PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D,...

17
. . . . ' . ' . . . NASA Electronic Parts and Packaging (NEPP) Program PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs [email protected] Deliverable to NASA Electronic Parts and Packaging (NEPP) Program to be published on nepp.nasa.gov originally presented by Alexander Teverovsky at the 7th International Conference on Electroceramics (ICE'15), May 13-16, 2015, State College PA. https://ntrs.nasa.gov/search.jsp?R=20150010724 2020-02-21T06:03:38+00:00Z

Transcript of PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D,...

Page 1: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

. . .

N~. . ' . '

. . . NASA Electronic Parts and Packaging (NEPP) Program

PME and BME Ceramic Capacitors

Alexander Teverovsky AS&D, Inc.

Alexander .A. Teverovs [email protected]

Deliverable to NASA Electronic Parts and Packaging (NEPP) Program to be published on nepp.nasa.gov originally presented by Alexander Teverovsky at the 7th International Conference on Electroceramics (ICE'15), May 13-16, 2015, State College PA.

https://ntrs.nasa.gov/search.jsp?R=20150010724 2020-02-21T06:03:38+00:00Z

Page 2: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

Ps X Co ct d

DCL E e

(/JB

HALT HT Jabs IM IR k

List of Acronyms and Sym bois

base metal electrode capacitor current density Schottky constant quasi static electric susceptibility nominal capacitance absorption capacitance thickness of the dielectric direct current leakage Electric field dielectric constant barrier heights highly accelerated life testing high temperature absorption current infant mortality insulation resistance Boltzmann constant

J.l MLCC

nv PME

Qt RT (T

s SCLC

tel

TTF u

VBR VBRd VBR.

I v ++ 0

VR

apacitor constant

-----,

mobility of electrons multilayer ceramic c voltage acceleration precious metal elect absorption charge room temperature surface charge dens

rode capacitor ~

ity surface area space charge leakag electrification time time to failure

e current

activation energy of leakage currents breakdown voltage breakdown voltage due to defects intrinsic breakdown voltage charged oxygen vacancy rated voltage

Deliverable to NASA Electronic Parts and Packaging (NEPP) Program to be published on nepp.nasa.gov originally presented by Alexander Teverovsky at the 7th International Conference on Electroceramics (ICE'15), May 13-16, 2015, State College PA. 2

Page 3: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

Abstract

Introduction of BME capacitors to high-reliability electronics as a replacement for PM E capacitors requires better understanding of changes in performance and reliability of M LCCs to set justified screening and qualification requirements. In this work, absorption and leakage currents in various lots of commercial and military grade X7R MLCCs rated to 1 OOV and less have been measured to reveal difference in behavior of PME and BME capacitors in a wide range of voltages and temperatures. Degradation of leakage currents and failures in virgin capacitors and capacitors with introduced cracks has been studied at different voltages and temperatures during step stress highly accelerated life testing. Mechanisms of charge absorption, conduction and degradation have been discussed and a failure model in capacitors with defects suggested.

Deliverable to NASA Electronic Parts and Packaging (NEPP) Program to be published on nepp.nasa.gov originally presented by Alexander Teverovsky at the 7th International Conference on Electroceramics (ICE'15), May 13-16, 2015, State College PA. 3

Page 4: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

0 Introduction.

0 Leakage currents. • Absorption currents and room temperature IR. • Intrinsic leakage currents and high temperature IR.

0 Degradation of leakage currents during HALT. 0 Effect of cracking on degradation of leakage currents

at high temperatures. 0 Models of degradation and failures for BME

capacitors with defects. 0 Conclusion.

Deliverable to NASA Electronic Parts and Packaging (NEPP) Program to be published on nepp.nasa.gov originally presented by Alexander Teverovsky at the 7th International Conference on Electroceramics (ICE'15), May 13-16, 2015, State College PA. 4

Page 5: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

D Stability of DCL or IR at environmental testing indicates reliability of MLCCs.

D Currently, hi-rei systems employ MLCCs with Ag/Pd metal electrodes.

D Insertion of BME capacitors in hi-rei applications requires a closer look at differences in DCL for PMEs and BMEs under environmental stresses.

D Reliability issues with MLCC: • Degradation of IR related to oxygen vacancies. • Failures related to manufacturing defects. • Failures related to soldering and assembly introduced cracking. • Effect of moisture and low-voltage phenomena.

D Intrinsic wear-out failures caused by oxygen vacancies typically do not cause failures during applications. Reliability is limited by defects.

