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JAEA-Review-2010-065.pdf:15.99MB - 日本原子力研究開発機構

JAEA-Review-2010-065.pdf:15.99MB - 日本原子力研究開発機構

JAEA-Review-2010-065.pdf:15.99MB - 日本原子力研究開発機構

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1-03<br />

Evaluation of Soft Error Rates in SOI SRAM with<br />

a Technology Node of 90 nm Using Oxygen Ion Probe<br />

S. Abo a) , N. Masuda a) , F. Wakaya a) , S. Onoda b) , T. Makino b) , T. Hirao b) ,<br />

T. Ohshima b) , T. Iwamatsu c) , H. Oda c) and M. Takai a)<br />

a) Center for Quantum Science and Technology under Extreme Conditions, Osaka University,<br />

b) Environment and Industrial Materials Research Division, QuBS, <strong>JAEA</strong>,<br />

c) Advanced Device Development Department, Renesas Technology Corporation<br />

A soft error or bitstate upset due to the excess charge<br />

carriers generated by high energy incident particles becomes<br />

a serious problem in advanced semiconductor devices. A<br />

silicon-on-insulator (SOI) device has an advantage over the<br />

conventional bulk device for the soft error, in which a<br />

device region is insulated from the silicon substrate by a<br />

buried oxide (BOX) layer and the excess charge carriers in<br />

the silicon substrate are not accumulated to the drain<br />

electrode. However, the generated excess carriers in a SOI<br />

body are kept at the channel region in the SOI body or<br />

accumulated to the drain and source electrodes. The<br />

generated holes in the channel region of an n-channel SOI<br />

metal oxide semiconductor field effect transistor (MOSFET)<br />

increase the SOI body potential, which results in a floating<br />

body effect and the soft error. The floating body effect can<br />

be suppressed by a body-tie structure, in which the SOI<br />

body regions are connected to the source electrode. The<br />

body electrode subtracts the generated excess carriers from<br />

the channel region and suppresses the floating body effect.<br />

In this study, the difference in soft error rates (SERs) of<br />

SOI SRAM with a technology node of 90 nm was<br />

investigated by oxygen ion probes with energies ranging<br />

from 9.0 to 18.0 MeV. The memory cell included 4<br />

n-MOSFETs sand 2 p-MOSFETs. The memory cell size,<br />

the memory capacity and the critical charge of SOI SRAM<br />

were 1.25 m 2 , 8 Mbits and 1.8 fC, respectively. The<br />

thicknesses of the SOI body and the BOX layer were 75 and<br />

145 nm. The over-layers were 4 copper metal and<br />

polyimide passivation layers without top plastic mould.<br />

The body-tie structure was used for suppressing the floating<br />

body effect. The amount of soft error in SRAM was<br />

monitored after oxygen ion probe irradiation. The dose<br />

Normalized SER<br />

2.0<br />

1.5<br />

1.0<br />

0.5<br />

0.0<br />

8 10 12 14 16 18<br />

Energy (MeV)<br />

Fig. 1 SERs as a function of oxygen ion energy for the<br />

SOI SRAMs. The values of SER were normalized to<br />

the error bits by 12 MeV oxygen ion irradiation.<br />

<strong>JAEA</strong>-<strong>Review</strong> <strong>2010</strong>-065<br />

- 7 -<br />

rates of oxygen probes for each of the energies were<br />

monitored by a solid state detector before irradiation. The<br />

minimum and maximum dose rates were 50 and 930 cps.<br />

The beam spot sizes were less than 1 m. The scanned<br />

areas were calculated from secondary electron images.<br />

The minimum and maximum scanned areas were 220 ×<br />

187 m 2 and 327 × 275 m 2 , respectively. The irradiation<br />

time was adjusted for less than 1 oxygen ion hit to 1 SRAM<br />

cell from the dose rate and the scanned area.<br />

Figure 1 shows SERs as a function of oxygen ion energy<br />

in SOI SRAM. The values of SER were normalized to the<br />

error bits for those by 12 MeV oxygen ion irradiation. No<br />

soft error occurred in SOI SRAM with oxygen ion energies<br />

of less than 10.0 MeV. This indicates that the oxygen ions<br />

with energies of less than 10.0 MeV were shielded by the<br />

over-layers of MOSFET. Soft error rates started to<br />

increase at 10.5 MeV and gradually saturated with energies<br />

above 13.5 MeV. Figure 2 shows the generated charge in<br />

the SOI body in SOI SRAM as a function of oxygen ion<br />

energy simulated by SRIM code. The energy loss through<br />

the over-layers was corrected by the designed thickness.<br />

The oxygen ions with energies less than 12.5 MeV<br />

generated less excess charge carriers than the critical charge.<br />

Therefore the soft error in SOI SRAM by oxygen ion<br />

irradiation with energies at end below 12.5 MeV shown in<br />

Fig. 1 occurred by the floating body effect due to the<br />

generated excess charge carriers in the channel regions.<br />

The oxygen ions with energies at end above 13.0 MeV<br />

generated more excess charge carriers than the critical<br />

charge, in which the soft error was induced by both the<br />

floating body effect and these excess carriers at the storage<br />

nodes.<br />

Generated Charge in SOI Body (fC)<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

0<br />

8 10 12 14 16 18<br />

Energy (MeV)<br />

Fig. 2 Generated charge in the SOI body as a function<br />

of oxygen ion energy in the SOI SRAM.

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