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SEMI G30-88 © SEMI 198 6, 1988 3 recommended that the therm o couple be secured into the mount ing ba se wi th a the rmal cond uctin g adhe sive ( or solder) and that pa rticular attention be paid to mini mizi ng air voi…

SEMI G30-88 © SEMI 1986, 1988 2
efficient interface between the package and the primary
heat sink. The mounting surface temperature is
determined with a thermocouple attached from the side
or bottom of the adapter with a thermal conducting
adhesive or grease at or near the interface between the
adapter and the package. It is at this point that the
device-under-test temperature is specified and
controlled. The adapter also contains the socket or other
electrical interconnection scheme. A thin coating (about
25 – 50 mm thick) of a thermal heat-sinking compound,
such as zinc-oxide-loaded silicone thermal grease, is
used at the interface to provide a reliable thermal
contact.
2.3 Fluid Bath Assembly — A typical temperature-
controlled fluid bath for thermally characterizing the
microelectronic device under test is shown in Figure 2.
In this figure, the package is mounted in a fluid bath
separate from the fluid circulator, although it can be
immersed directly in an integrated fluid circulator/bath
unit. The fluid in the bath should be continuously
stirred or agitated to ensure the required temperature
stability. Since this working fluid is being used as an
infinite heat sink, the case-to-fluid (ambient)
temperature difference at the case temperature reference
point of interest should be minimized, i.e., less than or
equal to 20°C. For case-to-fluid temperature differences
greater than 20°C, accuracy and repeatability
difficulties may occur due to a large variable
temperature gradient in the fluid film boundary layer at
the package-fluid interface. The case-to-fluid
temperature difference can be minimized by increasing
the fluid velocity and by decreasing the power density
seen by the fluid. The device under test should be
mounted such that heat transfer to the fluid is not
impeded. For leaded devices, the leads should be
oriented in such a manner so as not to interfere with the
heat transfer to the fluid and provide freedom to any
thermal currents caused by the power dissipation within
the package. The case temperature of the device under
test should be measured with a thermocouple that is
attached to the package and should not be assumed to
be at the fluid temperature. Care should be taken to
minimize exposure of the thermocouple bead to the
high temperature gradient in the fluid film boundary
layer at the package-fluid interface. The working fluid
should have a thermal conductivity at 25°C of at least
0.0006 W/cm°C. Working fluids such as inert
fluorocarbon liquids and silicone oils are suitable as a
cooling media.
3 Procedure
3.1 Direct Measurement of Refere nce Point
Temperature — T
C
. For the purpose of measuring a
microelectronic device thermal resistance, the reference
point temperature shall be measured at the package
location of highest temperature which is accessible
outside the package. This reference point location is
determined with the device operating in free air and
with no external heat-sinking. In general, this reference
point is found to be on the outside surface of the
package substrate directly underneath the chip in the
major path of heat flow from the chip to the heat sink or
ambient. Examples of the reference point location for
both cavity-up and cavity-down ceramic packages are
depicted in Figure 3. The package surface may be
altered to facilitate this measurement, provided that
such alteration does not affect the original heat transfer
paths and, hence, the thermal resistance, within the
package by more than a few percent. For packages with
an integral heat dissipater attached to the outside
surface of the package substrate, the case temperature
reference point shall be on the surface of the heat
dissipater at a point opposite the backside of the chip as
indicated in Figure 4.
3.1.1 Case temperature, T
C
. The microelectronic
device under test shall be mounted under specified
conditions so that the case temperature can be held at
the specified value. A thermocouple shall be attached
on the surface of the device package directly under the
chip. A conducting epoxy may be used for this purpose.
The thermocouple bead should be in direct mechanical
contact with the case of the microelectronic device
under test. For devices which, in their normal
application, are intimately connected (by pressure
contact, adhesive, soldering, or other means) to an
external heat sink, the mounting surface temperature, as
measured directly below the primary heat removal
surface of the case, may be used as the equivalent case
temperature.
