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Improved Reliability and ESD
characteristics of Flip-Chip GaN-based LEDs with Internal
Inverse-parallel Protection Diodes Jinn-Kong Sheu1,*, Shih-Chang
Shei2, Chien-Fu Shen3 1Institute of Electro-optical Science and
Engineering, National Cheng Kung
University,Taiwan. 2Department of Electronic
Engineering, National University of Tainan,700,
Taiwan 3Institute of Microelectronics & Department
of Electrical Engineering National Cheng Kung University, Tainan,
70101, Taiwan Email:jksheu@mail.ncku.edu.tw
IEEE
Electron Device Letters, Vol. 28, No. 5, May, 346-349(
2007).
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Although great improvement in
efficiency has been well proven in GaN-based LEDs with ITO upper
contact layers, the light extraction efficiency (LEE) is still
limited by several factors. For example, the shadow of the bonding
pads and wires in conventional face-up devices would result in a
reduction of LEE. One possible way to solve the problem is to
use flip-chip (FC) technology. Reliability is a crucial factor for
different applications such as LCD (liquid crystal display)
backlight modules. Aside the decay of light output power,
Electrostatic discharge (ESD)-induced electrical pulse is one of the
main reliability concerns for LEDs. It is well known that GaN-based
LEDs can be electrically connected to Si Zener diodes in order to
significantly improve the ESD protection capability [3]. Recent
studies have demonstrated that GaN/sapphire LEDs can be electrically
protected from ESD damage by using a shunt GaN Schottky barrier
diodes (SBDs) connected in parallel to the GaN LED. Since the GaN
Schottky diodes were formed by metal contacts deposited on the
etched GaN surfaces, the reproducibility and reliability were not
perfect. Therefore, the device yield was much lower than typical
yield of conventional GaN/sapphire LEDs without the shunt SBDs. In
this study, a LED structure featuring electrostatic discharge (ESD)
protection function was designed. The design incorporated a
GaN-based p-n diode (named ESD diode) instead of the SBD. The p-n
diode was electrically connected in inversely parallel direction to
the GaN LED. According to the design, the layer structure of the ESD
diode was identical to the GaN LED, but the area of the ESD diode
was smaller than the area of GaN LED, as shown in Fig.1(a). The idea
behind the design was to provide GaN LEDs good protection from the
ESD damage. In our design pulsed surge current could flow through
the ESD diode in case of reversely electrostatic discharge or an
abnormally high voltage. On the other hand, to further improve the
output power of the ESD-protected GaN-based LEDs, FC technology was
also used in this study.
Fig. 1.(a)Bare-chip photograph of the LED-I. (b)
Equivalent circuit diagram schematically illustrating LED-II. The
schematic layer structure comprises(c) an inverse-parallel-connected
GaN ESD diode and (d) a GaN LED The InGaN/GaN MQW LED
wafers used in this study were all grown by MOCVD on c-face sapphire
substrates. After the wafer growth procedures, the ITO layer was
subsequently evaporated onto the sample to serve as a transparent
contact layer. For device process, wafers were partially etched
until the n+-GaN layers were exposed. In order to
electrically isolate the GaN LED diodes and the ESD diodes disposed
on the same substrate, the n+-GaN layers were further
partially etched away by dry etching until the sapphire substrate
was exposed. Next, 1-m-thick SiO2 films were deposited over the
chips to simultaneously serve as the passivation layer and the
electrical insulation layer between the two diodes. Following the
deposition of the SiO2 films, Cr/Pt/Au (300/100/25m) were deposited
onto the exposed n+-GaN/ITO contact layers to
simultaneously serve as the n-type/p-type electrodes and the
interconnection between the GaN LED diodes and the ESD diodes. It
should be noted that the above-mentioned LEDs were labeled as LED-I.
