Abstract:33 pages, 18 figuresThe Surrounding Field Compensation (SFC) system described in this work is installed around the four-layer Mu-metal magnetic shield of the neutron electric dipole moment spectrometer located at the Paul Scherrer Institute. The SFC system reduces the DC component of the external magnetic field by a factor of about 20. Within a control volume of approximately 2.5m x 2.5m x 3m disturbances of the magnetic field are attenuated by factors of 5 to 50 at a bandwidth from $10^{-3}$ Hz up to 0.5 Hz, … Show more
“…1. The pulse duration (τ ) determines the fractional population of atoms in the two photon (P = sin 2 [Ω p τ /2]) and clock (1 − P ) interferometers. The state after the preparation pulse is given by…”
Section: Interferometric Signal From a Dual Interferometermentioning
confidence: 99%
“…Magnetic fluctuations are a common source of decoherence in quantum information applications [13,14]. The choice of the proper transition and the use of active feedback or magnetic shielding helps minimizing these noise contributions [2,15,16]. Atomic clocks, for example, use the so called clock transition that connects levels with no linear Zeeman effect.…”
Section: Introductionmentioning
confidence: 99%
“…Atoms can be configured as magnetometers that achieve sensitivity slightly better than other available technologies [1]. These sensors have been used to achieve magnetic noise free regions [2][3][4][5], to study biomagnetism [6,7], to generate squeezing in spin systems [8][9][10] or to look for physics beyond the Standard Model [11,12].…”
Atomic interferometers are often affected by magnetic field fluctuations. Using the clock transition at zero magnetic field minimizes the effect of these fluctuations. There is another transition in rubidium that minimizes the magnetic sensitivity at 3.2 Gauss. We combine the previous two transitions to obtain minimum magnetic sensitivity at a tunable magnetic field between 2.2 and 3.2 Gauss. The two interferometers evolve independently from each other and we control the magnetic sensitivity by changing the population in both transitions with a microwave pulse.
“…1. The pulse duration (τ ) determines the fractional population of atoms in the two photon (P = sin 2 [ Ω p τ /2]) and clock (1 − P ) interferometers. The state after the preparation pulse is given by…”
Section: Interferometric Signal From a Dual Interferometermentioning
confidence: 99%
“…Magnetic fluctuations are a common source of decoherence in quantum information applications [13,14]. The choice of the proper transition and the use of active feedback or magnetic shielding helps minimizing these noise contributions [2,15,16]. Atomic clocks, for example, use the so called clock transition that connects levels with no linear Zeeman effect.…”
Section: Introductionmentioning
confidence: 99%
“…Atoms can be configured as magnetometers that achieve sensitivity slightly better than other available technologies [1]. These sensors have been used to achieve magnetic noise free regions [2][3][4][5], to study biomagnetism [6,7], to generate squeezing in spin systems [8][9][10] or to look for physics beyond the Standard Model [11,12].…”
Atomic interferometers are often affected by magnetic field fluctuations. Using the clock transition at zero magnetic field minimizes the effect of these fluctuations. There is another transition in rubidium that minimizes the magnetic sensitivity at 3.2 Gauss. We combine the previous two transitions to obtain minimum magnetic sensitivity at a tunable magnetic field between 2.2 and 3.2 Gauss. The two interferometers evolve independently from each other and we control the magnetic sensitivity by changing the population in both transitions with a microwave pulse.
“…The first one is used in the neutron Electric Dipole Moment spectrometer installed at the Paul Scherrer Institute, Villigen, Switzerland 1,8 ). The system consists of three pairs of rectangular coils as shown in blue in Figure 6.…”
Section: Spherical and Rectangular Coil Systems For A Comparisonmentioning
confidence: 99%
“…Active field compensation utilizing threedimensional Helmholtz-like coil systems were applied e.g. in MiniCLEAN, 6 LIPSION 7 and nEDM 8 experiments.…”
An analytic solution to the magnetostatic inverse problem in the framework of vector spherical harmonic basis functions is presented. This formalism is used for the design of a spherical magnetic field compensation system and its performance is compared with an already existing rectangular coil system. The proposed set of spherical coils with 15 degrees of freedom achieves a shielding factor of 1000 or better in a large part of the volume enclosed by the coils for a dipolar type external perturbation.
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