Cited by 38Atomic and Molecular PhysicsQuantum Information and CryptographyQuantum Mechanics and Applications

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Phase-sensitive measurement of trapped particle motions

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Stahl, S, Alonso, J, Djekic, S, Kluge, H-J, Quint, W, Verdu, J, Vogel, M, Werth, G·2005·Journal of Physics B: Atomic, Molecular and Optical Physics

Abstract

We have developed and applied a novel method for the precise determination of small frequency differences of particle motions inside a Penning trap. In the present case, the frequency differences on the order of 100 mHz at motional frequencies on the order of 1 MHz are used to determine the spin state of an electron bound in a hydrogen-like ion. This novel technique measures the integrated phase difference of the particles' motions relative to an excitation with a well-defined phase. Thereby, the Fourier-limit for frequency measurements based on Fourier-analyses of detection signals can be overcome.

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Crossref · 10.1088/0953-4075/38/3/013

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  • For the measurement of the (anti)proton's magnetic moment, a toroidal hybrid trap has been manufactured with B2 approximately 400 mTmm^-2, resulting in a frequency shift of about 200 mHz for a single (anti)proton at approximately 700 kHz axial frequency, thus enabling non-destructive detection of the (anti)proton's spin state.

    “For our measurement of the (anti)proton's magnetic moment, we have manufactured a toroidal hybrid trap with B 2 ∼ 400 mTmm -2 , resulting in a frequency shift of about 200 mHz for a single (anti)proton at ∼ 700 kHz axial frequency, thus enabling the non-destructive detection of the (anti)proton's spin state [28].”

    From Calculation of electrostatic fields using quasi-Green's functions: application to the hybrid Penning trap (2008) · cites this paper as [28]

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  • σ(∆φ) represents the minimum axial phase-difference required to distinguish between the particle at n_p=0 (ω_z=ω_0z) from the state n_p=1 (ω_z=ω_0z+∆ω_z).

    “In Equation ( 20) σ(∆φ) represents the minimum axial phase-difference required to distinguish between the particle at n p = 0 (i.e., with ω z = ω 0 z ) from the state n p = 1 (i.e., with ω z = ω 0 z + ∆ω z ) [26].”

    From Single Microwave Photon Detection with a Trapped Electron (2016) · cites this paper as [26]

    Section 3 defines σ(φ) as the uncertainty in determining a phase difference and demonstrates that a phase difference can distinguish two axial frequencies. It does not define σ(φ) as the minimum difference needed to distinguish states n_p=0 and n_p=1, or discuss those states; its example concerns simulated electron spin states. Page numbers are unavailable in our copy. (LLM, conf=0.84)

    Experimental — accuracy not yet measured
  • In the early experiments of [26], quantum jumps of 100 mHz were determined in 800 ms, with σ(∆φ)=45°.

    “In the early experiments of [26] quantum jumps of 100 mHz were determined in 800 ms, with σ(∆φ) = 45 • .”

    From Single Microwave Photon Detection with a Trapped Electron (2016) · cites this paper as [26]

    The Conclusion reports detecting a frequency difference around 100 mHz in about 0.8 s per data point. But Section 3 says the spin-state changes were simulated, not observed quantum jumps, and identifies approximately 45° as the separation between the measured phases, not the uncertainty σ(∆φ). (LLM, conf=0.90)

    Experimental — accuracy not yet measured
  • The enhanced curvature of the magnetic bottle from the toroidal ferromagnetic ring makes the resolution of the phase-sensitive Stern-Gerlach quantum jump spectrometer big enough for efficient determination of the spin state of a single (anti)proton.

    “therefore making the resolution of the phase-sensitive Stern-Gerlach quantum jump spectrometer [28] big enough for the efficient determination of the spin state of a single (anti)proton.”
  • Frequency variations ∆ωz can be determined substantially faster than a full 5 s measurement by recording the phase evolution of the axial motion without waiting for a full 2π oscillation.

    “However, frequency variations ∆ω z can be determined substantially faster, by recording the phase evolution of the axial motion but without waiting for a full 2π oscillation [26].”

    From Single Microwave Photon Detection with a Trapped Electron (2016) · cites this paper as [26]

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References 11 · Cited by 38

Research works printed but not linked: 2

  1. Dehmelt H G, 1983, Bull. Am. Phys. Soc., 18, 727
  2. Vogel M, Nucl. Instrum. Methods

Metadata

Authors
Stahl, S., Alonso, J., Djekic, S., Kluge, H.-J., Quint, W., Verdu, J., Vogel, M., & Werth, G.
Affiliations
  • Johannes Gutenberg University Mainz (DE)
  • GSI Helmholtz Centre for Heavy Ion Research (DE)
Venue
Journal of Physics B: Atomic, Molecular and Optical Physics
Published
2005-01-25
Volume
38
Issue
3
Pages
297-304
ISSN
  • 0953-4075 (ISSN-L)
  • 1361-6455
OpenAlex
W2028061529
Cited by
38
References
11
Citations by year
2025: 2 · 2024: 2 · 2021: 1 · 2020: 1 · 2018: 2 · 2016: 1 · 2015: 1 · 2014: 3 · 2013: 2 · 2012: 1
FWCI
1.84
Type
journal article
Language
en
Open access
Locations
Journal of Physics B Atomic Molecular and Optical Physics (publishedVersion)
Funders
  • Deutsche Forschungsgemeinschaft (HPRI-CT-2001-50036)
  • Bundesministerium für Bildung und Forschung (HPRI-CT-2001-50036)
Topics
  • Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Atomic and Molecular Physics
  • Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum Information and Cryptography
  • Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum Mechanics and Applications
Keywords
phase-sensitive measurement, Penning trap, frequency difference measurement, electron spin states, hydrogen-like ions, phase difference, ion cyclotron resonance

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