21

Japan Academy Prize to:

Hidetoshi Katori Professor, Graduate School of Engineering, The University of Chief Scientist, Quantum Metrology Labora- tory, RIKEN Research Director, ERATO Katori Innova- tive Space-Time Project, JST

for “Invention of the Optical Lattice Clock and its Development”

Outline of the work:

Precise time standard forms the base of science and fundamental metrology with a significant impact on applications. The standard of time is defined by the 13-th CGPM (1967) as follows: “The second is the duration of time equal to 9 192 631 770 times the period of radiation corresponding to the transition between the two hyperfine levels of the ground state of cesium 133”. The uncertainty of a cesium-atomic clock made in 1955 was of the order of 10-12. The international atomic time is currently kept by an ensemble of cesium clocks with an uncertainty of a few parts in 1015. Most precise measurements of physical quantities are therefore performed by converting them to time. The voltage is converted to time by using the Josephson effect and the length is converted to time by defining the speed of light, for example. Since the linewidth of atomic transition is more or less independent of the transition frequency, optical transitions allow 4-5 orders of magnitude improvement in fractional uncertainties compared to microwave transitions. The uncertainty in frequency Δf of an atomic clock is not only limited by the linewidth W, but also by the signal-to-noise ratio, which is approximately given by

W Δf = . signal-to-noise ratio

Any interaction between atoms is responsible for reduction of the life time of the quantum state. Thus an optical clock that used a laser-cooled single atomic ion confined in a Paul trap was the primary candidate for the best frequency standard. However, the poor signal given by an atomic transition with a long life time prevents reduction of uncertainties in the frequency. Invention of the optical lattice clock by Prof. Hidetoshi Katori realizes both reduction in linewidth and increase in signal-to-noise ratio. The scheme uses millions of neutral atoms trapped in an optical lattice, in which the light-shift is cancelled out by using a particular “magic” wavelength of the laser. According to the uncertainty principle, a long observation time is required for a narrow linewidth. A large number N of neutral atoms confined in the optical lattice significantly reduces the interrogation time of the atomic transition by 1/√ N so that the signal-to-noise ratio can be increased. Therefore ultrastable and highly precise frequency can be achieved. Prof. Katori experimentally demonstrated high accuracy of the optical lattice clock by using laser-cooled strontium atoms confined in the optical lattice at the magic wavelength. In 2011 he observed thatthe 22 uncertainty in frequency difference between optical lattice clocks of strontium-87 and strontium-88 was stable within 10-17. He also observed an expected gravitational shift of 2.6 Hz corresponding to the difference in altitude of 50 meters. The atomic transition frequency is susceptible to light-shift due to black-body radiation of the ambient temperature. In order to reduce the uncertainty due to black-body radiation he built a pair of cryogenically cooled clocks operating at a temperature of 95 K. The black-body radiation at 95 K is 1/100 of that at room temperature. Statistical agreement between the two cryogenic clocks was found to be 2×10-18 for a month. Higher order light-shifts are theoretically predicted to be smaller than 10-18 and their contribution has been experimentally investigated. The frequency shift corresponding to a vertical displacement of 1 cm on the surface of the earth is 1.1×10-18, which can be detected in a short time by the optical lattice clock. This allows realization of precise measurement of geoid, which will be a useful tool in earth science. Investigation of relativistically curved space-time by using optical lattice clocks may also be expected. Optical lattice clocks are now investigated in National Institute of Information and Communication Technology, National Institute of Advanced Industrial Science and Technology as well as in The and RIKEN by using strontium, ytterbium or mercury atoms. Comparisons between these clocks and international comparisons are being carried out. Then the optical lattice clock is regarded as the predominant candidate for the future redefinition of the unit of time.

