Development of a Stress Compensation Layer for 3-D Assembly of Thin Pixel Modules

2015 ◽  
Vol 12 (1) ◽  
pp. 29-36
Author(s):  
G. Pares ◽  
T. McMullen ◽  
S. Tomé ◽  
L. Vignoud ◽  
R. Bates ◽  
...  

Pixel modules are the fundamental building blocks of the ATLAS pixel detector system used in the CERN LHC facility. In their basic form, they consist of a silicon sensor that is flip-chip bonded to a CMOS read-out integrated chip (ROIC). One of the main objectives for the ATLAS experiment is to develop an approach toward low-mass modules, thus reducing radiation length. From the module perspective, this can be achieved by using advanced 3-D technology processes that include the formation of copper and solder microbumps on top of the ROIC front side, the thinning of both the sensor and the CMOS ROIC, and, finally, the flip-chip assembly of the two chips. The thinning of the silicon chips leads to low bump yield at the solder reflow stage, due to bad coplanarity of the two chips creating dead zones within the pixel array. In the case of the ROIC, which is thinned to 100 μm, the chip bow varies from −100 μm at room temperature to +175 μm at reflow temperature, resulting in CTE mismatch between materials in the CMOS stack and the silicon substrate. Our objective was to compensate dynamically for the stress of the front-side stack by adding a compensating layer to the back side of the wafer. Using our material thermomechanical database coupled with a proprietary analytical simulator, and measuring the bow of the ROIC at die level, we were able to reduce the bow magnitude by approximately a factor of 3 by introducing the compensating layer. We show that it is possible to change the sign of the bow at room temperature after deposition of a SiN/Al:Si stack. The amplitude of the correction can be manipulated by the deposition conditions of the SiN/Al:Si stack. Further development of the back-side deposition conditions are ongoing, where the target is to control the room temperature bow close to zero and reduce the bow magnitude throughout the full solder reflow temperature range, hence conserving bump yield. In keeping with a 3-D process, the materials used are compatible with through-silicon via (TSV) technology with a TSV-last approach in mind, should we integrate this technology in the future.

2014 ◽  
Vol 2014 (1) ◽  
pp. 000787-000793 ◽  
Author(s):  
G. Pares ◽  
T. McMullen ◽  
S. Tomé ◽  
L. Vignoud ◽  
R. Bates ◽  
...  

The pixel modules are the fundamental building blocks of the ATLAS pixel detector system used in CERN LHC facility. They consist in their basic form of a silicon sensor that is flip-chipped bonded to a CMOS read-out integrated chip (ROIC). One of the main objectives for the ATLAS experiment is to develop an approach towards low mass modules and thus reducing radiation length. From the module perspective this can be achieved by using advanced 3D technology processes that includes the formation of copper and solder micro-bumps on top of the ROIC front-side, the thinning of both the sensor and the CMOS ROIC and finally the flip chip assembly of the 2 chips. The thinning of the silicon chips leads to low bump yield at the solder reflow stage due to bad co-planarity of the two chips creating dead zones within the pixel array. In the case of the ROIC, which is thinned to 100um, the chip bow varies from − 100 μm at room temperature to + 175 μm at reflow temperature resulting of CTE mismatch between materials in the CMOS stack and the silicon substrate. Our objective is to compensate dynamically the stress of the front side stack by adding a compensating layer to the back-side of the wafer. Utilising our material thermo-mechanical database coupled with a proprietary analytical simulator and measuring the bow of the ROIC at die level we are able to reduce the bow magnitude by approximately a factor of 3 by the introduction of the compensating layer. We show that it is possible to change the sign of the bow at room temperature after deposition of a SiN/Al:Si stack. This amplitude of the correction can be manipulated by the deposition conditions of the SiN/Al:Si stack. Further development of the backside deposition conditions are on-going where the target is to control the room temperature bow close to zero and reducing the bow magnitude throughout the full solder reflow temperature range hence conserving bump yield. In keeping with a 3D process the materials used are compatible with Through Silicon Via (TSV) technology with a TSV last approach in mind should we integrate this technology in the future.


