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Showing papers by "George M. Seidel published in 2019"


Journal ArticleDOI
M. W. Ahmed1, M. W. Ahmed2, Ricardo Alarcon3, A. Aleksandrova4, S. Baeßler5, S. Baeßler6, L. Barrón-Palos7, L. M. Bartoszek, Douglas H Beck8, M. Behzadipour4, I. Berkutov, J. Bessuille9, M. Blatnik10, M. Broering4, Leah Broussard6, M. Busch2, R. Carr10, V. Cianciolo6, Steven Clayton11, M. D. Cooper11, Christopher Crawford4, Scott Currie11, C. Daurer, R. Dipert3, K. A. Dow9, Dipangkar Dutta12, Yu. Efremenko6, Yu. Efremenko13, C. B. Erickson8, B. W. Filippone10, Nadia Fomin13, Haiyan Gao2, Robert Golub14, C. R. Gould14, Geoffrey Greene13, Geoffrey Greene6, David G. Haase14, D. Hasell9, Ayman I. Hawari14, M. E. Hayden15, A. T. Holley16, R. J. Holt10, P. R. Huffman6, P. R. Huffman14, E. Ihloff9, S. K. Imam13, Takeyasu M. Ito11, M. Karcz17, J. Kelsey9, D. P. Kendellen2, Yongsun Kim9, E. Korobkina14, Wolfgang Korsch4, Steve K. Lamoreaux18, E. Leggett12, K. K. H. Leung14, A. Lipman14, C. Y. Liu17, J. Long17, S. W. T. MacDonald11, Mark Makela11, A. Matlashov11, James Maxwell9, James Maxwell19, Marcus H. Mendenhall10, Marcus H. Mendenhall20, H. O. Meyer17, Ross Milner9, P. E. Mueller6, Nima Nouri4, C. M. O'Shaughnessy11, C. Osthelder10, Jen-Chieh Peng8, Seppo Penttila6, N. S. Phan11, Brad Plaster4, John Ramsey6, John Ramsey11, T. M. Rao14, T. M. Rao8, R. P. Redwine9, A. Reid14, A. Reid17, A. Saftah4, George M. Seidel21, I.F. Silvera22, S. Slutsky10, E. Smith11, W. M. Snow17, W. E. Sondheim11, S. Sosothikul14, T. D. S. Stanislaus23, X. Sun10, C. Swank10, Z. Tang11, R. Tavakoli Dinani15, R. Tavakoli Dinani24, Evgeni Tsentalovich9, C. Vidal9, Wanchun Wei7, C. R. White14, S. E. Williamson8, Liang Yang8, W. Yao6, A. R. Young14 
TL;DR: In this paper, a new experiment, nEDM@SNS, is described that enables a major improvement in sensitivity compared to the existing limit in the search for a neutron Electric Dipole Moment (EDM), using superfluid 4He to produce a high density of ultra-cold Neutrons (UCN) which are contained in a suitably coated pair of measurement cells.
Abstract: A cryogenic apparatus is described that enables a new experiment, nEDM@SNS, with a major improvement in sensitivity compared to the existing limit in the search for a neutron Electric Dipole Moment (EDM). This apparatus uses superfluid ⁴He to produce a high density of Ultra-Cold Neutrons (UCN) which are contained in a suitably coated pair of measurement cells. The experiment, to be operated at the Spallation Neutron Source at Oak Ridge National Laboratory, uses polarized ³He from an Atomic Beam Source injected into the superfluid 4He and transported to the measurement cells where it serves as a co-magnetometer. The superfluid ⁴He is also used as an insulating medium allowing significantly higher electric fields, compared to previous experiments, to be maintained across the measurement cells. These features provide an ultimate statistical uncertainty for the EDM of 2−3× 10⁻²⁸ e-cm, with anticipated systematic uncertainties below this level.

32 citations


Journal ArticleDOI
TL;DR: In this paper, a new experiment, nEDM@SNS, is described that enables a major improvement in sensitivity compared to the existing limit in the search for a neutron Electric Dipole Moment (EDM).
Abstract: A cryogenic apparatus is described that enables a new experiment, nEDM@SNS, with a major improvement in sensitivity compared to the existing limit in the search for a neutron Electric Dipole Moment (EDM). It uses superfluid $^4$He to produce a high density of Ultra-Cold Neutrons (UCN) which are contained in a suitably coated pair of measurement cells. The experiment, to be operated at the Spallation Neutron Source at Oak Ridge National Laboratory, uses polarized $^3$He from an Atomic Beam Source injected into the superfluid $^4$He and transported to the measurement cells as a co-magnetometer. The superfluid $^4$He is also used as an insulating medium allowing significantly higher electric fields, compared to previous experiments, to be maintained across the measurement cells. These features provide an ultimate statistical uncertainty for the EDM of $2-3\times 10^{-28}$ e-cm, with anticipated systematic uncertainties below this level.

