driver 1  
I
IB–  
1 kΩ  
–40 –20  
0
20  
40  
60  
80  
100  
100k  
1M  
10M  
100M  
–40 –20  
0
20  
40  
60  
80  
T
A
– Free-Air Temperature – °C  
T
A
– Free-Air Temperature – °C  
f – Frequency – Hz  
Figure 9  
Figure 10  
Figure 8  
POWER SUPPLY REJECTION RATIO  
CLOSED-LOOP OUTPUT IMPEDANCE  
vs  
SUPPLY CURRENT  
vs  
vs  
FREE-AIR TEMPERATURE  
FREQUENCY  
SUPPLY VOLTAGE  
100  
12  
11  
10  
95  
V
R
= ±15 V  
CC  
= 1 kΩ  
G = 1  
= 1 kΩ  
T
R
= 25°C  
= 1 kΩ  
Gain = +1  
A
F
R
F
F
90  
85  
80  
75  
Gain = 2  
10  
1
T
= 25°C  
A
V
= 1 V  
I(PP)  
9
V
= 15 V  
= –5 V  
CC  
V
= 5 V  
CC  
8
7
6
5
V
0.1  
O
1 kΩ  
V
1 kΩ  
CC  
1 kΩ  
V
I
+
0.01  
1000  
V
= –15 V  
CC  
70  
65  
50 Ω  
V
I
Z
=
– 1  
o
)
(
V
O
0.001  
5
6
7
8
9
10 11 12 13 14 15  
–40 –20  
0
20  
40  
60  
80  
100  
100k  
1M  
10M  
100M  
500M  
f – Frequency – Hz  
± V  
– Supply Voltage – V  
CC  
T
A
– Free-Air Temperature – °C  
Figure 12  
Figure 13  
Figure 11  
11  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
TYPICAL CHARACTERISTICS (DRIVER)  
SLEW RATE  
SLEW RATE  
vs  
SUPPLY CURRENT  
vs  
vs  
OUTPUT STEP  
OUTPUT STEP  
FREE-AIR TEMPERATURE  
1500  
1000  
900  
800  
700  
600  
500  
400  
300  
200  
100  
13  
12  
10  
8
V
= ± 15V  
CC  
Gain = 5  
V
= ± 5V  
CC  
Gain = 2  
V
= ±15 V  
CC  
1300  
1100  
+SR  
+SR  
R
R
= 1 kΩ  
= 25 Ω  
F
L
R
R
= 1 kΩ  
F
L
= 25 Ω  
–SR  
V
= ±5 V  
–SR  
CC  
900  
700  
6
500  
300  
4
2
0
100  
0
20  
–40 –20  
0
20  
40  
60  
80  
100  
5
10  
15  
0
5
1
2
3
4
Output Step (Peak–To–Peak) – V  
Output Step (Peak–To–Peak) – V  
T
A
– Free-Air Temperature – °C  
Figure 15  
Figure 16  
Figure 14  
INPUT VOLTAGE AND CURRENT NOISE  
NORMALIZED FREQUENCY RESPONSE  
vs  
vs  
FREQUENCY  
FREQUENCY  
100  
2
100  
V
T
A
= ±15 V  
CC  
= 25°C  
R
= 300 Ω  
1
F
0
–1  
–2  
–3  
R
R
= 510 Ω  
I
Noise  
Noise  
F
F
n–  
= 750 Ω  
= 1 kΩ  
10  
10  
I
n+  
R
F
–4  
–5  
–6  
V
= ±15 V  
CC  
V = 200 mV  
I
R
= 25 Ω  
V
Noise  
L
n
Gain = 1  
T
A
–7  
–8  
= 25°C  
1
10  
1
100k  
100  
1k  
10k  
100  
1M  
10M  
100M  
500M  
f – Frequency – Hz  
f – Frequency – Hz  
Figure 18  
Figure 17  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
NORMALIZED FREQUENCY RESPONSE  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
3
2
9
8
2
R
= 360 Ω  
F
1
0
R
= 620 Ω  
F
R
= 510 Ω  
F
7
6
5
1
0
–1  
–2  
–3  
–4  
–5  
–1  
R
= 470 Ω  
F
R
= 1 kΩ  
R = 820 Ω  
F
F
–2  
–3  
–4  
–5  
–6  
4
3
2
1
0
R
= 1.5 kΩ  
R
= 1.2 kΩ  
F
F
R
= 620 Ω  
–6  
–7  
F
V
V
R
= ±15 V  
CC  
in  
L
V
= ± 5 V  
CC  
V
= ± 5 V  
= 200 mV  
= 25 Ω  
CC  
Gain = 2  
= 25 Ω  
Gain = 1  
= 25 Ω  
–8  
R
R
Gain = 2  
T
A
L
I
L
–9  
V = 200 mV  
R
= 1 kΩ  
V = 200 mV  
= 25°C  
F
I
–10  
100K  
100k  
1M  
10M  
100M  
500M  
100k  
1M  
10M  
100M  
500M  
1M  
10M  
100M 500M  
f – Frequency – Hz  
f – Frequency – Hz  
f – Frequency – Hz  
Figure 20  
Figure 21  
Figure 19  
12  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
TYPICAL CHARACTERISTICS (DRIVER)  
NORMALIZED OUTPUT RESPONSE  
vs  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
1
70  
60  
70  
60  
50  
40  
30  
20  
10  
0
R
= 200 Ω  
L
Gain = 1000  
Gain = 1000  
0
–1  
–2  
–3  
–4  
50  
40  
30  
20  
10  
0
Gain = 100  
Gain = 100  
R
= 100 Ω  
= 50 Ω  
L
R
L
R
= 25 Ω  
L
–5  
–6  
V
R
= ±15 V  
CC  
= 1 kΩ  
V
= ± 5 V  
CC  
G
L
V
R
R
= ± 5 V  
CC  
–7  
–8  
–9  
R
R
V
=10 Ω  
= 25 Ω  
= 2 V  
F
=10 Ω  
= 25 Ω  
= 2 V  
G
L
O
Gain = 1  
V = 200 mV  
I
O
V
–10  
100k  
–10  
100k  
100k  
1M  
10M  
100M  
500M  
1M  
10M  
100M  
500M  
1M  
10M  
100M  
500M  
f – Frequency – Hz  
f – Frequency – Hz  
f – Frequency – Hz  
Figure 23  
Figure 24  
Figure 22  
NORMALIZED OUTPUT RESPONSE  
vs  
NORMALIZED OUTPUT RESPONSE  
vs  
NORMALIZED OUTPUT RESPONSE  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
3
1
3
0
2
R
= 620 Ω  
R
= 430 Ω  
2
1
F
F
–1  
1
0
R
= 820 Ω  
F
–2  
–3  
–4  
0
–1  
–2  
–1  
–2  
R
= 1 kΩ  
F
R
R
= 25 Ω  
= 200 Ω  
= 100 Ω  
R
= 620 Ω  
= 1 kΩ  
L
L
F
–5  
–6  
–7  
–3  
–4  
–5  
R
–3  
–4  
–5  
–6  
F
R
L
V
R
= ±15 V  
= 100 Ω  
R
= 50 Ω  
V
R
= ±15 V  
= 100 Ω  
Gain = 2  
CC  
L
L
V
R
= ±15 V  
CC  
L
CC  
= 1 kΩ  
F
Gain = 1  
V = 200 mV  
I
Gain = 2  
V = 200 mV  
I
–8  
–9  
–6  
–7  
V = 200 mV  
I
100k  
