通过芯片到晶圆混合键合实现多层芯片堆叠

时间:2024-07-16 15:37:33 浏览量:0

Abstract—A collective die-to-wafer bonding flow is extended  beyond the N=2 tier to the N=3 and N=4 tier by collectively  bonding multiple layers of dies on top of a target wafer. The N=2  die-level is shown to be consistently free of bonding voids (bond  yields close to 100%) with +99% die transfer yields. For the N=3  and N=4 die-levels, both the transfer yields and bonding yields are  significantly lower. Both N=2 and N=3 stacks show similar die-totarget wafer alignment. A cross sectional SEM of a 5-micron pitch  shows excellent alignment and connectivity between Die 1 and Die  2 (N=3).


I. INTRODUCTION  

Certain 3D IC technologies require a vertical interconnect with high connectivity densities between dies. A high  alignment accuracy follows and as such the choice of process favors a hybrid bonding process. Both collective die-to-wafer  bonding and direct die-to-wafer bonding schemes are attractive in this regard.  Where a direct bonding flow seems much  less complex compared to a collective bonding flow, there  remain limitations regarding die-level cleanliness. Much  progress has been made though, by enabling a wafer level  cleaning approach before die pick up. However, during the final  pick-up step the sensitive bond surface will be in contact with  the die-placement tool leading to very stringent tool-cleanliness requirements or in situ die-level cleaning capability. In contrast, a collective die-to-wafer bonding flow, although more complex,  allows all processing on wafer-level tools and as such allows  inspection of the die level bonding surface prior to bonding. In  several previous reports, imec’s proposed flows were explained in detail. It was shown that very thin dies (50 µm) or  thick dies (775 µm) can be transferred from a temporary carrier  to a target wafer with transfer yields and bond yields close to  imec. The choice of temporary carrier system will depend  strongly on the die type. For ultra-thin and flat dies (50 µm) a  silicon carrier system can be used that allows mechanical  debonding of the dies with transfer yields up to unity.Mechanical debonding has the advantage of using silicon  carriers. On the other hand, using glass offers the benefit of UVlaser debonding.


Whenever dies become either too thick, too warped or  simply have a different backside, the final touch to the adhesive of the carrier system might be impacted. Finetuning adhesion to  enable wafer level cleaning (without losing dies) and still  allowing a mechanical peel debond often results in either a  limited die transfer or extensive die damage.Solving dietemporary carrier adhesion issues can be time consuming and  very die-dependent. As such a glass carrier was introduced for the final debonding step together with a laser release layer (LRL)  on the dies. Although 100% die transfer could easily be  achieved, 1-4% of the dies showed some damage during the  process. A study was performed to assess potential laser damage  to ultrathin dies. The main finding was that during the ablation  process a shockwave is generated in the LRL that propagates to  the thin die and leads to some damage at the corners of the dies. This damage can easily be avoided by separating the ablation  interface from the die interface by either using a thick LRL or  an additional temporary bond material (TBM) between the LRL  and the die, (which we will call acoustic layer (AL). Using the latter methodology, 100% die transfer could be achieved with  electrically yielding daisy chains and kelvin structures up to  80% for the 7-µm pitch range.


The robustness of this flow was demonstrated several times  for the N=2 level, with N equal to the number of interfaces. Provided that the right dielectrics are present on the die  backside, after die transfer the dies can be collectively cleaned  and a second layer of dies can be bonded on top (Fig. 1). This  step can be repeated X times to allow multi die stacking. In this  publication the process of reference (POR) flow, using laser  debonding and acoustic layer, is utilized to enable N=3 and N=4  stacks. As such a first layer of dies is transferred to the target  wafer (tier 1) to enable N=2. During Tier 2 a second layer of dies  is transferred on top of the first layer of dies to enable N=3 and  finally Tier 3 to enable N=4. Both non-aligned bonding and  aligned bonds are shown. Finally, an N=3 stack is prepared  using electrically yielding dies in order to evaluate the  connectivity between die 1 and die 2 using a cross sectional  SEM of a 5-micron pitch connection.


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Figure 1. Simplified flow for N=2, N=3 and N=4  collective die-to-wafer transfer.


