1999
DOI: 10.1016/s0030-3992(99)00099-7
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A simple extended cavity diode laser for spectroscopy around 640 nm

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Cited by 11 publications
(13 citation statements)
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“…In this paper we extend our previous analysis by presenting a novel identification and calibration procedure for estimating the full set of Lamb parameters, i.e. α 1,2 , r 1,2 , ε 1,2 , self-and cross-saturation coefficients β 1,2 and θ 12,21 , and scale factor and null shift errors σ 1,2 and τ 12,21 , which depend in their turn on cavity losses µ 1,2 , plasma polarizability and single pass gain G of the laser medium.…”
Section: Introductionmentioning
confidence: 75%
“…In this paper we extend our previous analysis by presenting a novel identification and calibration procedure for estimating the full set of Lamb parameters, i.e. α 1,2 , r 1,2 , ε 1,2 , self-and cross-saturation coefficients β 1,2 and θ 12,21 , and scale factor and null shift errors σ 1,2 and τ 12,21 , which depend in their turn on cavity losses µ 1,2 , plasma polarizability and single pass gain G of the laser medium.…”
Section: Introductionmentioning
confidence: 75%
“…Then the sensitivity of diode lasers to external perturbations was utilized as a standard method for improving their poor spectral properties. To attain tunable output and a narrow optical bandwidth, various techniques have been implemented like injection locking, negative electronic feedback, resonant optical feedback from high-finesse cavities and optical feedback from an extended cavity [7]. Lasers with single optical frequency and narrow linewidth are being used in a wide range of highly significant applications like laser cooling, atomic physics researches and high precision measurements [8].…”
Section: Diode Lasers: An Overviewmentioning
confidence: 99%
“…4 shows an experimental setup of relative frequency locking (using two ECDLs) to the atomic groundstate hyperfine splitting by using an electromagnetically induced transparency (EIT) resonance in rubidium which was considered an economical and convenient method suitable for many two-frequency experiments such as lasing without inversion, slow light, coherent population trapping and Raman sideband cooling [16]. Some other examples include the resolution of hyperfine structure of the close P63 R70 (8, 4) transitions of iodine [13] with a 690 nm frequency stabilized diode laser setup [17], the oscillation frequency locking of each operating mode of a diode laser coupled to an external cavity to a hyperfine transition or a crossover resonance of the saturated absorption spectrum of cesium D 2 line [18], study of saturated absorption of several neon transitions in a radio-frequency discharge with 640 nm ECDL system [7], observation of Lamb dips in atomic indium spectrum at 410 nm with commercially available GaN-based laser diodes [19], etc.…”
Section: Hyperfine Transitions and Cooling Of Atomsmentioning
confidence: 99%
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“…With the progress in diode laser technology, inexpensive tunable single mode diode lasers with external cavity which are also called as external cavity diode lasers (ECDLs) [54][55][56][57][58] have recently been applied for the measurements of velocity distributions of In [59], He [60], Ar discharge is also shown in Fig. 21 for comparison.…”
Section: Measurement Of Gas Temperature Using An Extra Cavity Diode Lmentioning
confidence: 99%