transient liquid phase bonding technology of bi-ni …imapsne.org/virtualcds/2019/2019...

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Differential scanning calorimetry (DSC) analysis Overview Due to environmental issues, the use of Pb in electronics packaging is restricted. We are developing Bismuth-Nickel transient liquid phase bonding (TLPB) as a joining method for components in high temperature electronics as a substitute for Pb-based solders. This technique can be used for SiC modules in power electronics (over 500°C), automotive underwood electronics and downhole drilling equipment. Pure Bi with melting temperature of 271 ˚C is quite brittle due to its rhombohedral crystal structure and exhibits low thermal conductivity. By TLP bonding we are able to produce Bi-Ni intermetallic compounds with higher temperature capabilities (up to 614°C). TLPB can be made by sputtered Bi thin film on Au layer (70 nm for Ni protection). On heating process, Bi melts and reacts to Ni to form a structure of intermetallic compounds with higher melting temperature than Bi. Intermetallic phase forms via isothermal solidification in bond region during reflow. It was shown that temporal evaluation of two intermetallic phases, Bi 3 Ni and BiNi, along with the remaining Bi, are responsible for the mechanical properties and durability of TLPB [1-3]. Method Bonding component Si Die Bi-Ni TLP bonding Reflow process Transient liquid phase bonding technology of Bi-Ni system for high-temperature packaging applications Hamid Fallahdoost, Preeth Sivakumar and Junghyun Cho Binghamton University, Department of Mechanical Engineering, Materials Science and Engineering Program, Binghamton, NY 13902 Ni Ni Bi(s) Ni Ni Bi(l) Ni Ni Bi(l) Ni Ni Bi(l) IMC IMC Ni Ni IMC Solid Interlayer Melting Dissolution/Widening Isothermal Solidification (Start) Isothermal Solidification (Finish) Heating Starts Reaching 271 ˚C Heating above 271 ˚C Holding at Bonding Temperature Cooling Temperature T Bonding T m Bi Bonding IMCs : Bi 3 Ni, BiNi Sputtered Bi on Si die Backside metallization Ti (70 nm) / Ni (1000 nm) / Au (70 nm) dimensions: 1/8” x 1/8” i) Thin film approach Sputtering target from Angstrom Sciences (pure Bi, 99.999%) RF sputter 60 s pre-heat Deposition rate: ~ 0.5 μm per min Bi sputtered sandwich sample Schematic of the reflow furnace used in this research Microstructural evaluation on bonded area Schematic of IMC growth during reflow process [4] References 1. S. Marauska, et. al., Microsys Technol, 19 (2013), 1119. 2. Y. Li, et. al., Mater Sci Eng R, 51 (2006), 1. 3. H. Ma, et. al., Mater Sci, 44 (2009), 1141. 4. Sheikhi, R., Cho, J. Journal of Materials Science: Materials in Electronics, 29(22)(2018), 19034. 5. N. S. Bosco, et. al., Acta Materiala, 52 (2014), 2965. Acknowledgements Special thanks to Prof. Cotts and his research group for the reflow setup system and experiments. All characterizations were done in The Analytical and Diagnostics Laboratory (ADL) at ITC, Binghamton University. ii) Bismuth preform Pure Bi pieces cut from its ingot rod (99.999%; Goodfellow, Huntington, UK) were used as an interlayer. 1) Nucleation of Bi 3 Ni 2) Melting of pure Bi 3) Nucleation of BiNi 4) Melting of Bi 3 Ni 5) Undercooling of Bi 3 Ni 6) Nucleation of BiNi 7) Melting of Bi 3 Ni Peak Label Polarized OM 20 μm 20 μm Bi preform between two Si die (Ni) reflowed at 330 in vacuum furnace with 1-2 as heating rate 0 min reflow time 5 min reflow time Shear strength vs. reflow time 60 min reflow time 20 μm BSD investigation 0 min reflow time 10 min reflow time 5 μm 5 μm Remaining Ni; showing all of the Ni not consumed with the reaction during the reflow cycle. Enriched with Bi; Ni concentration was Not enough to form IMC BiNi band with darker contrast; Bi and Ni concentration were close to each other as a proof to form BiNi IMC. Bi 3 Ni formed as dominant IMC; Bi to Ni proportion in at.% close to 3 to 1; Bi 3 Ni forms first with either bulk or interface nucleation depending on the remaining of a Ni layer; BiNi forms at the interface between Bi 3 Ni and Ni with slower growth kinetics compared to that of Bi 3 Ni. With decreasing the thickness of Bi as an interlayer, a continuous crack can be seen due to shrinkage related to phase transformation to IMC. With increasing heating rate, thinner TLP bonds could be achieved based on the calculation above. Best bonding maintaining good mechanical reliability could contain a full IMC layer with a remaining Ni layer on the Si die. Conclusion Parameters affecting TLP bond quality Surface cleaning before reflow to remove an oxide scale Heating rate; increasing heating rate could avoid forming IMC before reaching to the melting point of interlayer. Optimum thickness of interlayer [5]; = 2ℎ × ( Τ ) 2 = 2ℎ × (1.075) = 2 X Bi = 9.533 Y Ni 0 5 10 15 20 25 30 35 40 45 50 0 20 40 60 80 Optimum thickness (μm) Heating rate (c/s) Bismuth Nickel Parameter Description Value Mass fraction of interlayer for Bi 3 Ni, (%) 91.43 Density of IMC (Bi 3 Ni), (ൗ ) 10.9 Density of interlayer (Bi) near m. p., ( ) 10.05 Growth constant, (μm 2 /s) 0.927 Q Activation energy around m. p. , (kJ/mol) 132.9 For growth of Bi 3 Ni 15.23 22.25 25.46 20.92 11.58 0 5 10 15 20 25 30 Max shear stress (MPa) Axis Title 0 min 5 min 10 min 20 min 60 min Bi sputtered sandwich sample Reflow at 330for 30 min with 65 Τ as heating rate Max shear strength 15 MPa SE BSD 20 μm 10 min reflow time