D A limited data exist on the effect of cracking on degradation of leakage currents.

Deliverable to NASA Electronic Parts and Packaging (NEPP) Program to be published on nepp.nasa.gov originally presented by Alexander Teverovsky at the 7th International Conference on Electroceramics (ICE'15), May 13-16, 2015, State College PA. 5

Page 6: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

Mfr. ap~lic EIA d, II I Part d, C, ~F 1~R, V t at1on size ~m ype ~m

0.33 50 v MIL 1825 25 1 50 BME A Gen. 25

0.33 50 PME c MIL 1825 30 1 100 PME p Hi-rei 2225 25 0.33 50 BME c Gen. 1210 12 2.2 50 BME c auto 1206 6 0.33 50 BME A Gen. 1210 16 2.2 50 BME c auto 1210 6 0.33 50 BME A auto 0805 9 2.2 50 BME A auto 1210 10 0.33 50 BME A Gen. 0805 9 2.2 100 BME A auto 1812 12

0.33 50 BME M auto 0805 7 2.2 50 PME A MIL stack 31 0.33 50 BME M Gen. 0805 7 0.1 50 BME c Gen. 1210 13 0.33 50 BME c auto 0805 6 0.1 50 BME A Gen. 1210 24 0.33 50 BME c Gen. 0805 6 0.1 50 PME c MIL 1210 24

1 10 BME A Gen. 0805 5.1 0.1 50 PME A MIL 1210 26 1 10 BME c auto 0805 3.5 0.47 50 PME v MIL 1825 22 1 10 BME M Gen. 0805 4.2 1 o.47 50 PME c MIL 1825 21 1 10 PME p Hi-rei 0805 10 1 o.47 50 BME c Gen. 1825 24

1 o.47 50 BME A Gen. 1825 28

~Six groups of similar PME and BME X7R capacitors from 5 mfrs. ~Cracks were introduced using Vickers indenter.

Deliverable to NASA Electronic Parts and Packaging (NEPP) Program to be published on nepp.nasa.gov originally presented by Alexander Teverovsky at the 7th International Conference on Electroceramics (ICE'15), May 13-16, 2015, State College PA. 6

Page 7: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

curre

nt, A

curre

nt, A

curre

nt, A

curre

nt, A

Page 8: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

char

ge, C

char

ge, C

char

ge, C

Page 9: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

abso

rptio

n cu

rrent

@60

sec,

Acu

rren

t, A

Page 10: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

m

m

curre

nt, A

curr

ent,

A

Page 11: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

J/E,

(A/c

m2)

/(V/u

m)

J/E,

(A/c

m2)

/(V/u

m)

J/E,

(A/c

m2 )

/(V/u

m)

Page 12: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

activ

atio

n en

ergy

, eV

activ

atio

n en

ergy

, eV

activ

atio

n en

ergy

, eV

Page 13: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

curre

nt, A

curre

nt, A

Page 14: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

curre

nt, A

curre

nt, A

curre

nt, A

Page 15: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

cumula

tive pr

obabi

lity, %

Page 16: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

cumula

tive p

robab

ility, %

Page 17: PME and BME Ceramic Capacitors - NASA · PME and BME Ceramic Capacitors Alexander Teverovsky AS&D, Inc. Alexander .A. Teverovs ky@nasa.gov Deliverable to NASA Electronic Parts and

Conclusion 0 At RT and V < 2VR, DCL is due to absorption processes and

depends on capacitance and quasi static electric susceptibility. IR values at RT are typically 2 times greater for PMEs than for BMEs.

0 Intrinsic leakage currents increase with voltage according to a power law with the exponent decreasing with temperature to -1.5-2 at T > 150 °C. Activation energies of DCL decrease with voltage and at VR are -1.2 eV for PMEs and -0.8 eV for BMEs.

0 Intrinsic conduction can be described using Simmons model atE> 5 V/J.lm. The difference in HT IR between military PMEs and commercial BMEs is mostly due to different barrier heights and thickness of the dielectric.

0 Cracks might not affect IR at room and/or high temperatures, but accelerate degradation of DCL in BME capacitors.

0 Currents in BME capacitors with defects might stabilize with time without causing catastrophic failures.

0 A model of DCL degradation in MLCCs with defects is suggested.

Deliverable to NASA Electronic Parts and Packaging (NEPP) Program to be published on nepp.nasa.gov originally presented by Alexander Teverovsky at the 7th International Conference on Electroceramics (ICE'15), May 13-16, 2015, State College PA. 17