Theoretical study of multielectron dissociative ionization of diatomic molecules and clusters in a strong laser field

1998 ◽  
Vol 58 (5) ◽  
pp. 3826-3835 ◽  
Author(s):  
Isidore Last ◽  
Joshua Jortner
2014 ◽  
Vol T162 ◽  
pp. 014012 ◽  
Author(s):  
S Odžak ◽  
A Čerkić ◽  
M Busuladžić ◽  
E Hasović ◽  
A Gazibegović-Busuladži ◽  
...  

Laser Physics ◽  
2012 ◽  
Vol 22 (12) ◽  
pp. 1827-1832 ◽  
Author(s):  
E. Hasović ◽  
D. B. Milošević ◽  
M. Busuladžić ◽  
A. Gazibegović-Busuladžić ◽  
W. Becker

Open Physics ◽  
2011 ◽  
Vol 9 (4) ◽  
Author(s):  
Yonghua Zhu ◽  
Peng Song ◽  
Huan Yang ◽  
Fengcai Ma

AbstractIn this work, the femtosecond time-resolved photoelectron spectra and the coupling between the A2Σ+ and B2Π states of the NO molecule in a strong laser field have been investigated by the time-dependent wave packet method. We demonstrate that the weak coupling between the A2Σ+ and B2Π states of NO plays a key role on the peak centered at 0.37 eV of the photoelectron spectra in the 2+1’ channel.


Photonics ◽  
2021 ◽  
Vol 8 (6) ◽  
pp. 192
Author(s):  
Theocharis Lamprou ◽  
Rodrigo Lopez-Martens ◽  
Stefan Haessler ◽  
Ioannis Liontos ◽  
Subhendu Kahaly ◽  
...  

Quantum-optical spectrometry is a recently developed shot-to-shot photon correlation-based method, namely using a quantum spectrometer (QS), that has been used to reveal the quantum optical nature of intense laser–matter interactions and connect the research domains of quantum optics (QO) and strong laser-field physics (SLFP). The method provides the probability of absorbing photons from a driving laser field towards the generation of a strong laser–field interaction product, such as high-order harmonics. In this case, the harmonic spectrum is reflected in the photon number distribution of the infrared (IR) driving field after its interaction with the high harmonic generation medium. The method was implemented in non-relativistic interactions using high harmonics produced by the interaction of strong laser pulses with atoms and semiconductors. Very recently, it was used for the generation of non-classical light states in intense laser–atom interaction, building the basis for studies of quantum electrodynamics in strong laser-field physics and the development of a new class of non-classical light sources for applications in quantum technology. Here, after a brief introduction of the QS method, we will discuss how the QS can be applied in relativistic laser–plasma interactions and become the driving factor for initiating investigations on relativistic quantum electrodynamics.


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