1M  
10M  
100M  
500M  
100k  
1M  
10M  
100M  
500M  
100k  
1M  
10M  
100M  
500M  
f – Frequency – Hz  
f – Frequency – Hz  
f – Frequency – Hz  
Figure 26  
Figure 27  
Figure 25  
SINGLE–ENDED HARMONIC DISTORTION  
vs  
SMALL AND LARGE SIGNAL  
FREQUENCY RESPONSE  
SMALL AND LARGE SIGNAL  
FREQUENCY RESPONSE  
FREQUENCY  
3
0
–3  
–6  
–40  
V = 500 mV  
I
V = 500 mV  
I
V
= ± 15 V  
CC  
Gain = 2  
–50  
–60  
R
R
V
= 680 Ω  
–3  
–6  
–9  
–9  
–12  
–15  
F
L
V = 250 mV  
I
= 25 Ω  
= 2V  
V = 250 mV  
I
O(PP)  
V = 125 mV  
I
V = 125 mV  
I
–70  
–80  
–12  
–15  
–18  
–21  
–24  
–18  
–21  
–24  
–27  
–30  
2nd Harmonic  
V = 62.5 mV  
I
V = 62.5 mV  
I
3rd Harmonic  
Gain = 2  
Gain = 1  
–90  
V
= ± 15 V  
= 680 Ω  
= 25 Ω  
V
R
R
= ± 15 V  
= 820 Ω  
= 25 Ω  
CC  
CC  
R
R
F
L
F
L
–100  
100k  
1M  
10M  
100M  
500M  
100k  
1M  
10M  
100k  
1M  
10M  
100M 500M  
f – Frequency – Hz  
f – Frequency – Hz  
f – Frequency – Hz  
Figure 29  
Figure 30  
Figure 28  
13  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
TYPICAL CHARACTERISTICS (DRIVER)  
SINGLE–ENDED HARMONIC DISTORTION SINGLE–ENDED HARMONIC DISTORTION SINGLE–ENDED HARMONIC DISTORTION  
vs  
vs  
vs  
FREQUENCY  
OUTPUT VOLTAGE  
OUTPUT VOLTAGE  
–50  
–60  
–70  
–80  
–50  
–60  
–40  
–50  
V
= ± 15 V  
Gain = 2  
= 680 Ω  
CC  
V
= ± 5 V  
Gain = 2  
= 680 Ω  
= 25 Ω  
V
= ± 5 V  
CC  
CC  
Gain = 2  
= 680 Ω  
= 25 Ω  
f = 1 MHz  
R
R
F
L
R
R
V
R
R
F
L
F
L
= 25 Ω  
f = 1 MHz  
2nd Harmonic  
= 2V  
–60  
–70  
O(PP)  
3rd Harmonic  
3rd Harmonic  
2nd Harmonic  
–80  
–80  
–90  
2nd Harmonic  
–90  
–90  
3rd Harmonic  
15  
–100  
–100  
–100  
5
10  
20  
1
2
3
4
0
100k  
1M  
10M  
V
– Output Voltage – V  
V
– Output Voltage – V  
f – Frequency – Hz  
O(PP)  
O(PP)  
Figure 32  
Figure 33  
Figure 31  
DIFFERENTIAL GAIN AND PHASE  
vs  
DIFFERENTIAL GAIN AND PHASE  
vs  
DC INPUT OFFSET VOLTAGE  
DC INPUT OFFSET VOLTAGE  
0.05  
0.04  
0.03  
0.02  
0.01  
0
0.10  
0.08  
0.06  
0.05  
0.04  
0.03  
0.02  
0.01  
0
0.10  
0.08  
0.06  
0.04  
0.02  
0
V
R
R
= ±15 V  
= 150 Ω  
= 1 kΩ  
CC  
L
F
V
R
R
= ±5 V  
= 150 Ω  
= 1 kΩ  
CC  
L
F
Gain  
f = 3.58 MHz  
Gain = 2  
f = 3.58 MHz  
Gain = 2  
40 IRE Modulation  
40 IRE Modulation  
Phase  
Gain  
0.04  
0.02  
0
Phase  
–0.7 –0.5 –0.3 –0.1 0.1  
0.3  
0.5 0.7  
–0.7 –0.5 –0.3 –0.1 0.1 0.3  
0.5 0.7  
DC Input Offset Voltage – V  
DC Input Offset Voltage – V  
Figure 35  
Figure 34  
DIFFERENTIAL GAIN AND PHASE  
vs  
DIFFERENTIAL GAIN AND PHASE  
vs  
NUMBER OF 150-LOADS  
NUMBER OF 150-LOADS  
0.15  
0.12  
0.09  
0.06  
0.03  
0
0.25  
0.15  
0.12  
0.09  
0.06  
0.03  
0
0.25  
0.20  
V
R
= ±15 V  
CC  
= 1 kΩ  
V
R
= ±5 V  
CC  
= 1 kΩ  
F
F
Gain = 2  
Gain = 2  
0.20  
0.15  
0.10  
f = 3.58 MHz  
40 IRE Modulation  
100 IRE Ramp  
f = 3.58 MHz  
40 IRE Modulation  
100 IRE Ramp  
0.15  
0.10  
Phase  
Gain  
Gain  
0.05  
0
0.05  
0
Phase  
6
1
2
3
4
5
6
7
8
1
2
3
4
5
7
8
Number of 150-Loads  
Number of 150-Loads  
Figure 37  
Figure 36  
14  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
TYPICAL CHARACTERISTICS (DRIVER)  
400-mV STEP RESPONSE  
10-V STEP RESPONSE  
20-V STEP RESPONSE  
400  
300  
200  
100  
0
8
6
16  
12  
8
4
2
4
0
0
V
= ±15 V  
–100  
–200  
–2  
–4  
CC  
Gain = 2  
V
= ±15 V  
V
= ±15 V  
–4  
–8  
CC  
Gain = 2  
CC  
Gain = 5  
R
R
= 25 Ω  
= 1 kΩ  
L
F
R
R
= 25 Ω  
= 1 kΩ  
R
R
= 25 Ω  
= 2 kΩ  
L
F
L
F
t /t = 300 ps  
r f  
t /t = 5 ns  
r f  
t /t = 5 ns  
r f  
–300  
–400  
–6  
–8  
–12  
–16  
0
50 100 150 200 250 300 350 400 450 500  
0
50 100 150 200 250 300 350 400 450 500  
0
50 100 150 200 250 300 350 400 450 500  
t – Time – ns  
t – Time – ns  
t – Time – ns  
Note: See Figure 3  
Note: See Figure 3  
Note: See Figure 3  
Figure 39  
Figure 40  
Figure 38  
DRIVER-TO-RECEIVER CROSSTALK  
RECEIVER-TO-DRIVER CROSSTALK  
POWER SUPPLY REJECTION RATIO  
vs  
vs  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
–90  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
–90  
80  
70  
60  
V
V
= ± 15 V  
V
V
= ± 15 V  
= 200 mV rms  
CC  
= 200 mV rms  
V
= ±15 V or ± 5 V  
CC  
I
CC  
I
Both Channels  
See Figure 1  
Input = Driver 1  
Output = Receiver 2  
Input = Receiver 1 or Receiver 2  
Output = Driver 1  
50  
40  
Input = Driver 2  
