2016
DOI: 10.1103/physreva.93.043615
|View full text |Cite
|
Sign up to set email alerts
|

Heisenberg-scaled magnetometer with dipolar spin-1 condensates

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
28
0

Year Published

2017
2017
2022
2022

Publication Types

Select...
7
2

Relationship

2
7

Authors

Journals

citations
Cited by 32 publications
(28 citation statements)
references
References 63 publications
0
28
0
Order By: Relevance
“…Despite SMD can generate the desired input state, it sensitively depends on the control of evolution time and these states are always not steady. In contrast, driving system through QPTs can deterministically generate the entangled states [37,39,40,[58][59][60]74]. Recently, entanglement generation by driving through QPTs has been realized in 87 Rb spinor condensate [59,60,62].…”
Section: B Lsv Test Via Driving Through Quantum Phase Transitionsmentioning
confidence: 99%
“…Despite SMD can generate the desired input state, it sensitively depends on the control of evolution time and these states are always not steady. In contrast, driving system through QPTs can deterministically generate the entangled states [37,39,40,[58][59][60]74]. Recently, entanglement generation by driving through QPTs has been realized in 87 Rb spinor condensate [59,60,62].…”
Section: B Lsv Test Via Driving Through Quantum Phase Transitionsmentioning
confidence: 99%
“…Up to now, studies of nonlinear atomic interferometer with spinor BECs have focused mainly on s -wave contact interaction 27 29 . According to the recent experimental and theoretical observation in 23 Na and 87 Rb atoms, the magnetic dipole-dipole interactions (MDDIs) are indeed not negligible for these spinor condensates 26 , 30 39 . For example, in 87 Rb atoms, the magnitude of the dipolar energy can be as large as 10% of the spin-exchange energy 35 , 36 .…”
Section: Introductionmentioning
confidence: 98%
“…This process does not require accurate control of qubits. Moreover, this process is protected by symmetry, i.e., nonadiabatic transitions from even-parity energy eigenstates to odd-parity energy eigenstates do not take place because of parity conservation due to spin-flip symmetry [36][37][38][39]. This suppression of nonadiabatic transitions protects the macroscopic entanglement from spontaneous symmetry breaking.…”
Section: Introductionmentioning
confidence: 99%