Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

AIP conference proceedings

Two-photon resonant, stimulated processes in krypton and xenon

John C. Miller

Published Jan 1, 1989• 1 citation
Publisher

Abstract

Both on‐axis and conical emissions have been observed following two‐photon pumping of the 5p states of krypton and the 6p’, 7p, 8p, and 4f states of xenon. In the former case, coherent emissions from the 5p states to the 5s are observed and in the latter case, many p → s, d → p, and f → d cascade emissions are observed. By analogy to the well‐studied alkali and alkaline earth examples, the emissions are discussed in terms of amplified spontaneous emission (ASE), stimulated hyper‐Raman scattering, and parametric four‐wave mixing. The physical processes responsible for the conical emission and for intensity anomalies in the xenon p → s emissions are not understood at present. Interference effects due to coherent cancellation between competing excitation pathways may be occurring.

DOI
10.1063/1.38672

Related papers

Two-photon resonant, stimulated processes in krypton and xenon

Joel C. Miller

Both on-axis and conical emissions have been observed following two-photon pumping of the 5p states of krypton and the 6p', 7p, 8p, and 4f states of xenon. In the former case, coherent emissions from the 5p states to the 5s are observed, and in the latter case, many p..-->..s, d..-->..p, and f..-->..d cascade emissions are observed. By analogy to the well-studied alkali and alkaline earth examples, the emissions are discussed in terms of amplified spontaneous emission (ASE), stimulated hyper-Raman scattering, and parametric four-wave mixing. The physical processes responsible for the conical emission and for intensity anomalies in the xenon p..-->..s emissions are not understood at present. Interference effects due to coherent cancellation between competing excitation pathways may be occurring. 4 refs., 3 figs.

•Nov 1, 1988•0 citations

Two-photon resonant multiphoton ionization and stimulated emission in krypton and xenon

John C. Miller

Forward- and backward-directed, stimulated emissions have been observed following two-photon pumping of the 5p states of krypton and the 6p', 7p, 8p, and 4f states of xenon. Multiphoton ionization spectra are also obtained and compared with the photon-detected excitation spectra. In krypton coherent emissions from the 5p states to the 5s are observed, and for xenon many p\ensuremath{\rightarrow}s, d\ensuremath{\rightarrow}p, and f\ensuremath{\rightarrow}d cascade emissions are observed. By analogy to the well-studied alkali-metal and alkaline-earth examples, the emissions are assigned as amplified spontaneous emission. Several intensity anomalies in the xenon p\ensuremath{\rightarrow}s emissions are not understood at present. Interference effects due to coherent cancellation between competing excitation pathways may be occurring.

Physical Review A•Dec 1, 1989•70 citations

Conical emission in atomic xenon

M. Rankin, Jon P. Davis, Christopher Giranda +2 more

Excitation of xenon near the two-photon resonance between the ground state and the 6p(1/2,0) state produces forward conical emission at a wavelength close to the 828-nm 6p(1/2,0)—6s(3/ 2,1) excited-state transition. We describe experimental features of this process as excited by 600-ps pulses of 250-nm radiation from a frequency-doubled dye laser with intensity up to 1.3 × 108 W/ cm2 in xenon at pressures of 1-20 Torr. The conical emission occurs most prominently when the driving field is a few gigahertz above the frequency at which spontaneous emission from the excited 6p state peaks. The cone angle increases with xenon pressure in the 1-10-Torr range. The dependence appears consistent with the predictions based on noncollinearly phase-matched four-wave mixing. In this interpretation, the fourth wave would be near resonance with the 146.9-nm first resonance transition of xenon and detuned to the low-frequency side. The conical emission co-exists (and may compete with) an axial stimulated process which may be either two-photon driven amplified spontaneous emission or stimulated hyper-Raman scattering. The different tuning characteristics for the two processes make the extent of their competition unclear.