11 citations


Journal ArticleDOI
K. K. H. Leung1, K. K. H. Leung2, M. W. Ahmed3, M. W. Ahmed1, M. W. Ahmed4, Ricardo Alarcon5, A. Aleksandrova6, S. Baeßler7, S. Baeßler8, L. Barrón-Palos9, L. M. Bartoszek, Douglas H Beck10, M. Behzadipour6, J. Bessuille11, M. Blatnik12, M. Broering6, Leah Broussard8, Matthew Busch1, Matthew Busch4, R. Carr12, Pinghan Chu4, V. Cianciolo8, Steven Clayton13, M. D. Cooper13, Christopher Crawford6, Scott Currie13, C. Daurer10, R. Dipert5, K. A. Dow11, Dipangkar Dutta14, Yu. Efremenko8, Yu. Efremenko15, C. B. Erickson10, B. W. Filippone12, Nadia Fomin15, Haiyan Gao4, Robert Golub1, Robert Golub2, C. R. Gould1, C. R. Gould2, Geoffrey Greene8, Geoffrey Greene15, David G. Haase2, David G. Haase1, D. Hasell11, Ayman I. Hawari2, M. E. Hayden16, A. T. Holley, R. J. Holt12, P. R. Huffman1, P. R. Huffman8, P. R. Huffman2, E. Ihloff11, Takeyasu M. Ito13, J. Kelsey11, Y.J. Kim13, E. Korobkina1, E. Korobkina2, Wolfgang Korsch6, Steve K. Lamoreaux17, E. Leggett14, A. Lipman2, A. Lipman1, C.-Y. Liu18, J. Long18, S. W. T. MacDonald13, Mark Makela13, A. Matlashov13, James Maxwell11, M. McCrea6, Marcus H. Mendenhall12, H. O. Meyer18, Ross Milner11, P. E. Mueller8, Nima Nouri17, Nima Nouri6, C. M. O'Shaughnessy13, C. Osthelder12, Jen-Chieh Peng10, Seppo Penttila8, N. S. Phan13, Brad Plaster6, John Ramsey13, John Ramsey8, T. Rao10, R. P. Redwine11, A. Reid2, A. Reid1, A. Saftah6, George M. Seidel19, I.F. Silvera20, S. Slutsky12, E. Smith13, W. M. Snow18, W. E. Sondheim13, S. Sosothikul1, S. Sosothikul2, T. D. S. Stanislaus21, X. Sun12, C. Swank12, Z. Tang13, R. Tavakoli Dinani16, Evgeni Tsentalovich11, C. Vidal11, Wanchun Wei12, Wanchun Wei13, C. R. White1, C. R. White2, S. E. Williamson10, Liang Yang10, W. Yao8, A. R. Young2, A. R. Young1 
TL;DR: The nEDM experiment at the Spallation Neutron Source (nEDM@SNS) as discussed by the authors was the first to implement the scheme of Golub & Lamoreaux [Phys. Rep., 237, 1 (1994).
Abstract: Novel experimental techniques are required to make the next big leap in neutron electric dipole moment experimental sensitivity, both in terms of statistics and systematic error control. The nEDM experiment at the Spallation Neutron Source (nEDM@SNS) will implement the scheme of Golub & Lamoreaux [Phys. Rep., 237, 1 (1994)]. The unique properties of combining polarized ultracold neutrons, polarized 3 He, and superfluid 4 He will be exploited to provide a sensitivity to ∼ 10−28 e · cm. Our cryogenic apparatus will deploy two small (3 L) measurement cells with a high density of ultracold neutrons produced and spin analyzed in situ. The electric field strength, precession time, magnetic shielding, and detected UCN number will all be enhanced compared to previous room temperature Ramsey measurements. Our 3 He co-magnetometer offers unique control of systematic effects, in particular the Bloch-Siegert induced false EDM. Furthermore, there will be two distinct measurement modes: free precession and dressed spin. This will provide an important self-check of our results. Following five years of “critical component demonstration,” our collaboration transitioned to a “large scale integration” phase in 2018. An overview of our measurement techniques, experimental design, and brief updates are described in these proceedings.

6 citations


Journal ArticleDOI
TL;DR: The nEDM experiment at the Spallation Neutron Source (nEDM@SNS) as discussed by the authors was the first to implement the scheme of Golub & Lamoreaux [Phys. Rep., 237, 1 (1994)].
Abstract: Novel experimental techniques are required to make the next big leap in neutron electric dipole moment experimental sensitivity, both in terms of statistics and systematic error control. The nEDM experiment at the Spallation Neutron Source (nEDM@SNS) will implement the scheme of Golub & Lamoreaux [Phys. Rep., 237, 1 (1994)]. The unique properties of combining polarized ultracold neutrons, polarized $^3$He, and superfluid $^4$He will be exploited to provide a sensitivity to $\sim 10^{-28}\,e{\rm \,\cdot\, cm}$. Our cryogenic apparatus will deploy two small ($3\,{\rm L}$) measurement cells with a high density of ultracold neutrons produced and spin analyzed in situ. The electric field strength, precession time, magnetic shielding, and detected UCN number will all be enhanced compared to previous room temperature Ramsey measurements. Our $^3$He co-magnetometer offers unique control of systematic effects, in particular the Bloch-Siegert induced false EDM. Furthermore, there will be two distinct measurement modes: free precession and dressed spin. This will provide an important self-check of our results. Following five years of "critical component demonstration," our collaboration transitioned to a "large scale integration" phase in 2018. An overview of our measurement techniques, experimental design, and brief updates are described in these proceedings.

3 citations