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Page 1: Transient liquid phase bonding technology of Bi-Ni …imapsne.org/virtualCDs/2019/2019 Posters/E4.pdfHamid Fallahdoost, Preeth Sivakumar and Junghyun Cho Binghamton University, Department

Differential scanning calorimetry (DSC) analysis

OverviewDue to environmental issues, the use of Pb in electronics packaging isrestricted. We are developing Bismuth-Nickel transient liquid phasebonding (TLPB) as a joining method for components in hightemperature electronics as a substitute for Pb-based solders. Thistechnique can be used for SiC modules in power electronics (over500°C), automotive underwood electronics and downhole drillingequipment. Pure Bi with melting temperature of 271 ˚C is quitebrittle due to its rhombohedral crystal structure and exhibits lowthermal conductivity. By TLP bonding we are able to produce Bi-Niintermetallic compounds with higher temperature capabilities (up to614°C). TLPB can be made by sputtered Bi thin film on Au layer (70nm for Ni protection). On heating process, Bi melts and reacts to Nito form a structure of intermetallic compounds with higher meltingtemperature than Bi. Intermetallic phase forms via isothermalsolidification in bond region during reflow. It was shown thattemporal evaluation of two intermetallic phases, Bi3Ni and BiNi,along with the remaining Bi, are responsible for the mechanicalproperties and durability of TLPB [1-3].

Method

Bonding component

Si Die

Bi-Ni TLP bonding

Reflow process

Transient liquid phase bonding technology of Bi-Ni system for high-temperature packaging applicationsHamid Fallahdoost, Preeth Sivakumar and Junghyun Cho

Binghamton University, Department of Mechanical Engineering, Materials Science and Engineering Program, Binghamton, NY 13902

Ni NiBi(s)

Ni NiBi(l)

Ni NiBi(l)

Ni NiBi(l)IMC IMC

Ni NiIMC

Solid Interlayer

Melting

Dissolution/Widening

Isothermal Solidification (Start)

Isothermal Solidification (Finish)

Heating

Starts

Reaching 271 ˚C

Heating

above 271 ˚C

Holding at

Bonding

Temperature

Cooling

Tem

per

atu

re

TBonding

Tm Bi

Bonding

IMCs : Bi3Ni, BiNi

Sputtered Bi on Si dieBackside metallization

Ti (70 nm) / Ni (1000 nm) / Au (70 nm)

dimensions: 1/8” x 1/8”

i) Thin film approach

Sputtering target from Angstrom Sciences (pure Bi, 99.999%)• RF sputter• 60 s pre-heat• Deposition rate: ~ 0.5 µm per min

Bi sputtered sandwich sample

Schematic of the reflow furnace used in this research

Microstructural evaluation on bonded area

Schematic of IMC growth during reflow process [4]

References1. S. Marauska, et. al., Microsys Technol, 19 (2013), 1119.2. Y. Li, et. al., Mater Sci Eng R, 51 (2006), 1.3. H. Ma, et. al., Mater Sci, 44 (2009), 1141.4. Sheikhi, R., Cho, J. Journal of Materials Science: Materials in Electronics, 29(22)(2018), 19034.5. N. S. Bosco, et. al., Acta Materiala, 52 (2014), 2965.