Output = Receiver 2  
Input = Receiver 1 or Receiver 2  
Output = Driver 2  
Input = Driver 1  
Output = Receiver 2  
Input = Driver 1  
Output = Receiver 1  
30  
20  
10  
0
100k  
1M  
10M  
100M  
100k  
1M  
10M  
100M  
10 k  
100 k  
1 M  
10 M  
100 M  
f – Frequency – Hz  
f – Frequency – Hz  
f – Frequency – Hz  
Figure 42  
Figure 41  
Figure 43  
15  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
TYPICAL CHARACTERISTICS (RECEIVER)  
OPEN LOOP GAIN & PHASE RESPONSE  
RECEIVER-TO-RECEIVER CROSSTALK  
vs  
vs  
FREQUENCY  
FREQUENCY  
100.00  
45°  
0°  
–20  
V
V
= ± 15 V  
CC  
= 200 mV rms  
–30  
–40  
–50  
–60  
–70  
–80  
–90  
I
80.00  
60.00  
40.00  
20.00  
0.00  
Gain  
–45°  
90°  
Phase  
Input = Receiver 2  
Output = Receiver 1  
135°  
180°  
Input = Receiver 1  
Output = Receiver 2  
V
= ±5 V and ±15 V  
CC  
1k  
–225°  
–20.00  
100  
10k 100k 1M 10M 100M 1G  
100k  
1M  
10M  
100M  
f – Frequency – Hz  
f – Frequency – Hz  
Figure 44  
Figure 45  
SETTLING  
TOTAL HARMONIC DISTORTION  
TOTAL HARMONIC DISTORTION  
vs  
vs  
vs  
OUTPUT STEP  
FREQUENCY  
FREQUENCY  
–40  
–50  
–60  
–70  
–80  
–90  
–100  
–40  
–50  
–60  
–70  
–80  
–90  
–100  
330  
290  
250  
210  
170  
130  
90  
V
= ± 15 V  
V
= ± 5 V  
CC  
Gain = 2  
CC  
Gain = 2  
V
= 2 V  
V
= 2 V  
O(PP)  
O(PP)  
R
= 150 Ω  
R
= 150 Ω  
V
= ±5 V(0.01%)  
CC  
L
L
V
= ±15 V(0.01%)  
CC  
R
= 1 kΩ  
L
V
= ±5 V(0.1%)  
CC  
R
= 1 kΩ  
L
V
= ±15 V(0.1%)  
CC  
50  
10  
2
3
4
5
100k  
1M  
10M  
100k  
1M  
10M  
f - Frequency - Hz  
f - Frequency - Hz  
V
– Output Step Voltage – V  
O
Figure 46  
Figure 47  
Figure 48  
POWER SUPPLY REJECTION  
DISTORTION  
vs  
OUTPUT VOLTAGE  
DISTORTION  
vs  
OUTPUT VOLTAGE  
RATIO  
vs  
FREQUENCY  
–50  
–50  
–60  
0
–20  
2nd Harmonic  
V
= ± 15 V & ± 5 V  
CC  
2nd Harmonic  
–60  
–70  
–V  
CC  
3rd Harmonic  
3rd Harmonic  
–70  
–40  
+V  
CC  
–80  
–80  
–60  
V
R
= ± 15 V  
V
= ± 15 V  
R = 150 Ω  
L
CC  
= 1 kΩ  
CC  
–90  
–90  
–80  
L
Gain = 5  
Gain = 5  
f = 1 MHz  
f = 1 MHz  
–100  
–100  
–100  
0
5
10  
15  
20  
0
5
10  
15  
20  
100k  
1M  
10M  
100M  
f - Frequency - Hz  
V
– Output Voltage – V  
V
– Output Voltage – V  
O
O
Figure 49  
Figure 50  
Figure 51  
16  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
TYPICAL CHARACTERISTICS (RECEIVER)  
DISTORTION  
vs  
DISTORTION  
vs  
DISTORTION  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
–50  
–60  
–50  
–60  
–50  
–60  
V
R
= ± 15 V  
V
R
= ± 5 V  
V
= ± 15 V  
CC  
= 1 kΩ  
CC  
= 1 kΩ  
CC  
R = 150 Ω  
L
L
L
Gain = 2  
= 2 V  
Gain = 2  
= 2 V  
Gain = 2  
V = 2 V  
V
V
O(PP)  
O(PP)  
O(PP)  
3rd Harmonic  
–70  
–70  
–70  
2nd Harmonic  
2nd Harmonic  
2nd Harmonic  
–80  
–80  
–80  
3rd Harmonic  
–90  
–90  
–90  
3rd Harmonic  
–100  
–100  
–100  
100k  
1M  
10M  
100k  
1M  
10M  
100k  
1M  
10M  
f – Frequency – Hz  
f – Frequency – Hz  
Figure 53  
f – Frequency – Hz  
Figure 52  
Figure 54  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
DISTORTION  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
–50  
–60  
4
4
V
R
= ± 5 V  
CC  
= 150 Ω  
Gain = 2  
= 2 V  
L
R
= 130 Ω  
F
R
= 51 Ω  
= 0 Ω  
F
2
0
2
0
V
O(PP)  
R
= 51 Ω  
R
= 130 Ω  
F
F
3rd Harmonic  
–70  
R
R
= 0 Ω  
F
F
2nd Harmonic  
–80  
–2  
–4  
–6  
–2  
–4  
–6  
V
= ± 15 V  
V
= ± 5 V  
CC  
Gain = 1  
= 150 Ω  
CC  
Gain = 1  
–90  
R
V
R
= 150 Ω  
L
L
= 63 mV  
V
= 63 mV  
O(PP)  
O(PP)  
–100  
100k  
1M  
10M  
100k  
1M  
10M 100M 1G  
100k  
1M  
10M 100M 1G  
f – Frequency – Hz  
f - Frequency - Hz  
f - Frequency - Hz  
Figure 55  
Figure 56  
Figure 57  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
2
2
2
R
= 51 Ω  
F
R = 1.3 kΩ  
F
R
= 51 Ω  
F
R
= 2 kΩ  
F
0
–2  
–4  
–6  
–8  
0
–2  
–4  
–6  
–8  
0
–2  
–4  
–6  
–8  
R
= 1 kΩ  
F
R
= 0 Ω  
R
= 0 Ω  
F
F
V
= ± 15 V  
V
= ± 5 V  
V
= ± 15 V  
CC  
Gain = 1  
CC  
Gain = 1  
= 1 kΩ  
CC  
Gain = –1  
R = 150 Ω  
L
R
V
= 1 kΩ  
R
V
L
L
= 63 mV  
= 63 mV  
V
= 63 mV  
O(PP)  
O(PP)  
O(PP)  
100k  
1M  
10M 100M 1G  
100k  
1M  
10M 100M 1G  
100k  
1M  
10M 100M 1G  
f - Frequency - Hz  
f - Frequency - Hz  
f - Frequency - Hz  
Figure 58  
Figure 59  
Figure 60  
17  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
