H. Ingerslev Jørgensen
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Research Interests
H. Ingerslev Jørgensen has a total of 13 co-authors. Here are the top co-authors by number of shared publications:
P. E. Lindelof
Nano-Science Center, Niels Bohr Institute, University of Copenhagen, Universitetsparken 5, DK-2100 Copenhagen Ø, Denmark
8 shared publications- Kasper Grove-Rasmussen
Center for Quantum Devices, Niels Bohr Institute, University of Copenhagen, 2100 Copenhagen, Denmark
5 shared publications K. Grove-Rasmussen
Nano-Science Center Niels Bohr Institute University of Copenhagen Universitetsparken 5 DK-2100 Copenhagen Ø Denmark
4 shared publications- Karsten Flensberg
Niels Bohr Institute
4 shared publications K. Flensberg
Nano-Science Center Niels Bohr Institute University of Copenhagen Universitetsparken 5 DK-2100 Copenhagen Ø Denmark
3 shared publicationsA. M. Blackburn
Hitachi Cambridge Laboratory, Hitachi Europe Ltd, Cambridge CB3 0HE, UK
2 shared publications
Latest Publications
- 27 April 2009
- Published by American Physical Society (APS) in Physical Review B
- Vol. 79 (15) , 155441
Critical and excess current through an open quantum dot: Temperature and magnetic-field dependence
We present measurements of temperature and magnetic-field dependence of the critical current and excess current in a carbon nanotube Josephson quantum dot junction. The junction is fabricated in a controlled environment which allows for extraction of the full critical current. The measurements are performed in the open quantum dot regime and fitted to theory with good qualitative agreement. We also show how to extract level spacing, level broadening, and charging energy of an open quantum dot from a bias spectroscopy plot.
- 27 April 2009
- Published by American Physical Society (APS) in Physical Review B
- Vol. 79 (15) , 155441
Critical and excess current through an open quantum dot: Temperature and magnetic-field dependence
We present measurements of temperature and magnetic-field dependence of the critical current and excess current in a carbon nanotube Josephson quantum dot junction. The junction is fabricated in a controlled environment which allows for extraction of the full critical current. The measurements are performed in the open quantum dot regime and fitted to theory with good qualitative agreement. We also show how to extract level spacing, level broadening, and charging energy of an open quantum dot from a bias spectroscopy plot.
- Open Access
Critical and excess current through an open quantum dot: Temperature and magnetic field dependence
We present measurements of temperature and magnetic field dependence of the critical current and excess current in a carbon nanotube Josephson quantum dot junction. The junction is fabricated in a controlled environment which allows for extraction of the full critical current. The measurements are performed in the open quantum dot regime, and fitted to theory with good qualitative agreement. We also show how to extract level spacing, level broadening, and charging energy of an open quantum dot from a bias spectroscopy plot.
Open AccessCritical and excess current through an open quantum dot: Temperature and magnetic field dependence
We present measurements of temperature and magnetic field dependence of the critical current and excess current in a carbon nanotube Josephson quantum dot junction. The junction is fabricated in a controlled environment which allows for extraction of the full critical current. The measurements are performed in the open quantum dot regime, and fitted to theory with good qualitative agreement. We also show how to extract level spacing, level broadening, and charging energy of an open quantum dot from a bias spectroscopy plot.
- 15 June 2008
- Published by Springer Nature in Nature Physics
- Vol. 4 (7) , 536-539
Singlet–triplet physics and shell filling in carbon nanotube double quantum dots
- 15 June 2008
- Published by Springer Nature in Nature Physics
- Vol. 4 (7) , 536-539
Singlet–triplet physics and shell filling in carbon nanotube double quantum dots
- Open Access
Singlet-Triplet Physics and Shell Filling in Carbon Nanotube Double Quantum Dots
An artifcial two-atomic molecule, also called a double quantum dot (DQD), is an ideal system for exploring few electron physics. Spin-entanglement between just two electrons can be explored in such systems where singlet and triplet states are accessible. These two spin-states can be regarded as the two states in a quantum two-state system, a so-called singlet-triplet qubit. A very attractive material for realizing spin based qubits is the carbon nanotube (CNT), because it is expected to have a very long spin coherence time. Here we show the existence of a gate-tunable singlet-triplet qubit in a CNT DQD. We show that the CNT DQD has clear shell structures of both four and eight electrons, with the singlet-triplet qubit present in the four-electron shells. We furthermore observe inelastic cotunneling via the singlet and triplet states, which we use to probe the splitting between singlet and triplet, in good agreement with theory.
Open AccessSinglet-Triplet Physics and Shell Filling in Carbon Nanotube Double Quantum Dots
An artifcial two-atomic molecule, also called a double quantum dot (DQD), is an ideal system for exploring few electron physics. Spin-entanglement between just two electrons can be explored in such systems where singlet and triplet states are accessible. These two spin-states can be regarded as the two states in a quantum two-state system, a so-called singlet-triplet qubit. A very attractive material for realizing spin based qubits is the carbon nanotube (CNT), because it is expected to have a very long spin coherence time. Here we show the existence of a gate-tunable singlet-triplet qubit in a CNT DQD. We show that the CNT DQD has clear shell structures of both four and eight electrons, with the singlet-triplet qubit present in the four-electron shells. We furthermore observe inelastic cotunneling via the singlet and triplet states, which we use to probe the splitting between singlet and triplet, in good agreement with theory.
