J. R. Petta

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Name: Petta, Jason
Organization: Princeton University , USA
Department: Department of Physics
Title: (PhD)
Co-reporter:Jason R. Petta
ACS Nano March 28, 2017 Volume 11(Issue 3) pp:2382-2382
Publication Date(Web):March 10, 2017
DOI:10.1021/acsnano.7b00850
Scanning tunneling microscopes (STMs) are conventionally used to probe surfaces with atomic resolution. Recent advances in STM include tunneling from spin-polarized and superconducting tips, time-domain spectroscopy, and the fabrication of atomically precise Si nanoelectronics. In this issue of ACS Nano, Tettamanzi et al. probe a single-atom transistor in silicon, fabricated using the precision of a STM, at microwave frequencies. While previous studies have probed such devices in the MHz regime, Tettamanzi et al. probe a STM-fabricated device at GHz frequencies, which enables excited-state spectroscopy and measurements of the excited-state lifetime. The success of this experiment will enable future work on quantum control, where the wave function must be controlled on a time scale that is much shorter than the decoherence time. We review two major approaches that are being pursued to develop spin-based quantum computers and highlight some recent progress in the atom-by-atom fabrication of donor-based devices in silicon. Recent advances in STM lithography may enable practical bottom-up construction of large-scale quantum devices.Keywords: Kane quantum computer; phosphorus; quantum device; silicon; spectroscopy;
Co-reporter:P. W. Deelman;J. V. Cady;X. Mi;D. M. Zajac
Science 2017 Volume 355(Issue 6321) pp:
Publication Date(Web):
DOI:10.1126/science.aal2469

Inducing strong coupling

Quantum dots, or artificial atoms, are being pursued as prospective building blocks for quantum information processing architectures. Communication with other, distant quantum dots requires strong coupling between photons and the electronic states of the dots. Mi et al. used double quantum dots defined in silicon and embedded in a superconducting cavity to achieve such coupling. This demonstration in an industry-relevant material bodes well for the large-scale development of semiconductor-based quantum processors.

Science, this issue p. 156

Co-reporter:J. Stehlik;Y.-Y. Liu;C. Eichler;J. M. Taylor;M. J. Gullans
Science 2015 Volume 347(Issue 6219) pp:285-287
Publication Date(Web):16 Jan 2015
DOI:10.1126/science.aaa2501

Tunnel through and emit coherently

The generation of coherent light (lasers and masers) forms the basis of a large optics industry. Liu et al. demonstrate a type of laser that is driven by the tunneling of single electrons in semiconductor double-quantum dots. Distinct from other existing semiconductor lasers, the emission mechanism is driven by tunneling of single charges between discrete energy levels that are electrically tunable. The ability to tune the levels by single-electron charging would allow their laser (or maser) to be turned on and off rapidly.

Science, this issue p. 285

Co-reporter:L. D. Alegria, M. D. Schroer, A. Chatterjee, G. R. Poirier, M. Pretko, S. K. Patel, and J. R. Petta
Nano Letters 2012 Volume 12(Issue 9) pp:4711-4714
Publication Date(Web):July 25, 2012
DOI:10.1021/nl302108r
We characterize nanostructures of Bi2Se3 that are grown via metal–organic chemical vapor deposition using the precursors diethyl selenium and trimethyl bismuth. By adjusting growth parameters, we obtain either single-crystalline ribbons up to 10 μm long or thin micrometer-sized platelets. Four-terminal resistance measurements yield a sample resistivity of 4 mΩ·cm. We observe weak antilocalization and extract a phase coherence length lϕ = 178 nm and spin–orbit length lso = 93 nm at T = 0.29 K. Our results are consistent with previous measurements on exfoliated samples and samples grown via physical vapor deposition.
Co-reporter:M. D. Schroer and J. R. Petta
Nano Letters 2010 Volume 10(Issue 5) pp:1618-1622
Publication Date(Web):April 12, 2010
DOI:10.1021/nl904053j
The electronic properties and nanostructure of InAs nanowires are correlated by creating multiple field effect transistors (FETs) on nanowires grown to have low and high defect density segments. 4.2 K carrier mobilities are ∼4× larger in the nominally defect free segments of the wire. We also find that dark field optical intensity is correlated with the mobility, suggesting a simple route for selecting wires with a low defect density. At low temperatures, FETs fabricated on high defect density segments of InAs nanowires showed transport properties consistent with single electron charging, even on devices with low resistance ohmic contacts. The charging energies obtained suggest quantum dot formation at defects in the wires. These results reinforce the importance of controlling the defect density in order to produce high quality electrical and optical devices using InAs nanowires.
Co-reporter:A. C. Gossard;H. Lu
Science 2010 Volume 327(Issue 5966) pp:669-672
Publication Date(Web):05 Feb 2010
DOI:10.1126/science.1183628
Co-reporter:J.R. Petta, A.C. Johnson, J.M. Taylor, E.A. Laird, A. Yacoby, M.D. Lukin, C.M. Marcus, M.P. Hanson, A.C. Gossard
Physica E: Low-dimensional Systems and Nanostructures 2006 Volume 35(Issue 2) pp:251-256
Publication Date(Web):December 2006
DOI:10.1016/j.physe.2006.08.020
We use gate voltage control of the exchange interaction to prepare, manipulate, and measure two-electron spin states in a GaAs double quantum dot. By placing two electrons in a single dot at low temperatures we prepare the system in a spin singlet state. The spin singlet is spatially separated by transferring an electron to an adjacent dot. The spatially separated spin singlet state dephases in ∼10ns due to the contact hyperfine interaction with the GaAs host nuclei. To combat the hyperfine dephasing, we develop quantum control techniques based on fast electrical control of the exchange interaction. We demonstrate coherent spin-state rotations in a singlet–triplet qubit and harness the coherent rotations to implement a singlet–triplet spin echo refocusing pulse sequence. The singlet–triplet spin echo extends the spin coherence time to 1.2μs.
2-METHYL-2-PROPANYL {[1-(HYDROXYMETHYL)CYCLOPROPYL]METHYL}CARBAMATE
Bismuthine, trimethyl-(6CI,7CI,8CI,9CI)