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Featured researches published by B. Spaun.


Science | 2014

Order of Magnitude Smaller Limit on the Electric Dipole Moment of the Electron

Jacob Baron; Wesley C. Campbell; David DeMille; John M. Doyle; G. Gabrielse; Y. V. Gurevich; Paul Hess; Nicholas Hutzler; Emil Kirilov; Ivan Kozyryev; Brendon O'Leary; C. D. Panda; Maxwell Parsons; Elizabeth Petrik; B. Spaun; A. C. Vutha; Adam West

Stubbornly Spherical The shape of the electrons charge distribution reflects the degree to which switching the direction of time impacts the basic ingredients of the universe. The Standard Model (SM) of particle physics predicts a very slight asphericity of the charge distribution, whereas SM extensions such as supersymmetry posit bigger and potentially measurable, but still tiny, deviations from a perfect sphere. Polar molecules have been identified as ideal settings for measuring this asymmetry, which should be reflected in a finite electric dipole moment (EDM) because of the extremely large effective electric fields that act on an electron inside such molecules. Using electron spin precession in the molecule ThO, Baron et al. (p. 269, published online 19 December; see the cover; see the Perspective by Brown) measured the EDM of the electron as consistent with zero. This excludes some of the extensions to the SM and sets a bound to the search for a nonzero EDM in other facilities, such as the Large Hadron Collider. Spin precession measurements in the polar molecule thorium monoxide indicate a nearly spherical charge distribution of an electron. [Also see Perspective by Brown] The Standard Model of particle physics is known to be incomplete. Extensions to the Standard Model, such as weak-scale supersymmetry, posit the existence of new particles and interactions that are asymmetric under time reversal (T) and nearly always predict a small yet potentially measurable electron electric dipole moment (EDM), de, in the range of 10−27 to 10−30 e·cm. The EDM is an asymmetric charge distribution along the electron spin (S→) that is also asymmetric under T. Using the polar molecule thorium monoxide, we measured de = (–2.1 ± 3.7stat ± 2.5syst) × 10−29 e·cm. This corresponds to an upper limit of | de | < 8.7 × 10−29 e·cm with 90% confidence, an order of magnitude improvement in sensitivity relative to the previous best limit. Our result constrains T-violating physics at the TeV energy scale.


Journal of Physics B | 2010

Search for the electric dipole moment of the electron with thorium monoxide

A. C. Vutha; Wesley C. Campbell; Y. V. Gurevich; Nicholas Hutzler; Maxwell Parsons; David Patterson; Elizabeth Petrik; B. Spaun; John M. Doyle; G. Gabrielse; David DeMille

The electric dipole moment of the electron (eEDM) is a signature of CP-violating physics beyond the standard model. We describe an ongoing experiment to measure or set improved limits to the eEDM, using a cold beam of thorium monoxide (ThO) molecules. The metastable H 3 � 1 state in ThO has important advantages for such an experiment. We argue that the statistical uncertainty of an eEDM measurement could be improved by as much as three orders of magnitude compared to the current experimental limit, in a first-generation apparatus using a cold ThO beam. We describe our measurements of the H state lifetime and the production of ThO molecules in a beam, which provide crucial data for the eEDM sensitivity estimate. ThO also has ideal properties for the rejection of a number of known systematic errors; these properties and their implications are described. (Some figures in this article are in colour only in the electronic version)


Physical Chemistry Chemical Physics | 2011

A cryogenic beam of refractory, chemically reactive molecules with expansion cooling

Nicholas Hutzler; Maxwell Parsons; Y. V. Gurevich; Paul Hess; Elizabeth Petrik; B. Spaun; A. C. Vutha; David DeMille; G. Gabrielse; John M. Doyle

Cryogenically cooled buffer gas beam sources of the molecule thorium monoxide (ThO) are optimized and characterized. Both helium and neon buffer gas sources are shown to produce ThO beams with high flux, low divergence, low forward velocity, and cold internal temperature for a variety of stagnation densities and nozzle diameters. The beam operates with a buffer gas stagnation density of ∼10(15)-10(16) cm(-3) (Reynolds number ∼1-100), resulting in expansion cooling of the internal temperature of the ThO to as low as 2 K. For the neon (helium) based source, this represents cooling by a factor of about 10 (2) from the initial nozzle temperature of about 20 K (4 K). These sources deliver ∼10(11) ThO molecules in a single quantum state within a 1-3 ms long pulse at 10 Hz repetition rate. Under conditions optimized for a future precision spectroscopy application [A. C. Vutha et al., J. Phys. B: At., Mol. Opt. Phys., 2010, 43, 074007], the neon-based beam has the following characteristics: forward velocity of 170 m s(-1), internal temperature of 3.4 K, and brightness of 3 × 10(11) ground state molecules per steradian per pulse. Compared to typical supersonic sources, the relatively low stagnation density of this source and the fact that the cooling mechanism relies only on collisions with an inert buffer gas make it widely applicable to many atomic and molecular species, including those which are chemically reactive, such as ThO.


