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An innovative and practical scheme of building far-detuned optical lattice for 87Rb atoms is proposed.The disposals of aligning the lattice beams,tuning the lattice frequency and controlling the tapered amplifier for output are described in detail.Alignment of optical lattices is quite difficult in principle,for several beams are required to hit the same atomic cloud.For the relatively near-detuned one-and two-dimensional lattices,the coarse alignment is accomplished by tuning the lattice laser onto resonance with the magnetic-optic trap(MOT) frequency,and then blowing away the MOT in real time.A more precision alignment is implemented at the end of the MOT loading,the atoms are first pumped into the lower hyperfine level by turning off the repumping for some time;then,the pulsed lattice beams are turned on for a short time at some reasonably large detuning.Finally,a fluorescent image of the MOT is taken without repumping,in order to detect only those atoms which are repumped by the lattice laser.For the purpose of controlling the detuning of the lattice easily and accurately,a home-made grating wavemeter with a resolution better than 1 GHz is used.This way allows the laser to be locked at any frequency by using a software PID and is experimentally simple to implement.The intensity of the lattice is controlled directly by pulsing the current through the tapered amplifier using a function generator and a laser diode driver.This technique has already been demonstrated before by Prof.M.Kasevich's group at Stanford. Our experiment starts with a MOT capturing approximately 4107 atoms in 200 ms.The lattice loading is overlap with the end of polarization gradient cooling(PGC),after that,the molasses laser beams are extinguished, and the adiabatic expansion is accomplished in the same time by a decrease in the lattice light intensity according to release function.On the basis of MOT and PGC,the dependences of atomic loading on such parameters as the intensity and frequency detuning of optical lattice are investigated experimentally.The vibration frequency is measured by intentionally modulating the trap intensity.Experimental results show that the lattice structure facilitates the cooling with the temperature of atoms cloud being reduced to 1/3 compared with free space polarization gradient cooling.The system design,experimental results and conclusions are of definite significance and can serve as a fine reference for other kinds of lattices designs or alkali atomic plans.
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Keywords:
- cold atoms /
- optical lattice /
- polarization gradient cooling
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[5] Gustavson T L, Bouyer P, Kasevich M A 1997 Phys. Rev. Lett. 78 2046
[6] Adams C S 1994 Contemp. Phys. 35 1
[7] Monroe C 2002 Nature 416 238
[8] Duan L M, Lukin M D, Cirac J I, Zoller P 2001 Nature 414 413
[9] Anderson M H, Ensher J R, Matthews M R, Wieman C E, Cornell E A 1995 Science 269 198
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[14] Cooper C J, Hillenbrand G, Rink J, Townsend C G, Zetie K, Foot C J 1994 Europhys. Lett. 28 397
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[17] White J D, Scholten R E 2012 Rev. Sci. Instrum. 83 113104
[18] Takase K, Stockton J K, Kasevich M A 2007 Opt. Lett. 32 2617
[19] Kastberg A, Phillips W D, Rolston L, Spreeuw R J C 1995 Phys. Rev. Lett. 74 1542
[20] Kerman A J 2002 Ph. D. Dissertation (Stanford:Stanford university)
[21] Poulsen A S 2014 Ph. D. Dissertation（Houston:Rice Univeristy)
[22] Kerman A J, Vuletic V, Chin C, Chu S 2000 Phys. Rev. Lett. 84 439
[23] Winoto S L, DePue M T, Bramall N E, Weiss D S 1999 Phys. Rev. A 59 R19
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[1] Gibble K, Chu S 1993 Phys. Rev. Lett. 70 1771
[2] Santarelli G, Laurent P, Lemonde P, Clairon A, Mann A G, Chang S, Luiten A N, Salomon C 1999 Phys. Rev. Lett. 82 4619
[3] Hardman K S, Kuhn C C N, McDonald G D, Debs J E, Bennetts S, Close J D, Robins N P 2014 Phys. Rev. A 89 023626
[4] Peters A, Chung K Y, Chu S 1999 Nature 400 849
[5] Gustavson T L, Bouyer P, Kasevich M A 1997 Phys. Rev. Lett. 78 2046
[6] Adams C S 1994 Contemp. Phys. 35 1
[7] Monroe C 2002 Nature 416 238
[8] Duan L M, Lukin M D, Cirac J I, Zoller P 2001 Nature 414 413
[9] Anderson M H, Ensher J R, Matthews M R, Wieman C E, Cornell E A 1995 Science 269 198
[10] Davis K B, Mewes M O, Andrews M R, van Druten N J, Durfee D S, Kurn D M, Ketterle W 1995 Phys. Rev. Lett. 75 3969
[11] Lett P D, Watts R N, Westbrook C I, Phillips W D, Gould P L, Metcalf H J 1988 Phys. Rev. Lett. 61 169
[12] Ketterle W, Davis K B, Joffe M A, Martin A, Pritchard D E 1993 Phys. Rev. Lett. 70 2253
[13] Townsend C G, Edwards N H, Zetie K P, Cooper C J, Rink J, Foot C J 1996 Phys. Rev. A 53 1702
[14] Cooper C J, Hillenbrand G, Rink J, Townsend C G, Zetie K, Foot C J 1994 Europhys. Lett. 28 397
[15] Hillenbrand G, Burnett K, Foot C J 1995 Phys. Rev. A 52 4763
[16] Anderson M H, Ensher J R, Matthews M R, Wieman C E, Cornell E A 1995 Science 269 198
[17] White J D, Scholten R E 2012 Rev. Sci. Instrum. 83 113104
[18] Takase K, Stockton J K, Kasevich M A 2007 Opt. Lett. 32 2617
[19] Kastberg A, Phillips W D, Rolston L, Spreeuw R J C 1995 Phys. Rev. Lett. 74 1542
[20] Kerman A J 2002 Ph. D. Dissertation (Stanford:Stanford university)
[21] Poulsen A S 2014 Ph. D. Dissertation（Houston:Rice Univeristy)
[22] Kerman A J, Vuletic V, Chin C, Chu S 2000 Phys. Rev. Lett. 84 439
[23] Winoto S L, DePue M T, Bramall N E, Weiss D S 1999 Phys. Rev. A 59 R19
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