The collective die-to-wafer flow consists of several parts: i)  die preparation, ii) die pick and place, iii) bonding and iv)  debonding. For the die preparation step, the wafer is flipped and  mounted/bonded upside down to a temporary carrier using a temporary bonding system. The wafer is thinned down to 50 µm, and the backside surface is prepared. For the short loop  experiments the temporary bond system was BrewerBOND 305 paired with BrewerBOND 510 material which allows for  an easy mechanical release during the subsequent wafer flip  step. A low temperature SiCN is deposited as backside bonding  dielectric. For the full loop dies, presented in section IV,  Brewer’s Versa layer system consisting of BrewerBOND C1301 and BrewerBOND T1107 was used. This system  enables elevated temperature processing and much better CMP control during the preparation of the hybrid bond pads after TSV  reveal. The details of the full loop die processing and results will  be published elsewhere. After backside preparation the thin  wafer is flipped again, this time to a glass carrier, and the  frontside is thoroughly cleaned after which a photoresist is  coated to protect the frontside dielectric. This wafer flip step and  resist coating step has several functions: the resist protects the  die-frontside from the tape used during dicing as well as from  the dicing itself. The temporary bonding adhesive and laser  release layer allow for a final flip onto tape frame to enable  dicing. Both of the materials will be diced and re-used during  the final collective die transfer step.


Four N=2 stacks were prepared and evaluated by calculating  the transfer yields and bond yields. All prepared wafers had a transfer yield between 98-100% (Fig 3). The transfer yield is  defined as the number of dies that were successfully transferred  to the target wafer over the number of dies that were successfully  populated on the temporary carrier. The bond yield (described  in detail in [8]) is a measure of how void free the transferred dies  are and are all close to 99%.


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Figure 3. Simplified collective die-to-wafer bonding flow with pictures of the N=2 target wafer (after tier 1), the N=3  bonded stack and the N=3 target wafer (after tier 2).


In the following step the four N=2 stacks were used to  generate four N=3 stacks (Fig 3 & 4). In contrast to the Tier 1 transfers the transfer yields of Tier 2 vary strongly from stack to  stack with the best result being 93% and the worst 64% (92%  and 84% for the two others). The lower transfer yields are also  reflected in lower bond yields (Fig 4 & 6). The bond yields range  between 60% and 85% however, this data is misleading due to  the non-transferred dies. Normalizing the bond yield over the  number of transferred dies gives a more realistic number of the  number of voids per transferred dies. These normalized bond  yields range from 85 to 90%. This means that around 10-15% of  the die area shows voiding indicative of a die-backside problem,  caused either during back side processing or, more likely, an  insufficient cleaning of the die backside after the Tier 1 transfer  step. It is interesting to note that the bond yield of the Tier 1 layers (N=2) does not suffer from the Tier 2 step (Fig 4). Indeed, extremely limited voiding can be seen for the Tier 1 interface  compared to the tier 2 interface (Fig 5 A&B). Due to the die  thickness, after transfer of the second die-layer it is difficult to  distinguish between a single die layer or a double die layer. The  SAM measurement clearly reveals the missing dies (Fig 5B & 7). Further visualization of the double die stacks can be provided  with IR microscopy (Fig 5C) and SEM imaging (Fig 5D).


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Figure 5. A) SAM of N=2 interface, B) SAM of the N=3  interface, C) optical image of 2 misaligned dies, D) SEM  of 2 well aligned dies.


V. CONCLUSIONS 

Although a lot of work has been published in collective dieto-wafer bonding, truly little has been done on using this flow  for multi-tier die stacking. Within this publication it is shown  that the proposed imec collective-die-to-wafer bonding flow, including laser debonding with laser release layer and acoustic  layer, can be extended to the multi-tier level. Although much  optimization still needs to be done, mostly regarding die  cleaning, several N=3 stacks were prepared with transfer yields  up to 93% and bond yields up to 90%. Similar die-to-target  wafer alignment results can be obtained as for the tier 1 level  (Majority of the dies below 2 µm). Further extension to the N=4  level was less successful as the transfer yield decreased to 48%  with much lower bond yield (~80%). Finally, an N=3 stack was  built with hybrid bond pads and TSVs to evaluate the hybrid  bond interface between die 1 and die 2 using cross sectional  SEM, which shows excellent connectivity between the 2 dies  for the 5 µm pitch.

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