Model for Electric Potential for Gate Electrodes in a Quantum Bus (1): Difference between revisions
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Description: homogeneous Poisson's equation for electric potential<br /> | Description: homogeneous Poisson's equation for electric potential<br /> | ||
Defining formulation:<br /> | Defining formulation:<br /> | ||
<!--<math>-\nabla \cdot ( \varepsilon(\boldsymbol{r}) \nabla \Phi(\boldsymbol{r},t)) = 0</math> | <!--<math>-\nabla \cdot ( \varepsilon(\boldsymbol{r}) \nabla \Phi(\boldsymbol{r},t)) = 0</math>--> | ||
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| time-dependent profile of the electric potential in the quantum bus | | time-dependent profile of the electric potential in the quantum bus | ||
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| <math>\varepsilon</math> | | <!--<math>\varepsilon</math>--> | ||
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| static dielectric permittivity of a material | | static dielectric permittivity of a material | ||
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| position vector used for description of fields | | position vector used for description of fields | ||
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Description: definition of static dielectric permittivity of a material by the relative permittivity<br /> | Description: definition of static dielectric permittivity of a material by the relative permittivity<br /> | ||
DefiningFormulation:<br /> | DefiningFormulation:<br /> | ||
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<math>\varepsilon(\boldsymbol{r}) = \varepsilon_0 \varepsilon_r(\boldsymbol{r})</math> | <math>\varepsilon(\boldsymbol{r}) = \varepsilon_0 \varepsilon_r(\boldsymbol{r})</math> | ||
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Revision as of 10:31, 15 April 2024
Title: "Model for Electric Potential for Gate Electrodes in a Quantum Bus"
Authors:
- family-names: Koprucki
given-names: Thomas
orcid: https://orcid.org/0000-0001-6235-9412
- family-names: Shehu
given-names: Aurela
orcid: https://orcid.org/0000-0002-1994-0612
Date-Released: 2024-04-05
Version: 1.0.0
Mathematical Model MM1: Electron Shuttling Model
Description: The gate electrodes form an electric potential landscape that generates an array of QDs in the QW. Suitable pulsing allows to propagate the QDs along the channel and thus enables conveyor-mode shuttling. As the device is operated at deep cryogenic temperature (50 mK), there exist no thermally activated electrons in the conduction band and space charge regions can be safely neglected. In this case, the electric potential obeys the homogeneous Poisson equation.
Properties: Is Deterministic, Is Space-Continous, Is Time-Continous, Is Linear
List of Mathematical Formulations
F1: Poisson's equation
Description: homogeneous Poisson's equation for electric potential
Defining formulation:
Symbol | Quantity | Quantity Id | Quantity Kind | Quant. Kind Id | Description |
---|---|---|---|---|---|
- | - | Electric Potential | Q55451 | time-dependent profile of the electric potential in the quantum bus | |
- | - | Permittivity | Q211569 | static dielectric permittivity of a material | |
- | - | Position | Q192388 | position vector used for description of fields | |
- | - | Time | Q11471 | time |
F2: Permittivity law
Description: definition of static dielectric permittivity of a material by the relative permittivity
DefiningFormulation:
Relations between Mathematical Formulations and Computational Tasks:
F2 Contained As Assumption In CT1.
F3 Contained As Boundary Condition In CT1.
F4 Contained As Boundary Condition In CT1.
Publication
P1: WIAS-Preprint 3082
DOI: 10.20347/WIAS.PREPRINT.3082
Relations between Mathematical Model and Publication:
MM1 Used In P1
Relations between Computational Task and Publication:
CT1 Documented In P1
Research Field
RF1: Semiconductor Physics
WikiData: Q4483523
Research Problem
RP1: Electrostatics in a Si/SiGe quantum bus
Description: Simulation of the electrostatics in a Si/SiGe quantum bus