TYPICAL CHARACTERISTICS (RECEIVER)  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
2
0
2
0
2
0
R
= 1.3 kΩ  
R = 1.5 kΩ  
F
F
R
= 1.5 kΩ  
F
R
= 2 kΩ  
R
= 2 kΩ  
F
F
R
= 1.3 kΩ  
R = 1.3 kΩ  
F
F
R
= 1 kΩ  
F
–2  
–4  
–6  
–8  
–2  
–4  
–6  
–8  
–2  
–4  
–6  
–8  
V
= ± 5 V  
V
= ± 15 V  
V
= ± 5 V  
CC  
CC  
Gain = –1  
= 1 kΩ  
CC  
Gain = –1  
R = 1 kΩ  
L
Gain = –1  
R
V
= 150 Ω  
R
V
L
L
= 63 mV  
= 63 mV  
V
= 63 mV  
O(PP)  
O(PP)  
O(PP)  
100k  
1M  
10M 100M 1G  
100k  
1M  
10M 100M 1G  
100k  
1M  
10M 100M 1G  
f - Frequency - Hz  
f - Frequency - Hz  
f - Frequency - Hz  
Figure 61  
Figure 62  
Figure 63  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
8
8
8
R = 1.2 kΩ  
F
R
= 1.2 kΩ  
R
= 1.5 kΩ  
F
F
R
= 1.5 kΩ  
F
R
= 1.5 kΩ  
F
6
4
6
4
6
4
R
= 1.2 kΩ  
F
R
= 750 Ω  
F
R
= 750 Ω  
F
2
2
2
V
= ± 15 V  
V
= ± 5 V  
V
= ± 15 V  
CC  
Gain = 2  
= 150 Ω  
CC  
CC  
Gain = 2  
R = 1 kΩ  
L
0
0
0
Gain = 2  
R
R
= 150 Ω  
L
L
V
= 126 mV  
V
= 126 mV  
V
= 126 mV  
O(PP)  
O(PP)  
O(PP)  
–2  
–2  
–2  
100k  
1M  
10M 100M 1G  
100k  
1M  
100k  
1M  
10M 100M 1G  
10M  
100M  
1G  
f - Frequency - Hz  
f - Frequency - Hz  
f - Frequency - Hz  
Figure 64  
Figure 65  
Figure 66  
OUTPUT AMPLITUDE  
vs  
FREQUENCY  
2-V STEP RESPONSE  
5-V STEP RESPONSE  
8
1.2  
3
V
= ± 5 V  
CC  
Gain = 2  
R
= 1.2 kΩ  
F
0.8  
0.4  
2
1
R
R
= 1.2 kΩ  
= 150 Ω  
6
4
F
L
R
= 1.5 kΩ  
F
0.0  
0
2
–0.4  
–0.8  
–1.2  
–1  
–2  
–3  
V
= ± 5 V  
CC  
Gain = –1  
V
= ± 5 V  
CC  
Gain = 2  
0
R
R
= 1.3 kΩ  
= 150 Ω  
F
L
R
V
= 1 kΩ  
L
= 126 mV  
O(PP)  
–2  
100k  
1M  
10M 100M 1G  
0
200  
400  
600  
800  
1000  
0
200  
400  
600  
800  
1000  
f - Frequency - Hz  
t - Time - ns  
t - Time - ns  
Figure 67  
Figure 68  
Figure 69  
18  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
TYPICAL CHARACTERISTICS (RECEIVER)  
INPUT OFFSET VOLTAGE  
vs  
FREE-AIR TEMPERATURE  
2-V STEP RESPONSE  
20-V STEP RESPONSE  
1.2  
1.0  
12  
10  
8
1.5  
1.3  
1.1  
0.9  
0.7  
0.5  
0.3  
V
= ± 15 V  
V
= ± 15 V  
CC  
Gain = 2  
CC  
Gain = 5  
0.8  
R
R
= 1.2 kΩ  
= 150 Ω  
R
R
= 1.2 kΩ  
= 150 Ω  
F
L
F
L
V
= ± 15 V  
0.6  
6
CC  
0.4  
4
0.2  
2
–0.0  
–0.2  
–0.4  
–0.6  
–0.8  
–1.0  
–1.2  
0
–2  
–4  
–6  
–8  
–10  
–12  
V
= ± 5 V  
CC  
0
200  
400  
600  
800  
1000  
0
200  
400  
600  
800  
1000  
–40 –20  
0
20  
40  
60  
80 100  
t - Time - ns  
t - Time - ns  
T
- Free-Air Temperature - °C  
A
Figure 70  
Figure 71  
Figure 72  
OUTPUT VOLTAGE  
vs  
INPUT BIAS CURRENT  
vs  
OUTPUT VOLTAGE  
vs  
FREE-AIR TEMPERATURE  
SUPPLY VOLTAGE  
FREE-AIR TEMPERATURE  
15  
13  
11  
9
2.0  
1.9  
1.8  
1.7  
1.6  
1.5  
1.4  
1.3  
15  
13  
11  
9
T
=25°C  
A
V
R
= ± 15 V  
= 150 Ω  
CC  
L
V
R
= ± 15 V  
CC  
= 1 kΩ  
R
= 1 kΩ  
V
= ±15 V  
L
L
CC  
7
V
R
= ± 5 V  
= 1 kΩ  
R
= 150 Ω  
CC  
L
L
7
5
V
= ± 5 V  
CC  
5
3
V
R
= ± 5 V  
CC  
= 150 Ω  
L
1
3
–40 –20  
0
20  
40  
60  
80 100  
–40 –20  
0
20  
40  
60  
80 100  
5
7
9
11  
13  
15  
T
– Free-Air Temperature – C  
T
- Free-Air Temperature - °C  
±V  
- Supply Voltage - V  
CC  
A
A
Figure 73  
Figure 74  
Figure 75  
COMMON-MODE INPUT VOLTAGE  
SUPPLY CURRENT  
vs  
VOLTAGE AND CURRENT NOISE  
vs  
vs  
SUPPLY VOLTAGE  
SUPPLY VOLTAGE  
FREQUENCY  
15  
13  
11  
9
3.8  
3.6  
3.4  
3.2  
3.0  
2.8  
2.6  
2.4  
2.2  
100  
10  
V
= ± 15 V and ± 5 V  
CC  
= 25°C  
T
=25°C  
A
T
A
T
=85°C  
A
V
N
T
=25°C  
A
I
7
N
1
T
=–40°C  
A
5
0.1  
3
5
7
9
11  
13  
15  
5
7
9
11  
13  
15  
10  
100  
1k  
10k  
100k  
±V  
- Supply Voltage - V  
± V  
- Supply Voltage - V  
f - Frequency - Hz  
CC  
CC  
Figure 76  
Figure 77  
Figure 78  
19  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
APPLICATION INFORMATION  
ADSL  
TheTHS6007wasprimarilydesignedasalinedriverandlinereceiverforADSL(asymmetricaldigitalsubscriber  
line). The driver output stage has been sized to provide full ADSL power levels of 20 dBm onto the telephone  
lines. Although actual driver output peak voltages and currents vary with each particular ADSL application, the  
THS6007 is specified for a minimum full output current of 400 mA at its full output voltage of approximately 12  
V. ThisperformancemeetsthedemandingneedsofADSLatthecentralofficeendofthetelephoneline. Atypical  
ADSL schematic is shown in Figure 79.  
