
Laser Signal Injection Microscope Laser Scanning Fundamentals
|
|
To contact us: |
|
Phone: 425-251-6363 |
|
1. For further details on these
techniques see Tony Wilson "Theory and Practice of Scanning Optical
Microscopy", Academic Press, London (1984); E.I. Cole, Jr., J.M. Soden,
J.L. Rife, D.L. Barton, and C.L. Henderson, "Novel Failure Analysis
Techniques Using Photon Probing with a Scanning Optical Microscope",
IRPS, 388-98 (1994); E.I. Cole, Jr., P. Tangyunyong, and D.L. Barton,
"Backside Localization of Open and Shorted IC Interconnections",
IRPS, 129-136 (1998); E.I. Cole, Jr., P. Tangyunyong, D.A. Benson and D.L.
Barton, TIVA and SEI Developments for Enhanced Front and Backside
Interconnection Failure Analysis", ESREF (1999). 2. For further details see P. Perdu,
R. Desplats, and F. Beaudin, "Comparative Study of Sample Preparation
Techniques for Backside Analysis", ISTFA, 161-72 (2000) and B.V. Davis,
"Antireflection Coatings for Semiconductor Failure Analysis",
ISTFA, 155-60. (2000). 3. For topside probing, a dark
coating can be used to allow surface heating without photocarrier generation. |
|
OptoMetrix |
|
A class of failure analysis techniques has evolved
over the last several years that uses a scanning laser beam to activate
electrical characteristics of the test device. Optical Beam Induced Current
(OBIC) was the first of the class. It was later followed by Light Induced
Voltage Alterations (LIVA), Thermally Induced Voltage Alteration (TIVA), and
Seebeck Effect Imaging (SEI).(1) |
The use of this class of techniques for failure
analysis is primarily in fault isolation. TIVA, for example, locates ohmic
shorts due to the high resistance change that occurs with thermal heating at
most shorts. SEI locates opens due to
the electrical imbalance of the thermal electric effects at the open site. |
|
|
|
|
A significant feature of this class
of techniques is their ability to work from both the topside and backside of
an integrated circuit (IC). Backside analysis is critical for
"flip-chip" packages and devices with multiple metal layers that
obscure visibility from the topside. A basic system for performing the
fault isolation techniques uses a laser scanning microscope (LSM) to
sequentially scan a focused laser spot over the IC. Scanning can be performed
from the front or backside, with near infrared (IR) lasers used for backside
probing. Some device preparation for backside
scanning is also necessary. In addition to unzipping the package, thinning
and polishing of the substrate is generally required. Use of an
anti-reflection coating improves image quality and allows more of the laser
beam to penetrate into the substrate (2). As the focused laser beam passes over
an IC, it causes changes in the device’s electrical characteristics through
two effects, generation of photocarriers and heating. If the laser wavelength
is chosen to be below the semiconductor bandgap(3) then only heating occurs. |
Shorter wavelengths, above the
bandgap, will produce both photocarriers and heating. However,
photocarrier effects are orders of magnitude stronger and generally dominate
any thermal signals. Both photocarrier generation and heating can cause
changes in the circuit resistance (photoconductive and thermal-conductive
effects) and cause currents to flow (photovoltaic and Seebeck effects). For the photovoltaic and Seebeck
effects, no external bias is needed to observe a signal. For the
photoconductive and thermal conductive effects, application of a constant
current to the IC causes small voltage alterations to occur across the device
in response to the optically induced changes in the circuit resistance. The main application of these
techniques, to date, has been fault isolation. In some cases, faults are
located by comparison of an image from a "good" sample to the image
of a failed device. Comparison is not generally required for TIVA and SEI,
which only produce signals at the fault, associated drivers and drivelines.
The types of faults detected are determined by the detailed physics of the
laser interaction. |