Author(s):  
Raymond Lee ◽  
Nicholas Antoniou

Abstract The increasing use of flip-chip packaging is challenging the ability of conventional Focused Ion Beam (FIB) systems to perform even the most basic device modification and debug work. The inability to access the front side of the circuit has severely reduced the usefulness of tradhional micro-surgery. Advancements in FIB technology and its application now allow access to the circuitry from the backside through the bulk silicon. In order to overcome the problem of imaging through thick silicon, a microscope with Infra Red (IR) capability has been integrated into the FIB system. Navigation can now be achieved using the IR microscope in conjunction with CAD. The integration of a laser interferometer stage enables blind navigation and milling with sub-micron accuracy. To optimize the process, some sample preparation is recommended. Thinning the sample to a thickness of about 100 µm to 200 µm is ideal. Once the sample is thinned, it is then dated in the FIB and the area of interest is identified using the IR microscope. A large hole is milled using the FIB to remove most of the silicon covering the area of interest. At this point the application is very similar to more traditional FIB usage since there is a small amount of silicon to be removed in order to expose a node, cut it or reconnect it. The main differences from front-side applications are that the material being milled is conductive silicon (instead of dielectric) and its feature-less and therefore invisible to a scanned ion beam. In this paper we discuss in detail the method of back-side micro-surgery and its eflkcton device performance. Failure Analysis (FA) is another area that has been severely limited by flip-chip packaging. Localized thinning of the bulk silicon using FIB technology oflkrs access to diagnosing fdures in flip-chip assembled parts.


2012 ◽  
Vol 2012 (1) ◽  
pp. 001162-001168
Author(s):  
Yuka Tamadate ◽  
Seiji Sato ◽  
Hitomi Imai ◽  
Kota Takeda ◽  
Takeshi Meguro ◽  
...  

In order to significantly improve warpage of a PoP bottom package, Shinko developed an enhanced PoP structure. The inclusion of a support material attached to the backside of the flip chip die and over molded resin is the structure's key attribute. By adjusting the balance of each material (mold resin, substrate and support material thickness), we can better control warpage at both room temperature and reflow temperature. This enhanced thin PoP structure can be easily incorporated into a standard assembly process with existing equipment sets. This paper describes simulation results, along with measured warpage characteristics of the new package.


Author(s):  
Hung-Yun Lin ◽  
Abhishek Tambat ◽  
Ian Claydon ◽  
Ganesh Subbarayan ◽  
Dae Young Jung ◽  
...  

The risk of fracture in Interlayer Dielectric (ILD) stack is evaluated for various configurations of flip-chip packages in this paper. A novel analysis on the mechanical behavior of package with a focus on die surface provides the insights into the critical deformation state as well as its location. In Controlled Collapse Chip Connection (C4) process, the reflow phase involves a cooling of the entire package from the reflow temperature to room temperature, and is critical for package induced die cracking (Chip-Package Interaction or CPI). We use commercial finite element software ABAQUS to construct local sub-models of ILD region from global models of a representative 3-D package with component materials modeled as being temperature dependent elastic or elasto-plastic as appropriate. The risk of ILD fracture is systematically investigated using the described approach.


Author(s):  
M. H. Rhee ◽  
W. A. Coghlan

Silicon is believed to be an almost perfectly brittle material with cleavage occurring on {111} planes. In such a material at room temperature cleavage is expected to occur prior to any dislocation nucleation. This behavior suggests that cleavage fracture may be used to produce usable flat surfaces. Attempts to show this have failed. Such fractures produced in semiconductor silicon tend to occur on planes of variable orientation resulting in surfaces with a poor surface finish. In order to learn more about the mechanisms involved in fracture of silicon we began a HREM study of hardness indent induced fractures in thin samples of oxidized silicon.Samples of single crystal silicon were oxidized in air for 100 hours at 1000°C. Two pieces of this material were glued together and 500 μm thick cross-section samples were cut from the combined piece. The cross-section samples were indented using a Vicker's microhardness tester to produce cracks. The cracks in the samples were preserved by thinning from the back side using a combination of mechanical grinding and ion milling.


Author(s):  
K. Dickson ◽  
G. Lange ◽  
K. Erington ◽  
J. Ybarra

Abstract This paper describes the use of Electron Beam Absorbed Current (EBAC) mapping performed from the back side of the device as a means of locating metallization defects on flip chip 45nm SOI technology.


Nanomaterials ◽  
2021 ◽  
Vol 11 (7) ◽  
pp. 1692
Author(s):  
Emmanuel K. Ampadu ◽  
Jungdong Kim ◽  
Eunsoon Oh

We fabricated a lateral photovoltaic device for use as infrared to terahertz (THz) detectors by chemically depositing PbS films on titanium substrates. We discussed the material properties of PbS films grown on glass with varying deposition conditions. PbS was deposited on Ti substrates and by taking advantage of the Ti/PbS Schottky junction, we discussed the photocurrent transients as well as the room temperature spectrum response measured by Fourier transform infrared (FTIR) spectrometer. Our photovoltaic PbS device operates at room temperature for wavelength ranges up to 50 µm, which is in the terahertz region, making the device highly applicable in many fields.


2015 ◽  
Author(s):  
Aneliya KARADZHINOVA ◽  
Anton Nolvi ◽  
Jaakko Härkönen ◽  
Panja Luukka ◽  
Teppo Mäenpää ◽  
...  

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