- 1 October 2007
- Published by Elsevier in Physica E: Low-dimensional Systems and Nanostructures
- Vol. 40 (1) , 92-98
Fabry–Perot interference, Kondo effect and Coulomb blockade in carbon nanotubes
- 1 October 2007
- Published by Elsevier in Physica E: Low-dimensional Systems and Nanostructures
- Vol. 40 (1) , 92-98
Fabry–Perot interference, Kondo effect and Coulomb blockade in carbon nanotubes
- Open Access
Critical Current 0-$π$ Transition in Designed Josephson Quantum Dot Junctions
We report on quantum dot based Josephson junctions designed specifically for measuring the supercurrent. From high-accuracy fitting of the current-voltage characteristics we determine the full magnitude of the supercurrent (critical current). Strong gate modulation of the critical current is observed through several consecutive Coulomb blockade oscillations. The critical current crosses zero close to, but not at, resonance due to the so-called 0-$\pi$ transition in agreement with a simple theoretical model.
Open AccessCritical Current 0-$π$ Transition in Designed Josephson Quantum Dot Junctions
We report on quantum dot based Josephson junctions designed specifically for measuring the supercurrent. From high-accuracy fitting of the current-voltage characteristics we determine the full magnitude of the supercurrent (critical current). Strong gate modulation of the critical current is observed through several consecutive Coulomb blockade oscillations. The critical current crosses zero close to, but not at, resonance due to the so-called 0-$\pi$ transition in agreement with a simple theoretical model.
- 18 July 2007
- Published by American Chemical Society (ACS) in Nano Letters
- Vol. 7 (8) , 2441-2445
Critical Current 0−π Transition in Designed Josephson Quantum Dot Junctions
We report on quantum dot based Josephson junctions designed specifically for measuring the supercurrent. From high-accuracy fitting of the current−voltage characteristics, we determine the full magnitude of the supercurrent (critical current). Strong gate modulation of the critical current is observed through several consecutive Coulomb blockade oscillations. The critical current crosses zero close to, but not at, resonance due to the so-called 0−π transition in agreement with a simple theoretical model.
- 18 July 2007
- Published by American Chemical Society (ACS) in Nano Letters
- Vol. 7 (8) , 2441-2445
Critical Current 0−π Transition in Designed Josephson Quantum Dot Junctions
We report on quantum dot based Josephson junctions designed specifically for measuring the supercurrent. From high-accuracy fitting of the current−voltage characteristics, we determine the full magnitude of the supercurrent (critical current). Strong gate modulation of the critical current is observed through several consecutive Coulomb blockade oscillations. The critical current crosses zero close to, but not at, resonance due to the so-called 0−π transition in agreement with a simple theoretical model.
- Open Access
Single wall carbon nanotube double quantum dot
We report on two top-gate defined, coupled quantum dots in a semiconducting single wall carbon nanotube, constituting a tunable double quantum dot system. The single wall carbon nanotubes are contacted by titanium electrodes, and gated by three narrow top-gate electrodes as well as a back-gate. We show that a bias spectroscopy plot on just one of the two quantum dots can be used to extract the addition energy of both quantum dots. Furthermore, honeycomb charge stability diagrams are analyzed by an electrostatic capacitor model that includes cross capacitances, and we extract the coupling energy of the double quantum dot.
Open AccessSingle wall carbon nanotube double quantum dot
We report on two top-gate defined, coupled quantum dots in a semiconducting single wall carbon nanotube, constituting a tunable double quantum dot system. The single wall carbon nanotubes are contacted by titanium electrodes, and gated by three narrow top-gate electrodes as well as a back-gate. We show that a bias spectroscopy plot on just one of the two quantum dots can be used to extract the addition energy of both quantum dots. Furthermore, honeycomb charge stability diagrams are analyzed by an electrostatic capacitor model that includes cross capacitances, and we extract the coupling energy of the double quantum dot.
- 25 May 2006
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 96 (20) , 207003
Electron Transport in Single-Wall Carbon Nanotube Weak Links in the Fabry-Perot Regime
We fabricated reproducible high transparency superconducting contacts consisting of superconducting trilayers to gated single-wall carbon nanotubes. The reported semiconducting single-wall carbon nanotubes have normal state differential conductance up to and exhibit clear Fabry-Perot interference patterns in the bias spectroscopy plot. We observed subharmonic gap structure in the differential conductance and a distinct peak in the conductance at zero bias, which is interpreted as a manifestation of the supercurrent. The gate dependence of this supercurrent as well as the excess current are examined and compared to the coherent theory of superconducting quantum point contacts with good agreement.- 25 May 2006
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 96 (20) , 207003
Electron Transport in Single-Wall Carbon Nanotube Weak Links in the Fabry-Perot Regime
We fabricated reproducible high transparency superconducting contacts consisting of superconducting trilayers to gated single-wall carbon nanotubes. The reported semiconducting single-wall carbon nanotubes have normal state differential conductance up to and exhibit clear Fabry-Perot interference patterns in the bias spectroscopy plot. We observed subharmonic gap structure in the differential conductance and a distinct peak in the conductance at zero bias, which is interpreted as a manifestation of the supercurrent. The gate dependence of this supercurrent as well as the excess current are examined and compared to the coherent theory of superconducting quantum point contacts with good agreement.