If it is found that attaching the thermocouple directly to
the case is impractical, an alternate approach utilizing a
thermocouple welded to one side of a thin metal disk
should be used. This can be accomplished by parallel
gap welding the crossed thermocouple wires to one side
of a 0.25 cm (0.094 in) diameter, 0.02 cm (0.008 in)
thick beryllium-copper disk and then, with a thin layer
of adhesive, bonding the other side of the disk to the
case at the point of interest.
3.1.1.1 Mounting surface temperature , T
M
. The
mounting surface temperature is measured directly
below the primary heat removal surface of the case. It is
measured with a thermocouple at or near the mounting
surface of the heat sink. A typical mounting
arrangement is shown in Figure 5. The surface of the
copper mounting base shall be nickel plated and free of
oxides.
The thermocouple hole shall be drilled into the
mounting base such that the thermocouple lead is
directly below the area on the case of interest. It is

SEMI G30-88 © SEMI 1986, 19883
recommended that the thermocouple be secured into the
mounting base with a thermal conducting adhesive (or
solder) and that particular attention be paid to
minimizing air voids around the ball or the
thermocouple. A thermal conducting compound (or
adhesive) should be used at the interfaces of the
mounting base and the device under test. The mounting
surface technique is application oriented in that it takes
into account the mounting surface interface.
3.2 Thermal Resistance, Junction-t o-Specified
Reference point, R
ΘJR
3.2.1 General Considerations — The thermal
resistance of a semiconductor device is a measure of the
ability of its carrier or package and mounting technique
to provide for heat removal from the semiconductor
junction. The thermal resistance of a microelectronic
device can be calculated when the case/mounting
surface temperature and power dissipation in the device
and a measurement of the junction temperature are
known.
When making the indicated measurements, the package
shall be considered to have achieved thermal
equilibrium when halving the time between the
application of power and the taking of the reading
causes no error in the indicated results within the
required accuracy of measurement.
3.2.2 Indirect Measurement of Junction Temperature
for the Determination of R
ΘJR
— The purpose of the test
is to measure the thermal resistance of integrated
circuits by using particular semiconductor elements on
the chip to indicate the device junction temperature. In
order to obtain a realistic estimate of the operating
junction temperature, the whole chip in the package
should be powered in order to provide the proper
internal temperature distribution. During measurement
of the junction temperature the chip heating power
(constant voltage source) shall remain constant while
the junction calibration current remains stable. It is
assumed that the calibration current will not be affected
by the circuit operation during the application of
heating power.
The temperature-sensitive device parameter is used as
an indicator of an average (weighted) junction
temperature of the semiconductor element for
calculations of thermal resistance. The measured
junction temperature is indicative of the temperature
only in the immediate vicinity of the element used to
sense the temperature.
The temperature-sensitive electrical parameters
generally used to indirectly measure the junction
temperature are the forward voltage of diodes and the
emitter-base voltage of bipolar transistors. Other
appropriate temperature-sensitive parameters may be
used for indirectly measuring junction temperature for
fabrication technologies that do not lend themselves to
sensing the active junction voltages.
3.2.2.1 Steady-state technique for mea suring T
J
. The
following symbols shall apply for the purpose of these
measurements:
I
M
Measuring current in milliamperes.
V
MH-
Value of temperature-sensitive parameter in
millivolts, measured at I
M
, and corresponding to the
temperature of the junction heated by P
H
.
T
MC-
Calibration temperature in degrees Celsius,
measured at the reference point.
V
MC-
Value of temperature-sensitive parameter in
millivolts, measured at I
M
, and specific value o
f
T
MC
.
The measurement of T
J
using junction forward voltage
as the TSP is made in the following manner:
Step 1 — Measurement of the temperature coefficient
of the TSP (calibration).