List of publication

1. I. Ushijima, M. Takamoto, M. Das, T. Ohkubo, and H. Katori, “Cryogenic optical lattice clocks, ” Nature Photon. 9, 185 (2015). 2. T. Akatsuka, H. Ono, K. Hayashida, K. Araki, M. Takamoto, T. Takano, and H. Katori, “30-km long opti- cal fiber link at 1397 nm for frquency comparison between distant strontium optical lattice clocks, ” Jpn. J. Appl. Phys. 53, 032801 (2014). 3. S. Okaba, T. Takano, F. Benabid, T. Bradley, L. Vincetti, Z. Maizelis, V. Yampol’skii, F. Nori, and H. Katori, “Lamb-Dicke spectroscopy of atoms in a hollow-core photonic crystal fibre, ” Nature Com- mun. 15, 4096 (2014). 4. V. D. Ovsiannikov, V. G. Pal’chikov, A. V. Taichenachev, V. I. Yudin, and H. Katori, “Multipole, nonlin- ear, and anharmonic uncertainties of clocks of Sr atoms in an optical lattice,” Phys. Rev. A 88, 013405 (2013). 5. A. Yamaguchi, M. Fujieda, M. Kumagai, H. Hachisu, S. Nagano, Y. Li, T. Ido, T. Takano, M. Takamoto, and H. Katori, “Direct comparison of distant optical lattice clocks at the10-16 uncertainty,” Appl. Phys. Exp. 4, 082203 (2011). 6. M. Takamoto, T. Takano, and H. Katori, “Frequency comparison of optical lattice clocks beyond the Dick limit,” Nature Photon. 5, 288-292 (2011). 7. H. Katori, “Optical lattice clocks and quantum metrology,” Nature Photon. 5, 203-210 (2011). 8. A. Derevianko and H. Katori, “Colloquium: Physics of optical lattice clocks,” Rev. Mod. Phys. 83, 331 (2011). 9. H. Katori, T. Takano, and M. Takamoto, “Optical lattice clocks and frequency comparison,” J. Phy. Conf. Ser. 264, 012011 (2011). 10. F. L. Hong and H. Katori, “Frequency metrology with optical lattice clocks,” Jpn. J. Appl. Phys. 49, 080001 (2010). 23

11. T. Akatsuka, M. Takamoto, and H. Katori, “Three-dimensional optical lattice clock with bosonic 88Sr at- oms,” Phys. Rev. A 81, 023402 (2010). 12. H. Katori, K. Hashiguchi, E. Yu. Il’inova, V. D. Ovsiannikov, “Magic wavelength to make optical lattice clocks insensitive to atomic motion,” Phys. Rev. Lett. 103, 153004 (2009). 13. M. Takamoto, H. Katori, S. I. Marmo, V. D. Ovsiannikov, and V. G. Pal’chikov, “Prospects for optical clocks with a blue-detuned lattice,” Phys. Rev. Lett. 102, 063002 (2009). 14. F. L. Hong, M. Musha, M. Takamoto, H. Inaba, S. Yanagimachi, A. Takamizawa, K. Watabe, T. Ikegami, M. Imae, Y. Fujii, M. Amemiya, K. Nakagawa, K. Ueda, and H. Katori, “Measuring the frequency of a Sr op- tical lattice clock using a 120 km coherent optical transfer.” Opt. Lett. 34, 692-694 (2009). 15. M. Takamoto and H. Katori, “Coherence of spin-polarized fermions interacting with a clock laser in a Stark-shift-free optical lattice,” J. Phys. Soc. Jpn. 78, 013301 (2009). 16. T. Akatsuka, M. Takamoto, and H. Katori, “Optical lattice clocks with non-interacting bosons and fermi- ons,” Nature Phys. 4, 954-959 (2008). 17. J. Ye, H. J. Kimble, and H. Katori, “Quantum state engineering and precision metrology using state-insen- sitive light traps,” Science 320, 1734-1738 (2008). 18. S. Blatt, A. D. Ludlow, G. K. Campbell, J. W. Thomsen, T. Zelevinsky, M. M. Boyd, J. Ye, X. Baillard, M. Fouche, R. L. Targat, A. Brusch, P. Lemonde, M. Takamoto, F. L. Hong, H. Katori and V. V. Flambaum, “New limits on coupling of fundamental constants to gravity using 87Sr optical lattice clocks.” Phys. Rev. Lett. 100, 140801 (2008). 19. H. Hachisu, K. Miyagishi, S. G. Porsev, A. Derevianko, V. D. Ovsiannikov, V. G. Pal’chikov, M. Takamo- to, and H. Katori, “Trapping of neutral mercury atoms and prospects for optical lattice clocks,” Phys. Rev. Lett. 100, 053001 (2008). 20. V. D. Ovsiannikov, V. G. Pal’chikov, A. V. Taichenachev, V. I. Yudin, H. Katori and M. Takamoto, “Mag- 1 3 ic-wave-induced S0- P0 transition in even isotopes of alkaline-earth-metal-like atoms,” Phys. Rev. A 75, 020501R (2007). 21. M. Takamoto, F.-L. Hong, R. Higashi, Y. Fujii, M. Imae, and H. Katori, “Improved frequency measure- ment of a one-dimensional optical lattice clock with a spin-polarized fermionic 87Sr isotope,” J. Phys. Soc. Jpn. 75, 104302 (2006). 22. T. Kishimoto, H. Hachisu, J. Fujiki, K. Nagato, M. Yasuda, and H. Katori, “Electrodynamic trapping of spinless neutral atoms with an atom chip,” Phys. Rev. Lett. 96, 123001 (2006). 23. V.D. Ovsiannikov, V.G. Pal’chikov, H. Katori, and M. Takamoto, “Polarization and dispersion properties of light shifts in ultrastable optical frequency standards,” Quant. Electron. 36, 3-19 (2006). 24. M. Yasuda, T. Kishimoto, M. Takamoto, H. Katori, “Photoassociation spectroscopy of 88Sr: reconstruction of the wave function near the last node,” Phys. Rev. A 73, 011403R (2006). 25. F.-L. Hong, M. Takamoto, R. Higashi, Y. Fukuyama, J. Jiang, and H. Katori, “Frequency measurement of a Sr lattice clock using an SI-second-referenced optical frequency comb linked by a global positioning system (GPS),” Opt. Express 13, 5253 (2005). 26. M. Takamoto, F.-L. Hong, R. Higashi, and H. Katori, “An optical lattice clock,” Nature 435, 321-324 (2005). 3 27. M. Yasuda and H. Katori, “Lifetime measurement of the P2 metastable state of strontium Atoms,” Phys. Rev. Lett. 92, 153004 (2004). 28. H. Katori and T. Akatsuka, “Electric manipulation of spinless neutral atoms on a surface,” Jpn. J. Appl. Phys. 43, 358-361 (2004). 1 3 87 29. M. Takamoto and H. Katori, “Spectroscopy of the S0- P0 clock transition of Sr in an optical lattice,” Phys. Rev. Lett. 91, 223001 (2003). 24

