Damage formation and annealing studies of low energy ion implants ...

Damage formation and annealing studies of low energy ion implants ... Damage formation and annealing studies of low energy ion implants ...

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The energy spectra have been converted into depth profiles. The profiles for both the NoPAI and PAI samples are shown in Figure 6.4a) and 6.4b) for As and Si, respectively. Figure 6.4 b) shows that the 3 keV As implant produces a ∼11 nm deep amorphous layer, as evidenced by the extra Si scattering yield behind the surface peak that reaches the random level and extends to a depth of ∼11 nm (half height). Arsenic implant profiles for the PAI and NoPAI implants are in close agreement. This is expected since Si is amorphised after a As dose of 10 14 cm -2 (14, chapter 5). MEIS shows that the peak of the As distribution is at 6.3 nm depth, in close agreement with TRIM calculations that yield an Rp = 6.4 nm (profiles not shown). Following a 600 °C 20 min anneal the amorphous layer has recrystallised by SPER. The regrowth is not perfect, leaving a surface damage peak of greater width (5 nm) than the surface peak width of the virgin sample (2.5 nm) and greater height. The As profile too has undergone considerable change with the disappearance from “ beam view” of most of the As in the implanted profile and the appearance of a narrow, segregated As peak with a maximum at a depth of 3 nm. The former is due to As taking up substitutional positions within the regrown Si, where it is no longer visible to the beam. The latter is due to the As concentration that exceeds the solid solubility and cannot be accommodated in the regrown layer due to solid solubility restrictions, although the operation of a simple activated segregation process cannot be excluded. In either case it is “snowploughed” ahead of the advancing amorphous/ crystalline interface and forms the segregated surface peak (7). 125

a) b) c) Yield (counts per 5 µC) Yield (counts per 5 µC) 100 90 80 70 60 50 40 30 20 10 0 0.0 0 2 4 6 8 10 12 14 16 300 250 200 150 100 50 Yield (counts per 5 µC) As depth Depth (nm) 126 3 keV as-impl As 3 keV 600C 20mins As 3 keV 1130C spike As 3 keV as-impl PAI As 3 keV 600C 20mins PAI As 3 keV 1130C spike PAI As 0 0 0 2 4 6 8 Depth (nm) 10 12 14 16 180 160 140 120 100 80 60 40 20 Si depth PAI, 1130C spike anneal virgin as-implanted 600C 20m 1130C spike PAI as-implanted PAI 600C 20m PAI 1130C spike 3.5x10 21 3.0x10 21 2.5x10 21 2.0x10 21 1.5x10 21 1.0x10 21 5.0x10 20 5x10 22 4x10 22 3x10 22 2x10 22 1x10 22 0 0 2 4 6 Depth (nm) 8 10 Figure 6.4 MEIS depth profiles along the [111] blocking direction a) As depth profiles for all the annealed samples. b) Si depth profiles for all the annealed samples. c) Combined depth profile of As, Si and O for the PAI 1130 °C spike annealed sample. As Si O Concentration (at/cm 3 ) concentration (at/cm 3 )

The <strong>energy</strong> spectra have been converted into depth pr<strong>of</strong>iles. The pr<strong>of</strong>iles for both<br />

the NoPAI <strong>and</strong> PAI samples are shown in Figure 6.4a) <strong>and</strong> 6.4b) for As <strong>and</strong> Si,<br />

respectively. Figure 6.4 b) shows that the 3 keV As implant produces a ∼11 nm deep<br />

amorphous layer, as evidenced by the extra Si scattering yield behind the surface peak<br />

that reaches the r<strong>and</strong>om level <strong>and</strong> extends to a depth <strong>of</strong> ∼11 nm (half height). Arsenic<br />

implant pr<strong>of</strong>iles for the PAI <strong>and</strong> NoPAI <strong>implants</strong> are in close agreement. This is<br />

expected since Si is amorphised after a As dose <strong>of</strong> 10 14 cm -2 (14, chapter 5). MEIS<br />

shows that the peak <strong>of</strong> the As distribut<strong>ion</strong> is at 6.3 nm depth, in close agreement with<br />

TRIM calculat<strong>ion</strong>s that yield an Rp = 6.4 nm (pr<strong>of</strong>iles not shown). Fol<strong>low</strong>ing a 600 °C<br />

20 min anneal the amorphous layer has recrystallised by SPER. The regrowth is not<br />

perfect, leaving a surface damage peak <strong>of</strong> greater width (5 nm) than the surface peak<br />

width <strong>of</strong> the virgin sample (2.5 nm) <strong>and</strong> greater height. The As pr<strong>of</strong>ile too has<br />

undergone considerable change with the disappearance from “ beam view” <strong>of</strong> most <strong>of</strong><br />

the As in the implanted pr<strong>of</strong>ile <strong>and</strong> the appearance <strong>of</strong> a narrow, segregated As peak with<br />

a maximum at a depth <strong>of</strong> 3 nm. The former is due to As taking up substitut<strong>ion</strong>al<br />

posit<strong>ion</strong>s within the regrown Si, where it is no longer visible to the beam. The latter is<br />

due to the As concentrat<strong>ion</strong> that exceeds the solid solubility <strong>and</strong> cannot be<br />

accommodated in the regrown layer due to solid solubility restrict<strong>ion</strong>s, although the<br />

operat<strong>ion</strong> <strong>of</strong> a simple activated segregat<strong>ion</strong> process cannot be excluded. In either case it<br />

is “snowploughed” ahead <strong>of</strong> the advancing amorphous/ crystalline interface <strong>and</strong> forms<br />

the segregated surface peak (7).<br />

125

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