15 V  
+
THS6007  
Driver 1  
0.1 µF  
6.8 µF  
12.5 Ω  
+
_
V
I+  
1:2  
680 Ω  
To Telephone Line  
100 Ω  
0.1 µF  
6.8 µF  
+
–15 V  
15 V  
1 kΩ  
15 V  
220 Ω  
+
2 kΩ  
1 kΩ  
THS6007  
Driver 2  
0.1 µF  
6.8 µF  
0.1 µF  
12.5 Ω  
+
V
I–  
+
_
V
O+  
THS6007  
Receiver 1  
680 Ω  
1 kΩ  
2 kΩ  
1 kΩ  
0.1 µF  
6.8 µF  
+
–15 V  
+
V
O–  
THS6007  
Receiver 2  
0.1 µF  
–15 V  
Figure 79. Typical THS6007 ADSL Application  
20  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
APPLICATION INFORMATION  
ADSL (continued)  
The ADSL transmit band consists of 255 separate carrier frequencies each with its own modulation and  
amplitude level. With such an implementation, it is imperative that signals put onto the telephone line have as  
low a distortion as possible. This is because any distortion either interferes directly with other ADSL carrier  
frequencies or it creates intermodulation products that interfere with ADSL carrier frequencies.  
The THS6007 has been specifically designed for ultralow distortion by careful circuit implementation and by  
taking advantage of the superb characteristics of the complementary bipolar process. Driver single-ended  
harmonic distortion measurements are shown in Figures 30 and 31. It is commonly known that in the differential  
driver configuration, the second order harmonics tend to be reduced by 6 dB or more. Thus, the dominant total  
harmonic distortion (THD) will be primarily due to the third order harmonics. For this test, the load was 25 and  
the output signal produced a 2 V  
signal. Thus, the test was run at full signal and full load conditions.  
O(PP)  
Another significant point is the fact that distortion decreases as the impedance load increases. This is because  
the output resistance of the amplifier becomes less significant as compared to the output load resistance.  
ADSL receive line noise  
Per ANSI T1.413, the receive noise power spectral density for an ADSL line is –140 dBm/Hz. This results in  
a voltage noise requirement of less than 31.6 nV/Hz for the receiver in an ADSL system with a 1:1 transformer  
ratio.  
Noise Power Spectral Density = –140 dBm/Hz  
Power = 1e–17 × 1 Hz = 0.01 fW  
Assume: R = 100 Ω  
L
V
= (P×R) = (0.01 fW × 100 ) = 31.6 nV/Hz  
noise  
For ADSL systems that use a 1:2 transformer ratio, such as central office line cards, the voltage noise  
requirement for the receiver is lowered to 15.8 nV/Hz.  
TRANSFORMER  
V
noise  
ON LINE  
RATIO  
1:1  
31.6 nV/Hz  
15.8 nV/Hz  
1:2  
The THS6007 receiver was designed to operate with 10 nV/Hz voltage noise, exceeding the noise  
requirements for an ADSL system operating with 1:1 or 1:2 transformer ratios.  
21  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS6007  
DUAL DIFFERENTIAL LINE DRIVERS AND LOW-POWER RECEIVERS  
SLOS334– DECEMBER 2000  
APPLICATION INFORMATION  
The THS6007 contains four independent operational amplifiers. Two are designated as drivers because of their  
highoutputcurrentcapability, andtwoaredesignatedasreceivers. Thereceiveramplifiersarevoltagefeedback  
topology amplifiers made for high-speed, low-power operation and are capable of driving output loads of at least  
50 mA. The drivers are current feedback topology amplifiers and have been specifically designed to deliver the  
full power requirements of ADSL. They can deliver output currents of at least 400 mA at full output voltage.  
The THS6007 is fabricated using Texas Instruments 30-V complementary bipolar process, BiCOM. This  
process provides excellent isolation and high slew rates that result in the device’s excellent crosstalk and  
extremely low distortion.  
independent power supplies  
Each driver amplifier and both receivers of the THS6007 have their own power supply pins. This was specifically  
done to solve a problem that often occurs when multiple devices in the same package share common power  
pins. This problem is crosstalk between the individual devices caused by currents flowing in common  
connections. Whenever the current required by one device flows through a common connection shared with  
anotherdevice, thiscurrent, inconjunctionwiththeimpedanceinthesharedline, producesanunwantedvoltage  
on the power supply. Proper power supply decoupling and good device power supply rejection helps to reduce  
this unwanted signal. What is left is crosstalk.  
However, with independent power supply pins for each device, the effects of crosstalk through common  
impedance in the power supplies is more easily managed. This is because it is much easier to achieve low  
common impedance on the PCB with copper etch than it is to achieve low impedance within the package with  
either bond wires or metal traces on silicon.  
22  
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APPLICATION INFORMATION  
power supply restrictions  
Although the THS6007 is specified for operation from power supplies of ±5 V to ±15 V (or singled-ended power  
supply operation from 10 V to 30 V), and each amplifier has its own power supply pins, several precautions must  
be taken to assure proper operation.  
1. The power supplies for each driver amplifier must be the same value. For example, if driver 1 uses ±15volts,  
then driver 2 must also use ±15 volts. Using ±15 volts for driver 1 and ±5 volts for driver 2 is not allowed.  
2. The power supplies for the receiver amplifiers may be different than the driver supply voltages. Although  
it is recommended to use the same type of supply, either split supplies(±V ) or single supply (+V  
GND), for both drivers and receivers.  
and  
CC  
CC  
All the amplifiers within the THS6007 incorporate a standard Class A-B output stage. This means that some  
of the quiescent current is directed to the load as the load current increases. So under heavy load conditions,  
accurate power dissipation calculations are best achieved through actual measurements. For small loads,  
however, internal power dissipation for each amplifier in the THS6007 can be approximated by the following  
formula:  
V
O
P
D
2 V  
I
V
_ V  
D
CC CC  
CC  
O
R
L
Where:  
P
V
= Power dissipation for one amplifier  
= Split supply voltage  
CC  
I
V
R
= Supply current for that particular amplifier  
= Output voltage of amplifier  
= Load resistance  
CC  
O
L
To find the total THS6007 power dissipation, we simply sum up all four amplifier power dissipation results.  
Generally, the worst case power dissipation occurs when the output voltage is one-half the V voltage. One  
CC  
last note, which is often overlooked: the feedback resistor (R ) is also a load to the output of the amplifier and  
f
should be taken into account for low value feedback resistors.  