Acknowledgements• Special thanks to Prof. Cotts and his research group for the reflow setup system and

experiments.• All characterizations were done in The Analytical and Diagnostics Laboratory (ADL) at ITC,

Binghamton University.

ii) Bismuth preform

Pure Bi pieces cut from its ingot rod (99.999%; Goodfellow, Huntington, UK)

were used as an interlayer.

1) Nucleation of Bi3Ni2) Melting of pure Bi

3) Nucleation of BiNi

4) Melting of Bi3Ni5) Undercooling of Bi3Ni6) Nucleation of BiNi

7) Melting of Bi3Ni

Peak Label

Polarized OM

20 µm

20 µm

Bi preform between two Si die (Ni) reflowed at 330 ℃ in vacuum furnace with 1-2 ℃ ∕𝒔 as heating rate

0 min reflow time

5 min reflow time

Shear strength vs. reflow time

60 min reflow time20 µm

BSD investigation0 min reflow time 10 min reflow time

5 µm

5 µm

Remaining Ni; showing all of the Ninot consumed with the reaction duringthe reflow cycle.

Enriched with Bi; Ni concentration was

Not enough to form IMC

BiNi band with darker contrast; Bi and Ni

concentration were close to each other as

a proof to form BiNi IMC.

Bi3Ni formed as dominant IMC;

Bi to Ni proportion in at.% close to 3 to 1;

➢ Bi3Ni forms first with either bulk or interface nucleation depending on the remaining of a Nilayer; BiNi forms at the interface between Bi3Ni and Ni with slower growth kineticscompared to that of Bi3Ni.

➢ With decreasing the thickness of Bi as an interlayer, a continuous crack can be seen due toshrinkage related to phase transformation to IMC. With increasing heating rate, thinner TLPbonds could be achieved based on the calculation above.

➢ Best bonding maintaining good mechanical reliability could contain a full IMC layer with aremaining Ni layer on the Si die.

Conclusion

Parameters affecting TLP bond quality• Surface cleaning before reflow to remove an oxide scale• Heating rate; increasing heating rate could avoid forming IMC before reaching to the

melting point of interlayer.• Optimum thickness of interlayer [5];

ℎ𝑂𝑝𝑡𝑖𝑚𝑢𝑚 = 2ℎ𝐼𝑀𝐶 × 𝐶𝐴( Τ𝜌𝐼𝑀𝐶 𝜌𝐵𝑖)2 ℎ𝑂𝑝𝑡𝑖𝑚𝑢𝑚 = 2ℎ𝐼𝑀𝐶 × (1.075) ℎ𝐼𝑀𝐶= 2𝑘𝑝𝑡ℎ𝑒𝑎𝑡

XBi = 9.533 YNi

0

5

10

15

20

25

30

35

40

45

50

0 20 40 60 80

Op

tim

um

th

ick

nes

s (µ

m)

Heating rate (c/s)

Bismuth

NickelParameter Description Value

𝑪𝑨 Mass fraction of interlayer for Bi3Ni, (%) 91.43

𝝆𝑰𝑴𝑪 Density of IMC (Bi3Ni), ( ൗ𝒈

𝒄𝒎𝟑) 10.9

𝝆𝑩𝒊 Density of interlayer (Bi) near m. p., ( ൗ𝒈

𝒄𝒎𝟑) 10.05

𝑲𝒑 Growth constant, (µm2/s) 0.927

Q Activation energy around m. p. , (kJ/mol) 132.9

For growth of Bi3Ni

15.23

22.25

25.46

20.92

11.58

0

5

10

15

20

25

30

Ma

x s

hea

r st

ress

(M

Pa

)

Axis Title

0 min 5 min 10 min 20 min 60 min

Bi sputtered sandwich sampleReflow at 330℃ for 30 min with 65 Τ℃ 𝒔 as heating rate

Max shear strength ≈ 15 MPa

SE

BSD

20 µm 10 min reflow time