Modulation of the shape of the photon echo pulse by a pulsed magnetic field: Zeeman splitting in LuLiF4:Er3+ and YLiF4:Er3+

Lisin, V. N.; Shegeda, A. M.

doi:10.1134/s0021364012170092

Cited by 10 publications

(8 citation statements)

References 3 publications

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“…We described the details of the experiment in [1,2]. For this reason, we present only the main moments and some differences.…”

Section: Experimental Conditionsmentioning

confidence: 99%

“…As a result, relative phase φ of these dipole groups is not equal to zero. Echo intensity oscillates versus the phase [1,2]:…”

Section: Introductionmentioning

confidence: 99%

“…If the relative phase φ is larger than 3π then the time form of an echo is modulated. There is enough of one waveform [2] to determine modulation period T and therefore Zeeman splitting:…”

Section: Introductionmentioning

confidence: 99%

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The application of the weak magnetic field pulse to measure g-factors of ground and excited optical states by a photon echo method

Lisin¹,

Shegeda²,

Самарцев³

2014

Laser Phys. Lett.

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A new scheme of the definition of g-factors as ground and excited optical states of a paramagnetic ion in zero external constant magnetic field has been proposed and experimentally realized in optical systems in which the Zeeman effect is manifested. A pulse of a weak magnetic field leads to the occurrence of relative phase shifts of the excited dipoles and, as a consequence, to modulation of a photon echo wave form if the magnetic pulse overlaps in time with the echo pulse. The modulation periods of the wave form depend on polarization of the laser light which excites the photon echo. The values of these periods for σ -and π-laser light polarization have been measured and then the g-factors of the ground 4 I 15/2 and excited 4 F 9/2 states of the Er 3+ ion in the LuLiF 4 and the YLiF 4 matrices have been determined. The g-factor values have been compared with the known literary data.

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“…We described the details of the experiment in [1,2]. For this reason, we present only the main moments and some differences.…”

Section: Experimental Conditionsmentioning

confidence: 99%

“…As a result, relative phase φ of these dipole groups is not equal to zero. Echo intensity oscillates versus the phase [1,2]:…”

Section: Introductionmentioning

confidence: 99%

See 1 more Smart Citation

The application of the weak magnetic field pulse to measure g-factors of ground and excited optical states by a photon echo method

Lisin¹,

Shegeda²,

Самарцев³

2014

Laser Phys. Lett.

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show abstract

“…If a pulse of the perturbation overlaps in time with echo-pulse then the echo waveform changes and photon echo beats must be. The photon echo beats have been observed firstly in systems in which the Zeeman splitting is realised [1,2,3]. In systems, in which the pseudo-Stark effect is manifested, the line splitting in electric field are due to the different Stark shifts at different lattice sites (as you cay see from figure 1).…”

Section: Introductionmentioning

confidence: 99%

The application of weak electric field pulses to measure the pseudo-Stark split by photon echo beating

2016

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Abstract. New scheme for determining the pseudo-Stark splitting of optical lines has been proposed and experimentally realized. A pulse of a weak electric field leads to occurrence of relative phase shifts of the excited dipoles and, as consequence, to beating of a photon echo wave form if electric pulse overlaps in time with echo-pulse. The value of the pseudo-stark splitting is the inverse period of the beats. The photon echo beating of the R1-line in Ruby have been observed. The pseudo-Stark splitting has been determined and it's value have been compared with the known literary data.

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“…If a pulse of the perturbation overlaps in time with the echo-pulse, then the echo waveform changes and photon echo beats arise. The PEB have been observed initially in systems in which Zeeman splitting is realized [1][2][3]. In systems in which the pseudo-Stark effect is manifest, the line splitting in electric field is due to the different Stark shifts at different lattice sites, for example A and B sites.…”

Section: Introductionmentioning

confidence: 99%

Stark shift in Y₂SiO₅:Er³⁺ by the photon echo beating method

Lisin¹,

Shegeda²,

Самарцев³

et al. 2018

Laser Phys.

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The coefficient of a linear Stark shift of the 4 F 9/2 -4 I 15/2 transition of Er 3+ ion in Y 2 SiO 5 is measured (14.3 kHzV −1 cm ) by splitting the upper and lower levels of the transition by a pulsed electric field and measuring the splitting frequency from the period of beatings of the temporal form of a photon echo signal (stark photon echo beating method). The linear Stark coefficients of Er 3+ transitions in Y 2 SiO 5 have not been measured before, and this is a valuable result for a number of applications such as gradient echo memory, group velocity control via spectral hole burning, etc.

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Modulation of the shape of the photon echo pulse by a pulsed magnetic field: Zeeman splitting in LuLiF4:Er3+ and YLiF4:Er3+

Cited by 10 publications

References 3 publications

The application of the weak magnetic field pulse to measure g-factors of ground and excited optical states by a photon echo method

The application of the weak magnetic field pulse to measure g-factors of ground and excited optical states by a photon echo method

The application of weak electric field pulses to measure the pseudo-Stark split by photon echo beating

Stark shift in Y₂SiO₅:Er³⁺ by the photon echo beating method

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Modulation of the shape of the photon echo pulse by a pulsed magnetic field: Zeeman splitting in LuLiF4:Er3+ and YLiF4:Er3+

Cited by 10 publications

References 3 publications

The application of the weak magnetic field pulse to measure g-factors of ground and excited optical states by a photon echo method

The application of the weak magnetic field pulse to measure g-factors of ground and excited optical states by a photon echo method

The application of weak electric field pulses to measure the pseudo-Stark split by photon echo beating

Stark shift in Y2SiO5:Er3+ by the photon echo beating method

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Stark shift in Y₂SiO₅:Er³⁺ by the photon echo beating method