C om piled Septem ber 7,2016 W e describe an optical bench in w hich w e lock the relative frequencies or phases of a set of three lasers in order to use them in a cold atom s interferom etry experim ent. A s a new feature, the sam e tw o lasers serve alternately to cool atom s and to realize the atom ic interferom eter. T his requires a fast change of the optical frequencies over a few G H z. T he num ber of required independent laser sources is then only 3, w hich enables the construction of the w hole laser system on a single transportable optical bench. R ecent results obtained w ith this opticalsetup are also presented. c 2016 O pticalSociety ofA m erica O C IS codes: 140. 3320,120.3180,140.3550,120.3930. W i thi n the l ast decades,atom i nterferom eters have devel oped i nto a hi ghl y com peti ti ve tool for preci si on m easurem ents. 1 A tom i c fountai ns used as atom i c cl ocks are the best real i zati on of the ti m e uni t. 2 A tom i nterferom etry al so prom i sessensorsto be hi ghl y sensi ti ve to i nerti alforces. 3{6 T he use of sti m ul ated R am an transiti ons to m ani pul ate the atom i c wave packet has proven to be an e ci entway to obtai n hi gh accuracy devi ces. 5,6 In thi s l etter,we descri be a robust,com pact and versati l e l aser system for atom i nterferom eters usi ng alkal iatom s.Such experi m ents basi cal l y need two di erentopti calfrequenci es,w hose di erence rem ai nscl oseto the hyper ne transi ti on frequency.W hen they are tuned cl ose to the D 2 transi ti ons, they are used to cool and repum p the atom s i n a m agneto-opti cal trap (M O T ). W hen far detuned,and phase l ocked,they are used to i nduce sti m ul ated R am an transi ti onsforthe i nterferometer. 7 Si nce l asers are not used si m ul taneousl y for trappi ng and R am an transi ti ons, we have i m pl em ented a techni que to use the sam e two l asers for both functi ons on ourgravi m eter. 8 Ital l owed usto bui l d the w hol el aser setup on a 60 90 cm 2 opti calbench.O url asersetup i sshow n i n gure 1.A rstl aserL1 i s l ocked on an atom i c transi ti on,usi ng FM -spectroscopy 9 on a saturated absorpti on si gnal .T hi s l aser consti tutes an opti calfrequency reference and i s used i n our experi m ent to detect or push the atom s.A second l aser L2 i s al ternatel y used asrepum per orasm asterR am an l aser. Part ofthe outputs ofL1 and L2 are superi m posed on a fast photodetector (PD 12 ) (H am am atsu G 4176) and the frequency ofthe beatnote i sservo l ocked by usi ng a frequency to vol tage converter.A thi rd l aser L3 i s used al ternatel y as cool i ng or as sl ave R am an l aser.T he frequency di erence between L2 and L3 i s m easured w i th a second opti cal beat note on PD 23 . Fi nal l y, both L2 and L3 beam s are superi m posed and di rected through an acousto-opti calm odul atorei therto a m agneto-opti cal trap or to an atom i c i nterferom eter.B oth frequency l ocks of L2 and L3 use the sam e schem e w hi ch i sshow n i n gure 2.T he opti calbeatnote i ssued from the photode...