2002
DOI: 10.1007/s00340-002-1041-2
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Laser frequency stabilization by Doppler-free magnetic dichroism

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Cited by 122 publications
(78 citation statements)
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“…1. External cavity diode laser is frequency locked to F g = 2 → F e = 1 * corresponding author; e-mail: krmpot@phy.bg.ac.yu transition in 87 Rb by Doppler-free dichroic atomic vapor laser lock (DDAVLL) method [13] in the vacuum Rb cell. The variable neutral density filter is used for the laser power adjustments.…”
Section: Methodsmentioning
confidence: 99%
“…1. External cavity diode laser is frequency locked to F g = 2 → F e = 1 * corresponding author; e-mail: krmpot@phy.bg.ac.yu transition in 87 Rb by Doppler-free dichroic atomic vapor laser lock (DDAVLL) method [13] in the vacuum Rb cell. The variable neutral density filter is used for the laser power adjustments.…”
Section: Methodsmentioning
confidence: 99%
“…Figure 2 shows a schematic diagram of the experimental apparatus. The experiments were performed with light from an 894 nm diode laser (Toptica DL100L, distributed feedback laser) whose frequency was actively locked to the F g = 4 → F e = 3 hyperfine transition of the cesium D 1 line using a Doppler-free dichroic atomic vapor laser lock (DAVLL) technique [11,12]. The laser beam was carried by a polarization maintaining fiber to the experiment proper and split by a polarizing beam splitter cube into two beams of approximately equal intensity.…”
Section: The Polarization Modulation Functionmentioning
confidence: 99%
“…The beams are generated by two semiconductor lasers (Toptica, model TA100). Both lasers are stabilized to the atomic transition by the Dopplerfree dichroism method [8]. One of the lasers produces the repumping light for both MOTs, tuned to the F g = 1 − F e = 2 transition.…”
Section: Laser Systemmentioning
confidence: 99%