J. Millo
Centre national de la recherche scientifique
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Featured researches published by J. Millo.
Physical Review Letters | 2011
Philip G. Westergaard; J. Lodewyck; Luca Lorini; Arnaud Lecallier; Eric A. Burt; M. Zawada; J. Millo; P. Lemonde
We present a comprehensive study of the frequency shifts associated with the lattice potential in a Sr lattice clock by comparing two such clocks with a frequency stability reaching 5×10(-17) after a 1 h integration time. We put the first experimental upper bound on the multipolar M1 and E2 interactions, significantly smaller than the recently predicted theoretical upper limit, and give a 30-fold improved upper limit on the effect of hyperpolarizability. Finally, we report on the first observation of the vector and tensor shifts in a Sr lattice clock. Combining these measurements, we show that all known lattice related perturbations will not affect the clock accuracy down to the 10(-17) level, even for lattices as deep as 150 recoil energies.
Physical Review A | 2009
J. Millo; Daniel Varela Magalhães; C. Mandache; Y. Le Coq; E. M. L. English; Philip G. Westergaard; Jérôme Lodewyck; S. Bize; P. Lemonde; G. Santarelli
We present two ultrastable lasers based on two vibration insensitive cavity designs, one with vertical optical axis geometry, the other horizontal. Ultrastable cavities are constructed with fused silica mirror substrates, shown to decrease the thermal noise limit, in order to improve the frequency stability over previous designs. Vibration sensitivity components measured are equal to or better than
Journal of The Optical Society of America B-optical Physics | 2008
Haifeng Jiang; Fabien Kéfélian; Scott Crane; O. Lopez; M. Lours; J. Millo; D. Holleville; P. Lemonde; Christian Chardonnet; A. Amy-Klein; Georgio Santarelli
1.5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}/\text{m}\text{ }{\text{s}}^{\ensuremath{-}2}
Applied Physics Letters | 2009
J. Millo; M. Abgrall; M. Lours; E. M. L. English; H. Jiang; J. Guéna; A. Clairon; Michael E. Tobar; S. Bize; Y. Le Coq; G. Santarelli
for each spatial direction, which shows significant improvement over previous studies. We have tested the very low dependence on the position of the cavity support points, in order to establish that our designs eliminate the need for fine tuning to achieve extremely low vibration sensitivity. Relative frequency measurements show that at least one of the stabilized lasers has a stability better than
Optics Letters | 2009
J. Millo; Rodolphe Boudot; M. Lours; P.Y. Bourgeois; Andre Luiten; Y. Le Coq; Y. Kersale; G. Santarelli
5.6\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}16}
Applied Optics | 2015
Khaldoun Saleh; J. Millo; Alexandre Didier; Y. Kersale; Clément Lacroûte
at 1 s, which is the best result obtained for this length of cavity.
Optics Letters | 2012
John J. McFerran; Daniel Varela Magalhães; C. Mandache; J. Millo; W. Zhang; Y. Le Coq; G. Santarelli; S. Bize
We transferred the frequency of an ultra-stable laser over 86 km of urban fiber. The link is composed of two cascaded 43-km fibers connecting two laboratories, LNE-SYRTE and LPL in Paris area. In an effort to realistically demonstrate a link of 172 km without using spooled fiber extensions, we implemented a recirculation loop to double the length of the urban fiber link. The link is fed with a 1542-nm cavity stabilized fiber laser having a sub-Hz linewidth. The fiber-induced phase noise is measured and cancelled with an all fiber-based interferometer using commercial off the shelf pigtailed telecommunication components. The compensated link shows an Allan deviation of a few 10-16 at one second and a few 10-19 at 10,000 seconds.
arXiv: Atomic Physics | 2012
John J. McFerran; Daniel Varela Magalhães; C. Mandache; J. Millo; W. Zhang; Y. Le Coq; G. Santarelli; S. Bize
We demonstrate the use of a fiber-based femtosecond laser locked onto an ultrastable optical cavity to generate a low-noise microwave reference signal. Comparison with both a cryogenic sapphire oscillator (CSO) and a titanium-sapphire-based optical frequency comb system exhibit a stability of about 3×10−15 between 1 and 10 s. The microwave signal from the fiber system is used to perform Ramsey spectroscopy in a state-of-the-art cesium fountain clock. The resulting clock is compared to the CSO and exhibits a stability of 3.5×10−14τ−1/2.
international frequency control symposium | 2009
J. Millo; Y. Le Coq; S. Bize; J. Guéna; H. Jiang; M. Abgrall; E. M. L. English; A. Clairon; G. Santarelli; Michael E. Tobar
In conclusion, we have used two FOFC based optical to microwave division frequency synthesizers referenced to a common optically source to create 11.55 GHz microwave signals with a relative frequency stability of 1.6×10-16 at 1 s. The relative phase noise spectral density at a 1 Hz offset from the 11.55 GHz carrier is measured at 111 dBrad2/Hz, limited by the readout system noise floor. Long term stability and accuracy down to 3×10-19 at 65536 s was also demonstrated from a set of 3 days continuous measurement. These results are obtained with classical double balanced mixers measurement scheme. By using a noise measurement system based on the carrier suppression method and advanced noise reduction techniques we are able to improve the results down to a phase noise spectral density at a 1 Hz of 117 dBrad2/Hz and a FFS is of 1.5×10-19 at 1000s (for a single system).
international frequency control symposium | 2008
M. Petersen; J. Millo; Daniel Varela Magalhães; C. Mandache; S. T. Dawkins; R. Chicireanu; Y. Lecoq; O. Acef; G. Santarelli; A. Clairon; S. Bize
Interferometric wavelength meters have attained frequency resolutions down to the megahertz range. In particular, Fizeau interferometers, which have no moving parts, are becoming a popular tool for laser characterization and stabilization. In this paper, we characterize such a wavelength meter using an ultrastable laser in terms of relative frequency instability σ(y)(τ) and demonstrate that it can achieve a short-term instability σ(y)(1s)≈2×10(-10) and a frequency drift of order 10 MHz/day. We use this apparatus to demonstrate frequency control of a near-infrared laser, where a frequency instability below 3×10(-10) from 1 to 2000 s is achieved. Such performance is, for example, adequate for ion trapping and atom cooling experiments.