23  
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APPLICATION INFORMATION  
device protection features  
The drivers of the THS6007 have two built-in protection features that protect the device against improper  
operation. The first protection mechanism is output current limiting. Should the drivers output become shorted  
to ground, the output current is automatically limited to the value given in the data sheet. While this protects the  
output against excessive current, the device internal power dissipation increases due to the high current and  
large voltage drop across the output transistors. Continuous output shorts are not recommended and could  
damage the device. Additionally, connection of the amplifier output to one of the supply rails (±V ) can cause  
CC  
failure of the device and is not recommended. The use of Schottky diodes from each amplifier’s output to each  
power supply voltage rail is recommended. This will limit surges from the transmission line so as to not damage  
the THS6007.  
The drivers second built-in protection feature is thermal shutdown. Should the internal junction temperature rise  
above approximately 180 C, the device automatically shuts down. Such a condition could exist with improper  
heat sinking or if the output is shorted to ground. When the abnormal condition is fixed and the junction  
temperature drops below 150°C, the internal thermal shutdown circuit automatically turns the device back on.  
thermal information  
The THS6007 is packaged in a thermally-enhanced PWP package, which is a member of the PowerPAD  
family of packages. This package is constructed using a downset leadframe upon which the die is mounted  
[see Figure 80(a) and Figure 80(b)]. This arrangement results in the lead frame being exposed as a thermal pad  
on the underside of the package [see Figure 80(c)]. Because this thermal pad has direct thermal contact with  
the die, excellent thermal performance can be achieved by providing a good thermal path away from the thermal  
pad.  
The PowerPAD package allows for both assembly and thermal management in one manufacturing operation.  
During the surface-mount solder operation (when the leads are being soldered), the thermal pad can also be  
soldered to a copper area underneath the package. Through the use of thermal paths within this copper area,  
heat can be conducted away from the package into either a ground plane or other heat dissipating device. This  
is discussed in more detail in the PCB design considerations section of this document.  
The PowerPAD package represents a breakthrough in combining the small area and ease of assembly of  
surface mount with the, heretofore, awkward mechanical methods of heatsinking.  
DIE  
Side View (a)  
Thermal  
Pad  
DIE  
End View (b)  
Bottom View (c)  
NOTE A: The thermal pad is electrically isolated from all terminals in the package.  
Figure 80. Views of Thermally Enhanced PWP Package  
24  
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APPLICATION INFORMATION  
recommended feedback and gain resistor values  
As with all current-feedback amplifiers, the bandwidth of the THS6007 drivers is an inversely proportional  
function of the value of the feedback resistor. This can be seen from Figures 18 and 19. For the driver, the  
recommended resistors for the optimum frequency response for a 25-load system are 680 for a gain = 1  
and 620 for a gain = 2 or –1. These should be used as a starting point and once optimum values are found,  
1% tolerance resistors should be used to maintain frequency response characteristics. Because there is a finite  
amount of output resistance of the operational amplifier, load resistance can play a major part in frequency  
response. This is especially true with the drivers, which tend to drive low-impedance loads. This can be seen  
in Figure 12, Figure 24, and Figure 25. As the load resistance increases, the output resistance of the amplifier  
becomes less dominant at high frequencies. To compensate for this, the feedback resistor should change. For  
100-loads, it is recommended that the feedback resistor be changed to 820 for a gain of 1 and 560 for  
a gain of 2 or –1. Although, for most applications, a feedback resistor value of 1 kis recommended, which is  
a good compromise between bandwidth and phase margin that yields a very stable amplifier.  
Consistent with current-feedback amplifiers, increasing the gain is best accomplished by changing the gain  
resistor, not the feedback resistor. This is because the bandwidth of the amplifier is dominated by the feedback  
resistor value and internal dominant-pole capacitor. The ability to control the amplifier gain independent of the  
bandwidth constitutes a major advantage of current feedback amplifiers over conventional voltage feedback  
amplifiers. Therefore, once a frequency response is found suitable to a particular application, adjust the value  
of the gain resistor to increase or decrease the overall amplifier gain.  
Finally, it is important to realize the effects of the feedback resistance on distortion. Increasing the resistance  
decreases the loop gain and increases the distortion. It is also important to know that decreasing load  
impedance increases total harmonic distortion (THD). Typically, the third order harmonic distortion increases  
more than the second order harmonic distortion.  
The receivers of the THS6007 are voltage feedback amplifiers (VFB). Therefore the amplifiers follow the  
classical amplifier use of a gain-bandwidth-product. As gain increases, the bandwidth (–3 dB) decreases  
accordingly. There are no limitations on using capacitors within the feedback loop of VFB amplifier circuits.  
Figures 56 through 67 show the effects of feedback resistance and gain versus frequency. Using these graphs  
as a reference point is highly recommended.  
offset voltage  
Theoutputoffsetvoltage,(V )isthesumoftheinputoffsetvoltage(V )andbothinputbiascurrents(I )times  
OO  
IO  
IB  
the corresponding gains. The following schematic and formula can be used to calculate the output offset  
voltage:  
R
F
I
IB–  
R
G
+
+
V
I
V
O
R
S
I
IB+  
R
R
R
R
F
F
V
V
1
I
R
1
I
R
OO  
IO  
IB  
S
IB–  
F
G
G
Figure 81. Output Offset Voltage Model  
25  
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THS6007  
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APPLICATION INFORMATION  
noise calculations and noise figure  
Noise can cause errors on very small signals. This is especially true for the receiver amplifiers which are  
generally used for amplifying small signals coming over a transmission line. The noise model for  
current-feedback amplifiers (CFB) is the same as voltage-feedback amplifiers (VFB). The only difference  
between the two is that the CFB amplifiers generally specify different current noise parameters for each input  
while VFB amplifiers usually only specify one noise-current parameter. The noise model is shown in Figure 82.  
This model includes all of the noise sources as follows:  
e = Amplifier internal voltage noise (nV/Hz)  
n
IN+ = Noninverting current noise (pA/Hz)  
IN– = Inverting current noise (pA/Hz)  
e
= Thermal voltage noise associated with each resistor (e = 4 kTR )  
Rx x  
Rx  
e
Rs  
e
n
R
Noiseless  
S
+
_
e
ni  
e
no  
IN+  
IN–  
e
Rf  
R
f
e
Rg  
R
g
Figure 82. Noise Model  
The total equivalent input noise density (e ) is calculated by using the following equation:  
ni  
2
2
2
e
e
IN  
R
IN–  
R
R
4 kTR  
4 kT R  
R
n
s
ni  
S
F
G
F
G
Where:  
–23  
k = Boltzmann’s constant = 1.380658 × 10  
T = Temperature in degrees Kelvin (273 +°C)  
R || R = Parallel resistance of R and R  
F
G
F
G
To get the equivalent output noise of the amplifier, just multiply the equivalent input noise density (e ) by the  
ni  
overall amplifier gain (A ).  