The coefficient of the temperature-sensitive parameter
is generated by measuring the TSP as a function of the
reference point temperature, for a specified constant
measuring current, IM, by externally heating the device
under test in an oven or in a fluid bath. The reference-
point temperature range used during calibration shall
encompass the temperature range encountered in the
power application test (see Step 2). The measuring
current is generally chosen such that the TSP decreases
linearly with increasing temperature over the range of
interest, and that negligible internal heating occurs in
the silicon and metal traces. For determining the
optimum TSP calibration or measuring current, V
MC
vs.
log I
M
curves for two temperature levels that encompass
the calibration temperature range of interest should be
plotted. The optimum measuring current, I
M
, is then
selected such that it resides on the linear portion of the
two V
MC
vs. log I
M
curves that were generated. A
measuring current ranging from 0.05 to 5 mA is
generally used, depending on the specifications and
operating conditions of the device under test, for
measuring the TSP. The value of the TSP temperature
coefficient, V
MC
/T
MC
, for the particular measuring
current used in the test, is calculated from the
calibration curve, V
MC
vs. T
MC
. At least three points
should be used to generate the voltage vs. temperature
curve for the determination of the TSP temperature
coefficient.
Step 2 — Power application test.
The power application test is performed in two parts.
For both portions of the test, the reference point
temperature is held constant at a preset value. The first

SEMI G30-88 © SEMI 1986, 1988 4
measurement to be made is that of the temperature-
sensitive parameter, i.e., V
MC
, under operating
conditions with the measuring current, I
M
, used during
the calibration procedure. The microelectronic device
under test shall then be operated with heating power
(P
H
) applied. The temperature-sensitive parameter,
V
MH
, shall be measured with constant measuring
current, I
M
, that was applied during the calibration
procedure (See Step 1).
The heating power, P
H
, shall be chosen such that the
calculated junction-to-reference point temperature
difference as measured at V
MH
is greater than or equal
to 20°C. In accomplishing this, the device under test
should not be operated at such a high heating power
level that the on-chip temperature-sensing and heating
circuitry is no longer electrically isolated. Care should
also be taken not to exceed the design ratings of the
package-interconnect system, as this may lead to an
overestimation of the power being dissipated in the
active area of the chip due to excessive power losses in
the package leads and wire bonds. The values of V
MH
,
V
MC
, and P
H
are recorded during the power application
test.
The following data shall be recorded for these test
conditions:
a. Temperature-sensitive electrical parameters (V
F
,
V
EB
, or other appropriate TSP).
b. Junction temperature, T
J
, is calculated from the
equation:
T
J
= T
R
+ V
MH
− V
MC
()
∆V
MC
∆T
MC
ê
ê
ú
ú
−1
where T
R
= T
C
or T
M
c. Case or mounting surface temperature, T
C
or T
M
.
d. Power dissipation, P
H
.
e. Mounting arrangement (including package
mounting force).
3.3 Calculations of R
ΘJR
3.3.1 Calculations of Package Therm al Resistance —
The thermal resistance of a microelectronic device can
be calculated when the junction temperature, T
J
, has
been measured in accordance with procedures outlined
in Sections 3.1 and 3.2.
With the data recorded from each test, the thermal
resistance shall be determined from:
R
Θ
JR
=
T
J
−
T
R
P
H(package)
, junction - to reference point,
where R
QJR
=R
QJC
or R
QJM
and T
R
=T
C
or T
M
, respectively.
4 Summary Report
The following details shall be specified as appropriate:
a. Description of package, including thermal test chip,
location of case or chip carrier temperature
measurement(s), and heat sinking arrangement.
b. Test condition(s), as applicable (see Section 3).
c. Test voltage(s), current(s), and power dissipation of
test chip.
d. Recorded data for each test condition, as applicable.
e. Symbol(s) with subscript designation(s) of the
thermal characteristics determined.
f. Accept or reject criteria.
RELATED REFERENCES
1. Unencapsulated Thermal Test Chip, SEMI G32-86
Guideline, Book of SEMI Standards, Packaging
Volume.
2. Accepted Practices for Making Microelectronic
Device Thermal Characteristics Test — A User’s
Guide. JEDEC Engrg. Bull. No. 20, Jan. 1975
(Electronic Industries Assoc., Washington, D.C.).
3. Thermal Characteristics, Method 1012.1, MIL-STD-
883C Test Methods and Procedures for
Microelectronics, Nov. 4, 1980 (Rev. Aug. 15,
1984).