Stanford PNT hollberg Nov07 b - Stanford Center for Position ...

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Self-Referenced Optical Frequency Sythesizer I(f) 0 Microwave out Jones, et al. Science 288, 635 (2000) Ideas, existed many places, Telle & Keller …, Udem, Hänsch … f n = n f rep + f o f o f rep x2 f 2n = 2nf rep + f o Pump f o 532 nm convex Optical Freq. Ref f Ti:Sapphire Gain
The frequency of a mode is simply F N = N * f rep – f 0 Where N is and integer ~ 10 6 0 f r =1/ τ r.t. f 0 f rep ~ 1000 MHz 0 Frequency
Page 1 and 2: Sundial Atoms and Lasers for Precis
Page 3 and 4: Accuracy of clocks through history
Page 5 and 6: Current Microwave-Based Standards a
Page 7 and 8: Relative position, dimensional metr
Page 9 and 10: Feedback System Locks LO to atomic
Page 11 and 12: Laser source Ca Oven Optical Atomic
Page 13 and 14: Fractional Frequency Uncertainty 1.
Page 15 and 16: 1 P1 (6s6p) Atom number [a.u.] Ytte
Page 17 and 18: Feedback System Locks LO to atomic
Page 19: Count Optical Frequencies with Opti
Page 23 and 24: Hg + ~1 fs per tooth Mechanical Ana
Page 25 and 26: Optical reference f opt M3 I(f) PUM
Page 27 and 28: Source Lab Laser Source 563 nm line
Page 29 and 30: Next generation Grace laser ranging
Page 31 and 32: Chip Scale Atomic Devices CSAC (clo
Page 33 and 34: 4.2 mm 1.5 mm NIST Chip-Scale Atomi
Page 35 and 36: (A Very Rough) Oscillator Compariso
Page 37 and 38: ? GPS Positioning with < 4 τ 3 τ
Page 39 and 40: Magnetometry with Chip-Scale Device
Page 41 and 42: Heater Currents Laser Current Local
Page 43 and 44: Magnetocardiography with a CSAM •
Page 45 and 46: Nuclear Spin Gyroscopes • Much wo

Stanford PNT hollberg Nov07 b - Stanford Center for Position ...

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