nanostrutture a base di si e ge per - cineca · 2014. 2. 26. · a. debernardi i bandi lisa 2014...

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Alberto Debernardi Laboratorio MDM, IMM-CNR Agrate Brianza (Italy) – www.mdm.imm.cnr.it Nanostrutture a base di Si e Ge per nuovi dispositivi nano-elettronici

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Shallow Si:P impurity for quantum computingAgrate Brianza (Italy) – www.mdm.imm.cnr.it
Nanostrutture a base di Si e Ge per nuovi dispositivi nano-elettronici
2A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
Plan of the talk
• P or Se doped Si-nanowires for quantum computing
• Delocalization of P(Se) wave-function Si NW [001], [011], [111] oriented
• Ab initio spectroscopy (Hyperfine parameters, MOKE)
• Conclusion and Discussion
Scaling down of CMOS logic devices
The number of components in a
single chip doubles every 18 months
Moore’s law
Scaling down of CMOS logic devices
INTEL Presentation SPIE 03/2003
International Technology Roadmap for
constantemente …
Scaling down of electronic devices
Nanodevices whose size
• Grafene (C)
• Silicene (Si)
• Germanene (Ge)
• Stanene (Sn)
Dispositivi ultra-veloci
Nuovi Sensori
Nuova elettronica
Si-Nanostructures Applications
Nanosensors (DNA, ...)
8A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
Density Functional Theory
E[n]rv

r'nrn ε=E[n]
functional of the density
Single atom electronics: Se impurity
Se doped H passivated Si nanowires
(nanoelectronics, quantum computer)
Nanowire passivation
H passivated Si nanowires
Se doped Si nanowires
• Correction to periodically repeated charged imeges (Rurali et al, Makov-Payne)
13A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
Band-gap of Si nano-wire
Band-gap as a function of NW diameter
As an effect of
Delocalization of donor wave-funnction
Delocalization of donor wave-funnction
2010).
same qualitative results
Delocalization of donor wave-function
• The of Se wave-function for [011] should be extrapolated
, = − 2 +
17A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
Delocalization of donor wave-function
….we suggest it is a general tends 0 5 10
[001]
[011]
[111]
Se
P
[001] <
[111] < [011]
direction …
Strain along the NW axis
• The of Se: non linear dependence of the strain
• The of P: strong dependence
Modification of shallow wave-function by strain
19A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
Strain along the NW axis • P
+6%
Unstrained
-6%
piezoelectrical
actuators
• Se
Conclusions
• The [011] is the best direction for nano-electronic and quantum computing applications
• Stress allow to tune delocalization
• The [011] is the best direction for nano-electronic and quantum computing applications
• Stress allow to tune delocalization
21A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
Ab initio spectroscopy
• Individua i meccanismi microscopici responsabili di una data proprietà
• Predice quali sono le condizioni ottimali per ottenere un dato fenomeno
• E’ più economica di un «vero» esperimento
22A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
Ab initio spectroscopy: MOKE
• Simulation of relatively large systems
----- our work
**** experiment Bulk Fe
Ab initio spectroscopy: XAS
spintronic applications (film di 29 nm)
Interazione luce-materia, predizioni
senza parametri aggiustabili
Hyperfine coupling constant: Charged defects
Hyperfine interaction requires a spin density≠0
Ionization of the impurity dipiso AAA 1
)()( 3
Si(Ge) dots:S+ contact term Si-NC:S+ (1)
Si-NC:S+ (2)
Single atom electronics: Se impurity
Se doped H passivated Si nanowires
(nanoelectronics, quantum computer)
Hyperfine coupling constants: axial Se
-1
0
1
2
3
4
5
6
7
d
(nm)
Aiso
(GHz)
b
(MHz)
NW1
NW2
NW3
NW4
NW5
NW6
negligible (< 0.22) for all the others
Confinement enhances the hyperfine coupling constant
Central impurity
Se doped Si-NW
• HFC couples nuclear and electron spin
• Quantum bits (qu-bits) are stored in the nuclear spin of Se atom
Distortion of NW
Isotropic Hyperfine Coupling
• STRONG DEPENDENCE OF HYPERFINE CONSTANT ON IMPURITY SITE
• It is possible to DETERMINE the POSITION of the impurity (Se) on the basis of EPR SPECTRA
30A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
Silicane: Si@H
Magnetic Semiconductor
Si@H: Proprietà Ottiche • Magneto Optical
Kerr Effect
Conclusions
• The position of the impurity can be determined by comparing EPR spectra with ab initio data
• MOKE signal in 2D for future nano-electronic devices
• La Simulazione è MOLTO più economica dell’esperimento
• Possiamo «inventare» nuovi materiali e modificarne le proprietà per una nuova elettronica.
33A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
A special thanks to
• D.Douma, D.Sangalli (IMM-CNR)
• M. Fanciulli (UNIMIB, MDM) and to all experimentalists at the MDM laboratory.
• LISA for computational resources ....
34A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
S doped Si Nano Dots
35A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
Se doped Si NW: Formation Energy
• Subsurface position is energergetic ally favoured (at least for small diameter)
• Effect of distortion for small diameters
36A. Debernardi I bandi LISA 2014 …, Milano 18.2.2014
Stability of ionized Se
• Formation energy of the defect on the axis of the nanowire as a function of the chemical potential.
• The three graphs represent the three different nanowires with diameter 1.2 nm, 1.5 nm, 2.0 nm respectively.