Annual Meeting Optical Society of America•Jan 1, 1987•0 citations

Emissions in potassium vapour under 4S[sub 1∕2]–7S[sub 1∕2] two-photon nsec excitation

Dionysios Pentaris, George Chatzikyriakos, A. Armyras +6 more

The two‐photon excitation of 4S1/2–7S1/2 transition of potassium atoms is studied. Several coherent emissions and processes are possible, such as parametric four‐wave (PFWM), parametric six‐wave (PSWM) mixing and competition with the stimulated hyper Raman (SHRS) and the amplified spontaneous emission (ASE). The radiations at the transitions 6P3/2,1/2−4S1/2, 6S1/2−4P3/2,1/2 and 5P3/2,1/2−4S1/2 are emitted only in the forward direction (indicating a parametric process), while the radiation at the transition 4P3/2,1/2−4S1/2 is emitted in the forward and in the backward direction, indicating an ASE process.

AIP conference proceedings•Jan 1, 2010•2 citations

Study of the emission in K under two-photon excitation

Thomas Efthimiopoulos, M. E. Movsesyan, M. Katharakis +2 more

It is shown that by proper use of the excitation spectra, the emission spectra of the transition and the far-field patterns it is possible to distinguish between competing processes involved in the two-photon excitation to the 6S state of potassium, namely: (a) resonant fluorescence emission associated with the cascading spontaneous emission (ASE) and (b) the four-wave mixing parametric process. The effect of the buffer gas on the intensities of the spectra of the radiations emitted is discussed. Conical emission and spatial instabilities of the excitation radiation and the emission were also observed for high excitation and high vapour pressure of potassium.

Journal of Physics B Atomic Molecular and Optical Physics•Nov 28, 1996•9 citations

Competing non-linear and cooperative light emissions

K. J. Boller, H.-J. Lau, J. Sparbier +1 more

Two‐photon excitation (λ1,λ2) of lithium vapor generates light emission by four processes involving the 3d,3s levels: 1. Two‐photon emission, 3d−2s, 2. superfluorescence, 3d−2p, 3. parametric mixing, and 4. two−photon scattering. Upon stepwise tuning λ2, emission spectra are recorded close to 610 and 812 nm, and thus the sum frequency ω1+ω2 is scanned across the 4f resonance. Light observed at 610 nm is superfluorescence. The light at 609.2 nm varies in wavelength upon a shift of λ1, but not of λ2: It is two‐photon emission. Two more emission peaks shift in step with λ2: Parametric emission by five‐wave mixing, and hyper‐Raman‐Stokes scattering of two photons. Interference of these emissions has been observed. The pulse fluctuations of parametric emission are caused by the pump light, while quantum fluctuations dominate the other processes.