V
R
R
F
e
e
A
e
1
(Noninverting Case)  
no  
ni  
ni  
V
G
26  
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APPLICATION INFORMATION  
noise calculations and noise figure (continued)  
As the previous equations show, to keep noise at a minimum, small-value resistors should be used. As the  
closed-loop gain is increased (by reducing R ), the input noise is reduced considerably because of the parallel  
g
resistance term. This leads to the general conclusion that the most dominant noise sources are the source  
resistor (R ) and the internal amplifier noise voltage (e ). Because noise is summed in a root-mean-squares  
S
n
method, noise sources smaller than 25% of the largest noise source can be effectively ignored. This can greatly  
simplify the formula and make noise calculations much easier to calculate.  
This brings up another noise measurement usually preferred in RF applications, noise figure (NF). Noise figure  
is a measure of noise degradation caused by the amplifier. The value of the source resistance must be defined  
and is typically 50 in RF applications.  
2
e
e
ni  
NF  
10log  
Rs  
Because the dominant noise components are generally the source resistance and the internal amplifier noise  
voltage, we can approximate the noise figure as:  
2
2
e
IN  
R
n
S
NF  
10log 1  
4 kTR  
S
The Figure 83 shows the noise figure graph for the drivers of the THS6007. Figure 84 shows the noise figure  
graph for the receivers of the THS6007.  
RECEIVER NOISE FIGURE  
vs  
SOURCE RESISTANCE  
DRIVER NOISE FIGURE  
vs  
SOURCE RESISTANCE  
40  
35  
30  
25  
20  
15  
10  
5
20  
T
A
= 25°C  
f = 10 kHz  
= 25°C  
18  
16  
14  
12  
10  
T
A
8
6
4
2
0
0
10  
100  
1k  
10k  
100k  
10  
100  
1k  
10k  
Source Resistance – R ()  
R
– Source Resistance – Ω  
S
s
Figure 83  
Figure 84  
27  
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APPLICATION INFORMATION  
PCB design considerations  
Proper PCB design techniques in two areas are important to assure proper operation of the THS6007. These  
areas are high-speed layout techniques and thermal-management techniques. Because the THS6007 is a  
high-speed part, the following guidelines are recommended.  
Ground plane – It is essential that a ground plane be used on the board to provide all components with a  
low inductive ground connection. Although a ground connection directly to a terminal of the THS6007 is not  
necessarily required, it is recommended that the thermal pad of the package be tied to ground. This serves  
two functions. It provides a low inductive ground to the device substrate to minimize internal crosstalk and  
it provides the path for heat removal.  
Input stray capacitance – To minimize potential problems with amplifier oscillation, the capacitance at the  
inverting input of the amplifiers must be kept to a minimum. To do this, PCB trace runs to the inverting input  
must be as short as possible, the ground plane should be removed under any etch runs connected to the  
inverting input, and external components should be placed as close as possible to the inverting input. This  
isespeciallytrueinthenoninvertingconfiguration. AnexampleofthiscanbeseeninFigure85, whichshows  
what happens when 1.8 pF is added to the inverting input terminal in the noninverting configuration. The  
bandwidth increases dramatically at the expense of peaking. This is because some of the error current is  
flowing through the stray capacitor instead of the inverting node of the amplifier. Although, in the inverting  
mode, stray capacitance at the inverting input has little effect. This is because the inverting node is at a  
virtual ground and the voltage does not fluctuate nearly as much as in the noninverting configuration.  
DRIVER  
NORMALIZED FREQUENCY RESPONSE  
vs  
FREQUENCY  
3
V
= ±15 V  
CC  
V = 200 mV  
2
I
R
R
= 25 Ω  
= 1 kΩ  
L
F
1
0
Gain = 1  
C = 0 pF  
I
(Stray C Only)  
–1  
–2  
C = 1.8 pF  
I
1 kΩ  
–3  
–4  
–5  
C
in  
in  
V
out  
V
+
R
25 Ω  
=
L
50 Ω  
–6  
–7  
100  
1M  
10M  
f – Frequency – Hz  
100M  
500M  
Figure 85. Driver Normalized Frequency Response vs Frequency  
28  
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APPLICATION INFORMATION  
PCB design considerations (continued)  
Proper power supply decoupling – Use a minimum of a 6.8-µF tantalum capacitor in parallel with a 0.1-µF  
ceramic capacitor on each supply terminal. It may be possible to share the tantalum among several  
amplifiers depending on the application, but a 0.1-µF ceramic capacitor should always be used on the  
supply terminal of every amplifier. In addition, the 0.1-µF capacitor should be placed as close as possible  
tothesupplyterminal. Asthisdistanceincreases, theinductanceintheconnectingetchmakesthecapacitor  
less effective. The designer should strive for distances of less than 0.1 inches between the device power  
terminal and the ceramic capacitors.  
Because of its power dissipation, proper thermal management of the THS6007 is required. Although there are  
many ways to properly heatsink this device, the following steps illustrate one recommended approach for a  
multilayer PCB with an internal ground plane.  
1. Prepare the PCB with a top side etch pattern as shown in Figure 86. There should be etch for the leads as  
well as etch for the thermal pad.  
2. Place the thermal transfer holes in the area of the thermal pad. These holes should be 13 mils in diameter.  
They are kept small so that solder wicking through the holes is not a problem during reflow.  
3. Additionalvias may be placed anywhere along the thermal plane outside of the thermal pad area. This helps  
dissipate the heat generated by the IC. These additional vias may be larger than the 13-mil diameter vias  
directly under the thermal pad. They can be larger because they are not in the thermal pad area to be  
soldered so that wicking is not a problem.  
4. Connect all holes to the internal ground plane.  
5. When connecting these holes to the ground plane, do not use the typical web or spoke via connection  
methodology. Webconnectionshaveahighthermalresistanceconnectionthatisusefulforslowingtheheat  
transfer during soldering operations. This makes the soldering of vias that have plane connections easier.  
In this application, however, low thermal resistance is desired for the most efficient heat transfer. Therefore,  
the holes under the IC package should make their connection to the internal ground plane with a complete  
connection around the entire circumference of the plated-through hole.  
6. The top-side solder mask should leave the terminals of the package and the thermal pad area with its  
thermal transfer holes exposed. The bottom-side solder mask should cover the thermal transfer holes of  
the thermal pad area. This prevents solder from being pulled away from the thermal pad area during the  
reflow process.  
7. Apply solder paste to the exposed thermal pad area and all of the IC terminals.  
8. With these preparatory steps in place, the THS6007 IC is simply placed in position and run through the  
solder reflow operation as any standard surface-mount component. This results in a part that is properly  
installed.  