New Journal of Physics | 2017

Methods, Analysis, and the Treatment of Systematic Errors for the Electron Electric Dipole Moment Search in Thorium Monoxide

Jacob Baron; Wesley C. Campbell; David DeMille; John M. Doyle; G. Gabrielse; Y. V. Gurevich; P W Hess; Nicholas Hutzler; E. Kirilov; Ivan Kozyryev; B R O’Leary; C. D. Panda; Maxwell Parsons; B. Spaun; Amar C. Vutha; Adam West; Elizabeth West

We recently set a new limit on the electric dipole moment of the electron (eEDM) (J Baron et al and ACME collaboration 2014 Science 343 269–272), which represented an order-of-magnitude improvement on the previous limit and placed more stringent constraints on many charge-parity-violating extensions to the standard model. In this paper we discuss the measurement in detail. The experimental method and associated apparatus are described, together with the techniques used to isolate the eEDM signal. In particular, we detail the way experimental switches were used to suppress effects that can mimic the signal of interest. The methods used to search for systematic errors, and models explaining observed systematic errors, are also described. We briefly discuss possible improvements to the experiment.


Physical Review A | 2011

Magnetic and Electric Dipole Moments of the \(H\ ^3\Delta_1\) State in ThO

A. C. Vutha; B. Spaun; Y. V. Gurevich; Nicholas Hutzler; Emil Kirilov; John M. Doyle; G. Gabrielse; David DeMille

The metastable H^3 Δ_1 state in the thorium monoxide (ThO) molecule is highly sensitive to the presence of a CP -violating permanent electric dipole moment of the electron (eEDM) [E. R. Meyer and J. L. Bohn, Phys. Rev. A 78, 010502 (2008)]. The magnetic dipole moment μ_H and the molecule-fixed electric dipole moment D_H of this state are measured in preparation for a search for the eEDM. The small magnetic moment μH=8.5(5)×10^(−3)μ_B displays the predicted cancellation of spin and orbital contributions in a ^3Δ_1 paramagnetic molecular state, providing a significant advantage for the suppression of magnetic field noise and related systematic effects in the eEDM search. In addition, the induced electric dipole moment is shown to be fully saturated in very modest electric fields (<10 V/cm). This feature is favorable for the suppression of many other potential systematic errors in the ThO eEDM search experiment.


Physical Review A | 2013

Shot-noise-limited spin measurements in a pulsed molecular beam

E. Kirilov; Wesley C. Campbell; John M. Doyle; G. Gabrielse; Y. V. Gurevich; Paul Hess; Nicholas Hutzler; Brendon O'Leary; Elizabeth Petrik; B. Spaun; A. C. Vutha; David DeMille

Heavy diatomic molecules have been identified as good candidates for use in electron electric dipole moment (eEDM) searches. Suitable molecular species can be produced in pulsed beams, but with a total flux and/or temporal evolution that varies significantly from pulse to pulse. These variations can degrade the experimental sensitivity to changes in the spin precession phase of an electrically polarized state, which is the observable of interest for an eEDM measurement. We present two methods for measurement of the phase that provide immunity to beam temporal variations, and make it possible to reach shot-noise-limited sensitivity. Each method employs rapid projection of the spin state onto both components of an orthonormal basis. We demonstrate both methods using the eEDM-sensitive H3Δ1 state of thorium monoxide, and use one of them to measure the magnetic moment of this state with increased accuracy relative to previous determinations.


Physical Review A | 2014

Zeeman interaction in ThO H 3&#120607;1 for the electron electric-dipole-moment search

A. N. Petrov; L. V. Skripnikov; A. V. Titov; Nicholas Hutzler; Paul Hess; Brendon O'Leary; B. Spaun; David DeMille; G. Gabrielse; John M. Doyle

The current limit on the electrons electric dipole moment,


Physical Review A | 2014

Zeeman interaction in ThO

A. N. Petrov; L. V. Skripnikov; A. V. Titov; Nicholas Hutzler; Paul Hess; Brendon O'Leary; B. Spaun; David DeMille; G. Gabrielse; John M. Doyle

|d_\mathrm{e}|<8.7\times 10^{-29} e {\cdotp} {\rm cm}


Physical Review A | 2014

H^3\Delta_1

A. N. Petrov; L. V. Skripnikov; A. V. Titov; Nicholas Hutzler; Paul Hess; Brendon O'Leary; B. Spaun; David DeMille; G. Gabrielse; John M. Doyle

(90% confidence), was set using the molecule thorium monoxide (ThO) in the


Physical Review A | 2011

for the electron EDM search

A. C. Vutha; B. Spaun; Y. V. Gurevich; Nicholas Hutzler; Emil Kirilov; John M. Doyle; G. Gabrielse; David DeMille

J=1

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