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參數資料
| 型號： | TZA3041U |
| 廠商： | NXP SEMICONDUCTORS |
| 元件分類： | 其它接口 |
| 英文描述： | Gigabit Ethernet/Fibre Channel laser drivers |
| 中文描述： | SPECIALTY INTERFACE CIRCUIT, UUC40 |
| 封裝： | 2 X 2 X 0.38 MM, DIE-40 |
| 文件頁數： | 9/32頁 |
| 文件大小： | 153K |
| 代理商： | TZA3041U |
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2002 Aug 13
9
Philips Semiconductors
Product specification
Gigabit Ethernet/Fibre Channel laser
drivers
TZA3041AHL; TZA3041BHL;
TZA3041U
In this example, the resulting bandwidth for the optical 1
modulation current control loop, without an external
capacitor, is:
10
×
500
×
×
2
π
40
×
10
×
80
×
The resulting bandwidth for the optical 0 bias current
control loop, without an external capacitor, is:
30
×
10
×
×
2
π
40
×
10
×
It is not necessary to add additional capacitance with this
type of laser.
Control loop data pattern and bit rate dependency
The constants in equations (1) and (3) are valid when the
data pattern frequently contains a sufficient number of
‘constantzeroes’and‘constantones’.Asinglecontrolloop
time period (
τ
ONE
and
τ
ZERO
) must contain ones and zeros
for at least approximately 6 ns. When using the IC in
1.2 Gbits/s applications, the optical extinction ratio will be
slightly higher when compared with slower line rates.
Therefore, it is important to use the actual data patterns
and bit rate of the final application circuit for adjusting the
optical levels.
The laser driver peak detectors are able to track MPD
output current overshoot and undershoot conditions.
Unfortunately, these conditions affect the ability of the IC
to correctly interpret the high and low level MPD current.
In particular, the occurrence of undershoot can have a
markedly adverse effect on the interpretation of the low
level MPD current.
Additional bias by modulation ‘off’ current
Although during operation, the full modulation current
switches between outputs LA and LAQ, a small amount of
modulation current continues to flow through the inactive
pin.
For example, when the laser, whose cathode is connected
to LA, is in the ‘dark’ part of its operating cycle (logic 0),
some of the modulation ‘off’ current flows through LA while
most of the current flows through LAQ. This value
I
o(mod)(off)
is effectively added to the bias current and is
subtracted from the modulation current. Fortunately, the
value correlates closely with the magnitude of the
modulation current. Therefore, applications requiring low
bias and low modulation are less affected. Figure 9 shows
the modulation ‘off’ current as a function of the modulation
‘on’ current.
Monitoring the bias and modulation current
Although not recommended, the bias and modulation
currents generated by the laser driver can be monitored by
measuring the voltages on pins TZERO and TONE,
respectively (see Fig.10). The relationship between these
voltages and the corresponding currents are given as
transconductance values and are specified in
Chapter “Characteristics”. The voltages on pins TZERO
and TONE range from 1.4 to 3.4 V. Any connection to
these pins should have a very high impedance value. It is
mandatory to use a CMOS buffer or an amplifier with an
input impedance higher than 100 G
and with an
extremely low input leakage current (pA).
B
ONE
3
–
10
×
3
–
12
–
10
3
----30
750 Hz
≈
=
B
ZERO
3
–
500
50
×
10
10
3
3
–
×
×
12
–
0.5
600 Hz
≈
=
handbook, halfpage
0
20
40
60
1
0
2
MGS902
Io(mod)(on) (mA)
(2)
(1)
Io(mod)(off)
(mA)
Fig.9 I
o(mod)(off)
as a function of I
o(mod)(on)
.
(1) Worst case operation (T
= 125
°
C, V
CC
= 5.5 V
and worst case parameter processes).
(2) Typical operation.
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