Figures 1(a), 1(c) and 1(d) show the top-view photograph of the
LED-I, the layer structure of ESD diode and the GaN LED diode,
respectively. In case of FC samples, Ag-based reflector was
performed on the ITO transparent contact layer by e-beam evaporator
[4]. Sn/Au(15 μm/5 μm) layers were then electroplated onto the
samples to form the P/N bumps. The processed wafers were then lapped
down to about 110 μm and then were broken into individual dies with
size of 380 μm × 350 μm. It should be noted that FC LEDs were
soldered onto Si sub-mounts prior to packaging and they were labeled
as LED-II. For comparison, conventional GaN-based LEDs without the
inverse-parallel internal diode were also prepared and labeled as
LED-III. The ESD characteristics were tested using the Electrostatic
Discharge Simulator-Model 910, which consisted of a variable high
voltage power supply, a high voltage switch and an R/C discharge
network. The device allowed to simulate different electrostatic
discharges produced by a human body (Mil Std. 883E)
The
analysis of Fig.1(a) shows that it is identical to a circuit diagram
schematically illustrated in the Fig.1(b). One can see that the ESD
diode (i.e., C-D junction has inverse-parallel connection to the GaN
LED diode (i.e., A-B junction). In general, the shunt ESD
diode operates in the reverse region unless it goes into the state
of irreversible breakdown due to high reverse bias. Thus the shunt
diode remains conducted and exhibits rectification characteristics.
When a normal forward bias is applied to the two ends of LED-I (V+
and V-), forward current is generated by the carriers passing the
A-B junction and the LED diode emits light. However, when
abnormal high reverse voltage or electrostatic charge event occurs,
the excessively high voltage can be discharged by the ESD diode that
is conducted in the forward-bias regions, and thus high reverse
current does not flow to the LED diode. Therefore, we can see
that the LED diode is protected from the potential damages resulting
from electrostatic discharge, abnormal reverse voltage or
excessively high voltage. Fig. 2 shows typical forward I-V
characteristics of LED-I, LED-II and LED-III. As shown in the inset
of Fig.2, the difference of forward voltage (at 20 mA) between these
LEDs does not exceed 0.1 Volt. On the other hand, to judge whether
the LEDs failed or not after an HBM pulse stress was applied, the
failure criterion was set at a reverse leakage current of 2A
measured at a reverse voltage of -5V. We applied negative ESD stress
to the anode, meanwhile keeping the cathode grounded, to evaluate
negative ESD levels. As shown in Fig.3, LED-III could only endure
negative ESD pulses of around 500V. However, our observations also
showed that LED-I could endure ESD pulses as high as negative 3500
V. In other words, we were able to significantly enhance the ESD
characteristics of GaN-based LEDs by using a shunt GaN ESD diode
connected in inversely-parallel direction to the GaN LED. As shown
in Fig. 3, similar results were also observed for LED-II with FC
configuration. Fig. 3 also shows typical output power-current (L-I)
characteristics of LED-I, LED-II and LED-III. Light output powers of
the LEDs with bare-chip form, packaged using epoxy-free metal TO
cans (TO-46), were measured under the same conditions. In addition
to excellent ESD-protection capabilities, the light output
performance of LED-I was also comparable with conventional LEDs
(LED-III). When a 20 mA current injection was applied, the output
power of LED-I and LED-III, emitting a wavelength of around 465 nm,
was around 7.3 mW and 7.5 mW, respectively. However, the LED-II with
FC configuration exhibited an output power as high as 12.6 mW.
Moreover, the reliability of the LED-II is expected to be superior
to the conventional GaN LEDs without the ESD protection function.
Reliability tests of LEDs featuring ESD protection were also
performed by injecting 20 mA DC current into these devices at room
temperature. Fig. 4 shows aging tests of relative luminous
intensities, measured for LED-I, LED-II, and LED-III, normalized to
their respective initial readings. After 1200 hours of operation, we
found that luminous intensities of LED-I, LED-II, and LED-III,
decreased by 19 %, 4 %, and 22 %, respectively. It is clear that the
degradation trend is comparable between LED-I and LED-III. However,
when compared to LED-I and LED-III, thermal path of LED-II was much
shorter. Thus, most heat generated in LED chips could easily flow to
the heat sink (Si sub-mount) in case of FC LEDs. As a result, we can
see that the FC technology allows obtaining LEDs with improved
reliability.
Fig. 2.Typical forward I-V characteristics of
LED-I, LED-II, and LED-III.
Fig. 3.Measured ESD results as a function of stress
voltage and light output power as function of forward current of the
LEDs. The values shown in the right-hand vertical axis mean the
total tested dvice numbers (100 devices) divided by the non-filed
device numbers ofr a given reverse stress voltage.
Fig. 4.Room-temperature aging tests of relative luminous
intensities, measured from LED-I, LED-II, and LED-III, normalized to
their respective inital readings.
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