30. H. Katori, M. Takamoto, V. G. Pal’chikov, and V. D. Ovsiannikov, “Ultrastable optical clock with neutral atoms in an engineered light shift trap,” Phys. Rev. Lett. 91, 173005 (2003). 31. T. Ido and H. Katori, “Recoil-free spectroscopy of neutral Sr atoms in the Lamb-Dicke regime,” Phys. Rev. Lett. 91, 053001 (2003). 32. T. Mukaiyama, H. Katori, T. Ido, Y. Li, and M. Kuwata-Gonokami, “Recoil-limited laser cooling of 87Sr atoms near the Fermi temperature,” Phys. Rev. Lett. 90, 113002 (2003). 33. H. Katori, “Spectroscopy of strontium atoms in the Lamb-Dicke confinement,” Proceedings of the 6th Symposium on Frequency Standards and Metrology, edited by P. Gill (World Scientific, Singapore, 2002) p.323-330. 34. H. Katori, T. Ido, Y. Isoya, and M. Kuwata-Gonokami, “Laser cooling of strontium atoms toward quan- tum degeneracy,” CP551, Atomic Physics 17, edited by E. Arimondo, P. DeNatele, and M. Inguscio, (American Institute of Physics, 2001) p.382-396. 35. T. Ido, Y. Isoya, and H. Katori, “Optical-dipole trapping of Sr atoms at a high phase-space density,” Phys. Rev. A. 61, 061403(R) (2000). 36. H. Katori, T. Ido, and M. Kuwata-Gonokami, “Optimal design of dipole potentials for efficient loading of Sr atoms,” J. Phys. Soc. Jpn. 68, 2479-2482 (1999). 37. H. Katori, T. Ido, Y. Isoya, and M. Kuwata-Gonokami, “Magneto-optical trapping and cooling of stron- tium atoms down to the photon recoil temperature,” Phys. Rev. Lett. 82, 1116-1119 (1999). 38. H. Katori, S. Schlipf, and H. Walther, “Anomalous dynamics of a single ion in an optical lattice,” Phys. Rev. Lett. 79, 2221-2224 (1997). 39. H. Katori, H. Kunugita and T. Ido, “Quantum statistical effect on ionizing collisions of ultracold metasta- ble kr isotopes,” Phys. Rev. A 52, R4324-R4327 (1995).

40. H. Katori and F. Shimizu, “Laser-induced ionizing collisions of ultracold krypton gas in the 1s5 metastable state,” Phys. Rev. Lett. 73, 2555-2558 (1994).

41. H. Katori and F. Shimizu, “Lifetime measurement of the 1s5 metastable state of argon and krypton with a magneto-optical trap,” Phys. Rev. Lett. 70, 3545-3548 (1993). 42. H. Katori and F. Shimizu, “Laser cooling and trapping of argon and krypton using diode lasers,” Jpn. J. Appl. Phys. 29, L2124-L2127 (1990).