2018
DOI: 10.1002/qute.201800038
|View full text |Cite
|
Sign up to set email alerts
|

The Effect of Lattice Damage and Annealing Conditions on the Hyperfine Structure of Ion Implanted Bismuth Donors in Silicon

Abstract: This study reports on high energy bismuth ion implantation into silicon with a particular emphasis on the effect that annealing conditions have on the observed hyperfine structure of the Si:Bi donor state. A suppression of donor bound exciton, D0X, photoluminescence is observed in implanted samples which have been annealed at 700 °C relating to the presence of a dense layer of lattice defects that is formed during the implantation process. Hall measurments at 10 K show that this implant damage manifests itself… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
6
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
5
2

Relationship

2
5

Authors

Journals

citations
Cited by 8 publications
(6 citation statements)
references
References 30 publications
(34 reference statements)
0
6
0
Order By: Relevance
“…Far from the clock transition, the measurements from the 3D resonator match well with the results from the microresonators, while at the 7.3 GHz clock transition a linewidth of approximately 0.5 MHz is seen, equivalent to a HWHM in A of 0.1 MHz, enabling Si isotope shifts to be resolved (see the Supplemental Material [22]). The difference in the distribution of hyperfine couplings from bulk-doped Si and the ionimplanted samples studied here could be caused either by the 100× higher bismuth-donor concentration and/or residual strain from ion implantation [20]. For spins in silicon beneath patterned microresonators, strain is known to arise from the different coefficients of thermal expansion (CTEs) of the various materials.…”
Section: Pulsed Esrmentioning
confidence: 93%
See 1 more Smart Citation
“…Far from the clock transition, the measurements from the 3D resonator match well with the results from the microresonators, while at the 7.3 GHz clock transition a linewidth of approximately 0.5 MHz is seen, equivalent to a HWHM in A of 0.1 MHz, enabling Si isotope shifts to be resolved (see the Supplemental Material [22]). The difference in the distribution of hyperfine couplings from bulk-doped Si and the ionimplanted samples studied here could be caused either by the 100× higher bismuth-donor concentration and/or residual strain from ion implantation [20]. For spins in silicon beneath patterned microresonators, strain is known to arise from the different coefficients of thermal expansion (CTEs) of the various materials.…”
Section: Pulsed Esrmentioning
confidence: 93%
“…1(b)]. Samples are annealed at 900 • C for 5 min to incorporate the bismuth atoms into the silicon lattice, forming spin-active donors with an efficiency of approximately 60% [20]. We place the resonators inside a copper 3D box in a setup similar to that used in Ref.…”
Section: Resonators and Spin Systemmentioning
confidence: 99%
“…As these specifics are dependent on the species and target of interest we leave possible simplifications to the reader. It has been shown previously that Bi implanted at a high energy into silicon (therefore creating many lattice defects) can be electrically activated to a high enough quality that the donor electron spin states are measurable [16]. This demonstrates the feasibility of ion implantation as the means creating the qubits of interest here.…”
Section: Results Of Optimising Cluster Probabilitymentioning
confidence: 54%
“…We fabricated composite devices where a silicon substrate is ion implanted by Bi + at a density of ∼10 17 cm −3 in the top ∼ 1 µm before being annealed for 5 mins at 900 • C [19]. It is then coated by a 50 nm layer of Al 2 O 3 deposited at 150 • C by ALD immediately after RCA cleaning.…”
mentioning
confidence: 99%