AIP conference proceedings•Jan 1, 1988•0 citations
Both on‐axis and conical emissions have been observed following two‐photon pumping of the 5p states of krypton and the 6p’, 7p, 8p, and 4f states of xenon. In the former case, coherent emissions from the 5p states to the 5s are observed and in the latter case, many p → s, d → p, and f → d cascade emissions are observed. By analogy to the well‐studied alkali and alkaline earth examples, the emissions are discussed in terms of amplified spontaneous emission (ASE), stimulated hyper‐Raman scattering, and parametric four‐wave mixing. The physical processes responsible for the conical emission and for intensity anomalies in the xenon p → s emissions are not understood at present. Interference effects due to coherent cancellation between competing excitation pathways may be occurring.
Both on-axis and conical emissions have been observed following two-photon pumping of the 5p states of krypton and the 6p', 7p, 8p, and 4f states of xenon. In the former case, coherent emissions from the 5p states to the 5s are observed, and in the latter case, many p..-->..s, d..-->..p, and f..-->..d cascade emissions are observed. By analogy to the well-studied alkali and alkaline earth examples, the emissions are discussed in terms of amplified spontaneous emission (ASE), stimulated hyper-Raman scattering, and parametric four-wave mixing. The physical processes responsible for the conical emission and for intensity anomalies in the xenon p..-->..s emissions are not understood at present. Interference effects due to coherent cancellation between competing excitation pathways may be occurring. 4 refs., 3 figs.
Forward- and backward-directed, stimulated emissions have been observed following two-photon pumping of the 5p states of krypton and the 6p', 7p, 8p, and 4f states of xenon. Multiphoton ionization spectra are also obtained and compared with the photon-detected excitation spectra. In krypton coherent emissions from the 5p states to the 5s are observed, and for xenon many p\ensuremath{\rightarrow}s, d\ensuremath{\rightarrow}p, and f\ensuremath{\rightarrow}d cascade emissions are observed. By analogy to the well-studied alkali-metal and alkaline-earth examples, the emissions are assigned as amplified spontaneous emission. Several intensity anomalies in the xenon p\ensuremath{\rightarrow}s emissions are not understood at present. Interference effects due to coherent cancellation between competing excitation pathways may be occurring.
Excitation of xenon near the two-photon resonance between the ground state and the 6p(1/2,0) state produces forward conical emission at a wavelength close to the 828-nm 6p(1/2,0)—6s(3/ 2,1) excited-state transition. We describe experimental features of this process as excited by 600-ps pulses of 250-nm radiation from a frequency-doubled dye laser with intensity up to 1.3 × 108 W/ cm2 in xenon at pressures of 1-20 Torr. The conical emission occurs most prominently when the driving field is a few gigahertz above the frequency at which spontaneous emission from the excited 6p state peaks. The cone angle increases with xenon pressure in the 1-10-Torr range. The dependence appears consistent with the predictions based on noncollinearly phase-matched four-wave mixing. In this interpretation, the fourth wave would be near resonance with the 146.9-nm first resonance transition of xenon and detuned to the low-frequency side. The conical emission co-exists (and may compete with) an axial stimulated process which may be either two-photon driven amplified spontaneous emission or stimulated hyper-Raman scattering. The different tuning characteristics for the two processes make the extent of their competition unclear.
The two‐photon excitation of 4S1/2–7S1/2 transition of potassium atoms is studied. Several coherent emissions and processes are possible, such as parametric four‐wave (PFWM), parametric six‐wave (PSWM) mixing and competition with the stimulated hyper Raman (SHRS) and the amplified spontaneous emission (ASE). The radiations at the transitions 6P3/2,1/2−4S1/2, 6S1/2−4P3/2,1/2 and 5P3/2,1/2−4S1/2 are emitted only in the forward direction (indicating a parametric process), while the radiation at the transition 4P3/2,1/2−4S1/2 is emitted in the forward and in the backward direction, indicating an ASE process.
It is shown that by proper use of the excitation spectra, the emission spectra of the transition and the far-field patterns it is possible to distinguish between competing processes involved in the two-photon excitation to the 6S state of potassium, namely: (a) resonant fluorescence emission associated with the cascading spontaneous emission (ASE) and (b) the four-wave mixing parametric process. The effect of the buffer gas on the intensities of the spectra of the radiations emitted is discussed. Conical emission and spatial instabilities of the excitation radiation and the emission were also observed for high excitation and high vapour pressure of potassium.
Two‐photon excitation (λ1,λ2) of lithium vapor generates light emission by four processes involving the 3d,3s levels: 1. Two‐photon emission, 3d−2s, 2. superfluorescence, 3d−2p, 3. parametric mixing, and 4. two−photon scattering. Upon stepwise tuning λ2, emission spectra are recorded close to 610 and 812 nm, and thus the sum frequency ω1+ω2 is scanned across the 4f resonance. Light observed at 610 nm is superfluorescence. The light at 609.2 nm varies in wavelength upon a shift of λ1, but not of λ2: It is two‐photon emission. Two more emission peaks shift in step with λ2: Parametric emission by five‐wave mixing, and hyper‐Raman‐Stokes scattering of two photons. Interference of these emissions has been observed. The pulse fluctuations of parametric emission are caused by the pump light, while quantum fluctuations dominate the other processes.