29  
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APPLICATION INFORMATION  
PCB design considerations (continued)  
Thermal pad area (0.12 x 0.3)  
with 10 vias  
(Via diameter = 13 mils)  
Figure 86. PowerPAD PCB Etch and Via Pattern  
The actual thermal performance achieved with the THS6007 in its PowerPAD package depends on the  
application. In the previous example, if the size of the internal ground plane is approximately 3 inches × 3 inches,  
then the expected thermal coefficient, θ , is about 27.9 C/W. For a given θ , the maximum power dissipation  
JA  
JA  
is shown in Figure 87 and is calculated by the following formula:  
T
–T  
MAX  
A
P
D
JA  
Where:  
P
= Maximum power dissipation of THS6007 (watts)  
= Absolute maximum junction temperature (150°C)  
= Free-ambient air temperature (°C)  
D
T
MAX  
T
A
θ
= θ + θ  
JA  
JC CA  
θ
θ
= Thermal coefficient from junction to case (0.72°C/W)  
= Thermal coefficient from case to ambient  
JC  
CA  
It is recommended to design the system to keep the junction temperature (T ) at a minimum of 125°C. Junction  
J
temperatures higher 125°C than can lead to increased output distortion. Additionally, because the heat of the  
device is dissipated through the PCB, care must be taken to ensure the PCB does not become thermally  
saturated. Once this happens, the power dissipation of the system (PCB and active devices) becomes very  
in-efficient and the performance will suffer.  
More complete details of the PowerPAD installation process and thermal management techniques can be  
found in the Texas Instruments Technical Brief, PowerPAD Thermally Enhanced Package. This document can  
be found at the TI web site (www.ti.com) by searching on the key word PowerPAD . The document can also  
be ordered through your local TI sales office. Refer to literature number SLMA002 when ordering.  
30  
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PCB design considerations (continued)  
MAXIMUM POWER DISSIPATION  
vs  
FREE-AIR TEMPERATURE  
8
7
6
5
4
3
θ
= 27.9 C/W  
JA  
2 oz. Trace and  
Copper Pad With  
Solder  
T
J
= 150  
C
2
1
θ
= 56.2 C/W  
JA  
2 oz. Trace and  
Copper Pad  
Without Solder  
0
–40  
–20  
0
20  
40  
60  
C
80  
100  
T
A
– Free-Air Temperature –  
Figure 87. Maximum Power Dissipation vs Free-Air Temperature  
31  
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APPLICATION INFORMATION  
general configurations  
A common error for the first-time CFB user is to create a unity gain buffer amplifier by shorting the output directly  
to the inverting input. A CFB amplifier in this configuration is now commonly referred to as an oscillator. The  
THS6007 drivers, like all CFB amplifiers, must have a feedback resistor for stable operation. Additionally,  
placing capacitors directly from the output to the inverting input is not recommended. This is because, at high  
frequencies, a capacitor has a very low impedance. This results in an unstable amplifier and should not be  
considered when using a current-feedback amplifier. Because of this, integrators and simple low-pass filters,  
which are easily implemented on a VFB amplifier, have to be designed slightly differently. If filtering is required,  
simply place an RC-filter at the noninverting terminal of the operational-amplifier (see Figure 88).  
R
R
F
G
V
R
R
O
F
1
1
V
1
sR1C1  
I
G
V
O
1
+
f
V
I
–3dB  
2 R1C1  
R1  
C1  
Figure 88. Single-Pole Low-Pass Filter  
If a multiple pole filter is required, a Sallen-Key filter can work very well with CFB amplifiers. This is because  
the filtering elements are not in the negative feedback loop and stability is not compromised. Because of their  
high slew-rates and high bandwidths, CFB amplifiers can create very accurate signals and help minimize  
distortion. An example is shown in Figure 89.  
C1  
R1 = R2 = R  
C1 = C2 = C  
Q = Peaking Factor  
(Butterworth Q = 0.707)  
+
_
V
I
1
R1  
R2  
f
–3dB  
2 RC  
C2  
R
F
1
R
=
G
R
F
2 –  
)
(
R
Q
G
Figure 89. 2-Pole Low-Pass Sallen-Key Filter  
32  
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APPLICATION INFORMATION  
general configurations (continued)  
THS6007 driver amplifiers can also be used as very good video distribution amplifiers. One characteristic of  
distribution amplifiers is the fact that the differential phase (DP) and the differential gain (DG) are compromised  
as the number of lines increases and the closed-loop gain increases. Be sure to use termination resistors  
throughout the distribution system to minimize reflections and capacitive loading.  
620 Ω  
620 Ω  
75 Transmission Line  
75 Ω  
+
V
O1  
V
I
THS6007  
75 Ω  
75 Ω  
N Lines  
75 Ω  
V
ON  
75 Ω  
Figure 90. Video Distribution Amplifier Application  
driving a capacitive load  
Driving capacitive loads with high performance amplifiers is not a problem as long as certain precautions are  
taken. The first is to realize that the THS6007 has been internally compensated to maximize its bandwidth and  
slew rate performance. When the amplifier is compensated in this manner, capacitive loading directly on the  
output will decrease the device’s phase margin leading to high frequency ringing or oscillations. Therefore, for  
capacitive loads of greater than 10 pF, it is recommended that a resistor be placed in series with the output of  
the amplifier, as shown in Figure 91. A minimum value of 20 should work well for most applications. For  
example, in 75-transmission systems, setting the series resistor value to 75 both isolates any capacitance  
loading and provides the proper line impedance matching at the source end.  
1.3 kΩ  
1.3 kΩ  
_
Input  
20 Ω  
THS6007  
Output  
Receiver  
+
C
LOAD  
Figure 91. Driving a Capacitive Load  
33  
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MECHANICAL INFORMATION  
PWP (R-PDSO-G**)  
PowerPAD PLASTIC SMALL-OUTLINE  
20 PINS SHOWN  
0,30  
0,19  
0,65  
20  
M
0,10  
11  
Thermal Pad  
(See Note D)  
0,15 NOM  
4,50  
4,30  
6,60  
6,20  
Gage Plane  
1
10  
0,25  
A
0°8°  
0,75  
0,50  
Seating Plane  
0,10  
0,15  
0,05  
1,20 MAX  
PINS **  
14  
16  
20  
24  
28  
DIM  
5,10  
4,90  
5,10  
4,90  
6,60  
6,40  
7,90  
7,70  
9,80  
9,60  
A MAX  
A MIN  
4073225/F 10/98  
NOTES: A. All linear dimensions are in millimeters.  
B. This drawing is subject to change without notice.  
C. Body dimensions do not include mold flash or protrusions.  
D. The package thermal performance may be enhanced by bonding the thermal pad to an external thermal plane.  
This pad is electrically and thermally connected to the backside of the die and possibly selected leads.  
E. Falls within JEDEC MO-153  
PowerPAD is a trademark of Texas Instruments.  
34  
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IMPORTANT NOTICE  
Texas Instruments and its subsidiaries (TI) reserve the right to make changes to their products or to discontinue  
any product or service without notice, and advise customers to obtain the latest version of relevant information  
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pertaining to warranty, patent infringement, and limitation of liability.  
TI warrants performance of its semiconductor products to the specifications applicable at the time of sale in  
accordance with TI’s standard warranty. Testing and other quality control techniques are utilized to the extent  
TI deems necessary to support this warranty. Specific testing of all parameters of each device is not necessarily  
performed, except those mandated by government requirements.  
Customers are responsible for their applications using TI components.  
In order to minimize risks associated with the customer’s applications, adequate design and operating  
safeguards must be provided by the customer to minimize inherent or procedural hazards.  
TI assumes no liability for applications assistance or customer product design. TI does not warrant or represent  
that any license, either express or implied, is granted under any patent right, copyright, mask work right, or other  
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